{"id":46,"date":"2013-11-08T11:00:54","date_gmt":"2013-11-08T09:00:54","guid":{"rendered":"http:\/\/mat.uab.cat\/~jvm\/?page_id=46"},"modified":"2023-09-26T14:47:29","modified_gmt":"2023-09-26T12:47:29","slug":"papers","status":"publish","type":"page","link":"https:\/\/mat.uab.cat\/web\/jvm\/papers\/","title":{"rendered":"RESEARCH PAPERS"},"content":{"rendered":"<div class=\"teachpress_pub_list\"><form name=\"tppublistform\" method=\"get\"><a name=\"tppubs\" id=\"tppubs\"><\/a><\/form><div class=\"teachpress_publication_list\"><h3 class=\"tp_h3\" id=\"tp_h3_2023\">2023<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">J. Cuf\u00ed, J.J. Donaire, P. Mattila, J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('51','tp_links')\" style=\"cursor:pointer;\">Existence of Principal Values of some singular Integrals on Cantor sets, and Hausdorff dimension<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Pacific Journal Of Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 326, <\/span><span class=\"tp_pub_additional_number\">no. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 285-300, <\/span><span class=\"tp_pub_additional_year\">2023<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_51\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('51','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_51\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('51','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_51\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('51','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_51\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Existence of Principal Values of some singular Integrals on Cantor sets, and Hausdorff dimension},<br \/>\r\nauthor = {J. Cuf\\'{i}, J.J. Donaire, P. Mattila, J. Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Pacific_3262_2023_285_300.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.2140\/pjm.2023.326.285},<br \/>\r\nyear  = {2023},<br \/>\r\ndate = {2023-12-31},<br \/>\r\nurldate = {2023-12-01},<br \/>\r\njournal = {Pacific Journal Of Mathematics},<br \/>\r\nvolume = {326},<br \/>\r\nnumber = {2},<br \/>\r\npages = {285-300},<br \/>\r\nabstract = {Consider a standard Cantor set in the plane of Hausdorff dimension 1. If<br \/>\r\nthe linear density of the associated measure \u03bc vanishes, then the set of<br \/>\r\npoints where the principal value of the Cauchy singular integral of \u03bc exists<br \/>\r\nhas Hausdorff dimension 1. The result is extended to Cantor sets in Rd of<br \/>\r\nHausdorff dimension \u03b1 and Riesz singular integrals of homogeneity \u2212\u03b1,<br \/>\r\n0 \\&lt; \u03b1 \\&lt; d: the set of points where the principal value of the Riesz singular<br \/>\r\nintegral of \u03bc exists has Hausdorff dimension \u03b1. A martingale associated with<br \/>\r\nthe singular integral is introduced to support the proof.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('51','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_51\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Consider a standard Cantor set in the plane of Hausdorff dimension 1. If<br \/>\r\nthe linear density of the associated measure \u03bc vanishes, then the set of<br \/>\r\npoints where the principal value of the Cauchy singular integral of \u03bc exists<br \/>\r\nhas Hausdorff dimension 1. The result is extended to Cantor sets in Rd of<br \/>\r\nHausdorff dimension \u03b1 and Riesz singular integrals of homogeneity \u2212\u03b1,<br \/>\r\n0 &lt; \u03b1 &lt; d: the set of points where the principal value of the Riesz singular<br \/>\r\nintegral of \u03bc exists has Hausdorff dimension \u03b1. A martingale associated with<br \/>\r\nthe singular integral is introduced to support the proof.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('51','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_51\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Pacific_3262_2023_285_300.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Pacific_3262_2023[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Pacific_3262_2023[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.2140\/pjm.2023.326.285\" title=\"Follow DOI:https:\/\/doi.org\/10.2140\/pjm.2023.326.285\" target=\"_blank\">doi:https:\/\/doi.org\/10.2140\/pjm.2023.326.285<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('51','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">J. Mateu, M.G. Mora, L. Rondi, L. Scardia, J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('54','tp_links')\" style=\"cursor:pointer;\">Explicit minimisers for anisotropic Coulomb energies in 3D<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Advances in Mathematics 434(2023) 109333, <\/span><span class=\"tp_pub_additional_volume\">vol. 434, <\/span><span class=\"tp_pub_additional_number\">no. december 2023, <\/span><span class=\"tp_pub_additional_year\">2023<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_54\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('54','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_54\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('54','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_54\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('54','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_54\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Explicit minimisers for anisotropic Coulomb energies in 3D},<br \/>\r\nauthor = {J. Mateu, M.G. Mora, L. Rondi, L. Scardia, J. Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV-review_nored.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1016\/j.aim.2023.109333 },<br \/>\r\nyear  = {2023},<br \/>\r\ndate = {2023-12-30},<br \/>\r\nurldate = {2023-12-31},<br \/>\r\njournal = {Advances in Mathematics 434(2023) 109333},<br \/>\r\nvolume = {434},<br \/>\r\nnumber = {december 2023},<br \/>\r\nabstract = {In this paper we consider a general class of anisotropic energies in three dimensions and give a complete characterisation of their minimisers. We show that, depending on the Fourier transform of the interaction potential, the minimiser is either the normalised characteristic function of an ellipsoid or a measure supported on a two- dimensional ellipse. In particular, it is always an ellipsoid if the transform is strictly positive, while when the Fourier transform is degenerate both cases can occur. Finally, we show an explicit example where loss of dimensionality of the minimiser does occur.<br \/>\r\n},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('54','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_54\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we consider a general class of anisotropic energies in three dimensions and give a complete characterisation of their minimisers. We show that, depending on the Fourier transform of the interaction potential, the minimiser is either the normalised characteristic function of an ellipsoid or a measure supported on a two- dimensional ellipse. In particular, it is always an ellipsoid if the transform is strictly positive, while when the Fourier transform is degenerate both cases can occur. Finally, we show an explicit example where loss of dimensionality of the minimiser does occur.<br \/>\r\n<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('54','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_54\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV-review_nored.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV-review_nore[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV-review_nore[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1016\/j.aim.2023.109333 \" title=\"Follow DOI:https:\/\/doi.org\/10.1016\/j.aim.2023.109333 \" target=\"_blank\">doi:https:\/\/doi.org\/10.1016\/j.aim.2023.109333 <\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('54','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('49','tp_links')\" style=\"cursor:pointer;\">The global regularity of vortex patches revisited<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Advances in Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 416, <\/span><span class=\"tp_pub_additional_year\">2023<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_49\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('49','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_49\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('49','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_49\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('49','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_49\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The global regularity of vortex patches revisited},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Revisited_Global_Regularity.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1016\/j.aim.2023.108917},<br \/>\r\nyear  = {2023},<br \/>\r\ndate = {2023-02-01},<br \/>\r\nurldate = {2023-01-01},<br \/>\r\njournal = {Advances in Mathematics},<br \/>\r\nvolume = {416},<br \/>\r\nabstract = {We prove persistence of the regularity of the boundary of vortex patches for a large class of transport equations in the plane. The velocity field is given by convolution of the vorticity with an odd kernel, homogeneous of degree \u22121 and of class C^2 off the origin. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('49','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_49\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We prove persistence of the regularity of the boundary of vortex patches for a large class of transport equations in the plane. The velocity field is given by convolution of the vorticity with an odd kernel, homogeneous of degree \u22121 and of class C^2 off the origin. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('49','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_49\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Revisited_Global_Regularity.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Revisited_Global_[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Revisited_Global_[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1016\/j.aim.2023.108917\" title=\"Follow DOI:https:\/\/doi.org\/10.1016\/j.aim.2023.108917\" target=\"_blank\">doi:https:\/\/doi.org\/10.1016\/j.aim.2023.108917<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('49','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Juan Carlos Cantero, Joan Orobitg, Joan Mateu; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('48','tp_links')\" style=\"cursor:pointer;\">Regularity of the boundary of vortex patches for some non-linear transport equations <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Analysis and PDE, <\/span><span class=\"tp_pub_additional_volume\">vol. 16, <\/span><span class=\"tp_pub_additional_number\">no. 7, <\/span><span class=\"tp_pub_additional_pages\">pp. 1621-1650, <\/span><span class=\"tp_pub_additional_year\">2023<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_48\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('48','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_48\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('48','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_48\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('48','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_48\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Regularity of the boundary of vortex patches for some non-linear transport equations },<br \/>\r\nauthor = {Juan Carlos Cantero, Joan Orobitg, Joan Mateu and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_Transport_Homog_Kernel.pdf},<br \/>\r\ndoi = {DOI:10.2140\/apde.2023.16.1621},<br \/>\r\nyear  = {2023},<br \/>\r\ndate = {2023-01-01},<br \/>\r\nurldate = {2022-05-01},<br \/>\r\njournal = {Analysis and PDE},<br \/>\r\nvolume = {16},<br \/>\r\nnumber = {7},<br \/>\r\npages = {1621-1650},<br \/>\r\nabstract = {We prove the persistence of boundary smoothness of vortex patches for non- linear transport equations with velocity fields given by convolution of the density with an odd kernel, homogeneous of order -(n-1) and C^2 smooth off the origin. This allows the velocity field to have non-trivial divergence. The quasi-geostrophic equation in R^3 and the Cauchy kernel in the plane are examples. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('48','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_48\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We prove the persistence of boundary smoothness of vortex patches for non- linear transport equations with velocity fields given by convolution of the density with an odd kernel, homogeneous of order -(n-1) and C^2 smooth off the origin. This allows the velocity field to have non-trivial divergence. The quasi-geostrophic equation in R^3 and the Cauchy kernel in the plane are examples. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('48','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_48\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_Transport_Homog_Kernel.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_Transpor[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_Transpor[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/DOI:10.2140\/apde.2023.16.1621\" title=\"Follow DOI:DOI:10.2140\/apde.2023.16.1621\" target=\"_blank\">doi:DOI:10.2140\/apde.2023.16.1621<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('48','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2021\">2021<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">J. Mateu, M. G. Mora, L. Rondi, L. Scardia; J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('15','tp_links')\" style=\"cursor:pointer;\">Stability of ellipsoids as the energy minimizers of perturbed Coulomb energies<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">SIAM Journal of Mathematical Analysis, <\/span><span class=\"tp_pub_additional_volume\">vol. 55, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 3650-3676, <\/span><span class=\"tp_pub_additional_year\">2021<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_15\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('15','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_15\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('15','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_15\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('15','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_15\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{,<br \/>\r\ntitle = {Stability of ellipsoids as the energy minimizers of perturbed Coulomb energies},<br \/>\r\nauthor = {J. Mateu, M. G. Mora, L. Rondi, L. Scardia and J. Verdera},<br \/>\r\neditor = {Society for Industrial and Applied Mathematics},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/MMRSV_2021-perturbation.pdf},<br \/>\r\ndoi = {10.1137\/22M1479695},<br \/>\r\nyear  = {2021},<br \/>\r\ndate = {2021-01-01},<br \/>\r\nurldate = {2021-01-01},<br \/>\r\njournal = {SIAM Journal of Mathematical Analysis},<br \/>\r\nvolume = {55},<br \/>\r\nnumber = {4},<br \/>\r\npages = {3650-3676},<br \/>\r\nabstract = {In this paper we characterize the minimizer for a class of nonlocal perturbations<br \/>\r\nof the Coulomb energy. We show that the minimizer is the normalized characteristic function of<br \/>\r\nan ellipsoid, under the assumption that the perturbation kernel has the same homogeneity as the<br \/>\r\nCoulomb potential, is even, is smooth off the origin, and is sufficiently small. This result can be seen<br \/>\r\nas the stability of ellipsoids as energy minimizers, since the minimizer of the Coulomb energy is the<br \/>\r\nnormalized characteristic function of a ball.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('15','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_15\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we characterize the minimizer for a class of nonlocal perturbations<br \/>\r\nof the Coulomb energy. We show that the minimizer is the normalized characteristic function of<br \/>\r\nan ellipsoid, under the assumption that the perturbation kernel has the same homogeneity as the<br \/>\r\nCoulomb potential, is even, is smooth off the origin, and is sufficiently small. This result can be seen<br \/>\r\nas the stability of ellipsoids as energy minimizers, since the minimizer of the Coulomb energy is the<br \/>\r\nnormalized characteristic function of a ball.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('15','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_15\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/MMRSV_2021-perturbation.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/MMRSV_2021-pertur[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/MMRSV_2021-pertur[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/10.1137\/22M1479695\" title=\"Follow DOI:10.1137\/22M1479695\" target=\"_blank\">doi:10.1137\/22M1479695<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('15','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('46','tp_links')\" style=\"cursor:pointer;\">The equilibrium measure for an anisotropic non local energy<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Calculus of Variations and Partial Differential Equations, <\/span><span class=\"tp_pub_additional_volume\">vol. 60, <\/span><span class=\"tp_pub_additional_pages\">pp. 109, <\/span><span class=\"tp_pub_additional_year\">2021<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_46\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('46','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_46\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('46','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_46\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('46','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_46\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The equilibrium measure for an anisotropic non local energy},<br \/>\r\nauthor = {Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/TheEquilibriumMeasureForAnAnis_Calculus_2021.pdf},<br \/>\r\nyear  = {2021},<br \/>\r\ndate = {2021-01-01},<br \/>\r\nurldate = {2021-01-01},<br \/>\r\njournal = {Calculus of Variations and Partial Differential Equations},<br \/>\r\nvolume = {60},<br \/>\r\npages = {109},<br \/>\r\nabstract = {In this paper we characterise the minimisers of a one-parameter family of nonlocal and anisotropic energies I\u03b1 defined on probability measures in Rn, with n\u22653. The energy I\u03b1 consists of a purely nonlocal term of convolution type, whose interaction kernel reduces to the Coulomb potential for \u03b1=0 and is anisotropic otherwise, and a quadratic confinement. The two-dimensional case arises in the study of defects in metals and has been solved by the authors by means of complex-analysis techniques. We prove that for \u03b1\u2208(\u22121,n\u22122], the minimiser of I\u03b1 is unique and is the (normalised) characteristic function of a spheroid. This result is a paradigmatic example of the role of the anisotropy of the kernel on the shape of minimisers. In particular, the phenomenon of loss of dimensionality, observed in dimension n=2, does not occur in higher dimension at the value \u03b1=n\u22122 corresponding to the sign change of the Fourier transform of the interaction potential. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('46','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_46\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we characterise the minimisers of a one-parameter family of nonlocal and anisotropic energies I\u03b1 defined on probability measures in Rn, with n\u22653. The energy I\u03b1 consists of a purely nonlocal term of convolution type, whose interaction kernel reduces to the Coulomb potential for \u03b1=0 and is anisotropic otherwise, and a quadratic confinement. The two-dimensional case arises in the study of defects in metals and has been solved by the authors by means of complex-analysis techniques. We prove that for \u03b1\u2208(\u22121,n\u22122], the minimiser of I\u03b1 is unique and is the (normalised) characteristic function of a spheroid. This result is a paradigmatic example of the role of the anisotropy of the kernel on the shape of minimisers. In particular, the phenomenon of loss of dimensionality, observed in dimension n=2, does not occur in higher dimension at the value \u03b1=n\u22122 corresponding to the sign change of the Fourier transform of the interaction potential. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('46','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_46\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/TheEquilibriumMeasureForAnAnis_Calculus_2021.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/TheEquilibriumMea[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/TheEquilibriumMea[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('46','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('47','tp_links')\" style=\"cursor:pointer;\">Explicit minimizers of nonlocal anisotropic energies: a short proof <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Izvestiya: Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 85, <\/span><span class=\"tp_pub_additional_number\">no. 3, <\/span><span class=\"tp_pub_additional_year\">2021<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_47\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('47','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_47\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('47','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_47\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('47','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_47\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Explicit minimizers of nonlocal anisotropic energies: a short proof },<br \/>\r\nauthor = {Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Shortest_Proof_Minimizers.pdf},<br \/>\r\nyear  = {2021},<br \/>\r\ndate = {2021-01-01},<br \/>\r\nurldate = {2021-01-01},<br \/>\r\njournal = {Izvestiya: Mathematics},<br \/>\r\nvolume = {85},<br \/>\r\nnumber = {3},<br \/>\r\nabstract = {n this paper we consider nonlocal energies defined on probability measures in the plane, given by a convolution interaction term plus a quadratic confinement. The interaction kernel is \u2212log\u2223\u2223z\u2223\u2223+alpha,x2\/\u2223\u2223z\u2223\u22232,z=x+iy, with \u22121\\&lt;alpha\\&lt;1. This kernel is anisotropic except for the Coulombic case alpha=0. We present a short compact proof of the known surprising fact that the unique minimiser of the energy is the normalised characteristic function of the domain enclosed by an ellipse with horizontal semi-axis sqrt1\u2212alpha and vertical semi-axis sqrt1+alpha. Letting alphato1\u2212 we find that the semicircle law on the vertical axis is the unique minimiser of the corresponding energy, a result related to interacting dislocations, and previously obtained by some of the authors. We devote the first sections of this paper to presenting some well-known background material in the simplest way possible, so that readers unfamiliar with the subject find the proofs accessible. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('47','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_47\" style=\"display:none;\"><div class=\"tp_abstract_entry\">n this paper we consider nonlocal energies defined on probability measures in the plane, given by a convolution interaction term plus a quadratic confinement. The interaction kernel is \u2212log\u2223\u2223z\u2223\u2223+alpha,x2\/\u2223\u2223z\u2223\u22232,z=x+iy, with \u22121&lt;alpha&lt;1. This kernel is anisotropic except for the Coulombic case alpha=0. We present a short compact proof of the known surprising fact that the unique minimiser of the energy is the normalised characteristic function of the domain enclosed by an ellipse with horizontal semi-axis sqrt1\u2212alpha and vertical semi-axis sqrt1+alpha. Letting alphato1\u2212 we find that the semicircle law on the vertical axis is the unique minimiser of the corresponding energy, a result related to interacting dislocations, and previously obtained by some of the authors. We devote the first sections of this paper to presenting some well-known background material in the simplest way possible, so that readers unfamiliar with the subject find the proofs accessible. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('47','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_47\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Shortest_Proof_Minimizers.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Shortest_Proof_Mi[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Shortest_Proof_Mi[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('47','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2020\">2020<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('12','tp_links')\" style=\"cursor:pointer;\">Birth and life of the L2 boundedness of the Cauchy Integral on Lipschitz graphs<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_year\">2020<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_12\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('12','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_12\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('12','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_12\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('12','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_12\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Birth and life of the L2 boundedness of the Cauchy Integral on Lipschitz graphs},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Birth_Life-1.pdf},<br \/>\r\nyear  = {2020},<br \/>\r\ndate = {2020-09-01},<br \/>\r\nurldate = {2020-09-01},<br \/>\r\nabstract = {We review various motives for considering the problem of estimating the Cauchy<br \/>\r\nSingular Integral on Lipschitz graphs in the L2 norm. We follow the thread that<br \/>\r\nled to the solution and then describe a few of the innumerable applications and<br \/>\r\nrami\u2000cations of this fundamental result. We concentrate on its influence in complex<br \/>\r\nanalysis, geometric measure theory and harmonic measure.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('12','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_12\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We review various motives for considering the problem of estimating the Cauchy<br \/>\r\nSingular Integral on Lipschitz graphs in the L2 norm. We follow the thread that<br \/>\r\nled to the solution and then describe a few of the innumerable applications and<br \/>\r\nrami\u2000cations of this fundamental result. We concentrate on its influence in complex<br \/>\r\nanalysis, geometric measure theory and harmonic measure.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('12','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_12\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Birth_Life-1.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Birth_Life-1.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Birth_Life-1.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('12','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">J. A. Carrillo, J. Mateu, M. G. Mora, L. Rondi, L. Scardia; J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('14','tp_links')\" style=\"cursor:pointer;\">The Ellipse Law: Kirchhoff Meets Dislocations<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Commun. Math. Physics, <\/span><span class=\"tp_pub_additional_volume\">vol. 373, <\/span><span class=\"tp_pub_additional_pages\">pp. 507-524, <\/span><span class=\"tp_pub_additional_year\">2020<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_14\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('14','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_14\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('14','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_14\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('14','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_14\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{,<br \/>\r\ntitle = {The Ellipse Law: Kirchhoff Meets Dislocations},<br \/>\r\nauthor = {J. A. Carrillo, J. Mateu, M. G. Mora, L. Rondi, L. Scardia and J. Verdera},<br \/>\r\neditor = {Springer},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/The-ellipse-law.Comm_.Math_.Physics-2.pdf},<br \/>\r\ndoi = {Digital Object Identifier (DOI) https:\/\/doi.org\/10.1007\/s00220-019-03368-w},<br \/>\r\nyear  = {2020},<br \/>\r\ndate = {2020-01-01},<br \/>\r\nurldate = {2020-01-01},<br \/>\r\njournal = {Commun. Math. Physics},<br \/>\r\nvolume = {373},<br \/>\r\npages = {507-524},<br \/>\r\nabstract = {In this paper we consider a nonlocal energy I_\u03b1 whose kernel is obtained by<br \/>\r\nadding to the Coulomb potential an anisotropic term weighted by a parameter \u03b1 \u2208 R.<br \/>\r\nThe case \u03b1 = 0 corresponds to purely logarithmic interactions, minimised by the circle<br \/>\r\nlaw; \u03b1 = 1 corresponds to the energy of interacting dislocations, minimised by the semicircle law. We show that for \u03b1 \u2208 (0, 1) the minimiser is the normalised characteristic<br \/>\r\nfunction of the domain enclosed by the ellipse of semi-axes sqrt{1 \u2212 \u03b1} and sqrt{1 + \u03b1}. This<br \/>\r\nresult is one of the very few examples where the minimiser of a nonlocal anisotropic<br \/>\r\nenergy is explicitly computed. For the proof we borrow techniques from fluid dynamics,<br \/>\r\nin particular those related to Kirchhoff\u2019s celebrated result that domains enclosed by<br \/>\r\nellipses are rotating vortex patches, called Kirchhoff ellipses.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('14','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_14\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we consider a nonlocal energy I_\u03b1 whose kernel is obtained by<br \/>\r\nadding to the Coulomb potential an anisotropic term weighted by a parameter \u03b1 \u2208 R.<br \/>\r\nThe case \u03b1 = 0 corresponds to purely logarithmic interactions, minimised by the circle<br \/>\r\nlaw; \u03b1 = 1 corresponds to the energy of interacting dislocations, minimised by the semicircle law. We show that for \u03b1 \u2208 (0, 1) the minimiser is the normalised characteristic<br \/>\r\nfunction of the domain enclosed by the ellipse of semi-axes sqrt{1 \u2212 \u03b1} and sqrt{1 + \u03b1}. This<br \/>\r\nresult is one of the very few examples where the minimiser of a nonlocal anisotropic<br \/>\r\nenergy is explicitly computed. For the proof we borrow techniques from fluid dynamics,<br \/>\r\nin particular those related to Kirchhoff\u2019s celebrated result that domains enclosed by<br \/>\r\nellipses are rotating vortex patches, called Kirchhoff ellipses.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('14','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_14\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/The-ellipse-law.Comm_.Math_.Physics-2.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/The-ellipse-law.C[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/12\/The-ellipse-law.C[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/Digital Object Identifier (DOI) https:\/\/doi.org\/10.1007\/s00220-019-03368-w\" title=\"Follow DOI:Digital Object Identifier (DOI) https:\/\/doi.org\/10.1007\/s00220-019-03368-w\" target=\"_blank\">doi:Digital Object Identifier (DOI) https:\/\/doi.org\/10.1007\/s00220-019-03368-w<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('14','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('45','tp_links')\" style=\"cursor:pointer;\">A maximum-principle approach to the minimisation of a nonlocal energy<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Mathematics in Engineering, <\/span><span class=\"tp_pub_additional_volume\">vol. 2, <\/span><span class=\"tp_pub_additional_issue\">iss. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 253-263, <\/span><span class=\"tp_pub_additional_year\">2020<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_45\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('45','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_45\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('45','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_45\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('45','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_45\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {A maximum-principle approach to the minimisation of a nonlocal energy},<br \/>\r\nauthor = {Joan Mateu, Maria Giovanna Mora, Luca Rondi, Lucia Scardia and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV_Max_Principle.pdf},<br \/>\r\nyear  = {2020},<br \/>\r\ndate = {2020-01-01},<br \/>\r\nurldate = {2020-01-01},<br \/>\r\njournal = {Mathematics in Engineering},<br \/>\r\nvolume = {2},<br \/>\r\nissue = {2},<br \/>\r\npages = {253-263},<br \/>\r\nabstract = {In this paper we use an approach based on the maximum principle to characterise the minimiser of a family of nonlocal and anisotropic energies I\u000b defined on probability measures in R2. The purely nonlocal term in I\u000b is of convolution type, and is isotropic for \u000b = 0 and anisotropic otherwise. The cases \u000b = 0 and \u000b = 1 are special: The first corresponds to Coulombic interactions, and the latter to dislocations. The minimisers of I\u000b have been characterised by the same authors in an earlier paper, by exploiting some formal similarities with the Euler equation, and by means of complex-analysis techniques. We here propose a di\u000berent approach, that we believe can be applied to more general energies. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('45','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_45\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we use an approach based on the maximum principle to characterise the minimiser of a family of nonlocal and anisotropic energies I\u000b defined on probability measures in R2. The purely nonlocal term in I\u000b is of convolution type, and is isotropic for \u000b = 0 and anisotropic otherwise. The cases \u000b = 0 and \u000b = 1 are special: The first corresponds to Coulombic interactions, and the latter to dislocations. The minimisers of I\u000b have been characterised by the same authors in an earlier paper, by exploiting some formal similarities with the Euler equation, and by means of complex-analysis techniques. We here propose a di\u000berent approach, that we believe can be applied to more general energies. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('45','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_45\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV_Max_Principle.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV_Max_Princip[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MMRSV_Max_Princip[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('45','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2019\">2019<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('44','tp_links')\" style=\"cursor:pointer;\">Capacitary differentiability of potentials of finite Radon measures  <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Arkiv f\u00f6r Matematik, <\/span><span class=\"tp_pub_additional_volume\">vol. 57, <\/span><span class=\"tp_pub_additional_issue\">iss. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 473-450, <\/span><span class=\"tp_pub_additional_year\">2019<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_44\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('44','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_44\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('44','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_44\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('44','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_44\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Capacitary differentiability of potentials of finite Radon measures  },<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiabilty_Potentials-1.pdf},<br \/>\r\nyear  = {2019},<br \/>\r\ndate = {2019-01-01},<br \/>\r\njournal = {Arkiv f\\\"{o}r Matematik},<br \/>\r\nvolume = {57},<br \/>\r\nissue = {2},<br \/>\r\npages = {473-450},<br \/>\r\nabstract = {We present alternative proofs of two results proven in a recent preprint of Ambrosio, Ponce and Rodiac arXiv:1810.03924 . Each proof provides, in addition, improvements on the original statements. The context is the following. We have a kernel K of class C2 off the origin of RN, whose absolute value is less than or equal to \u2223\u2223x\u2223\u2223\u2212N+1. Similarly its gradient is controlled by \u2223\u2223x\u2223\u2223\u2212N and its second order derivatives by \u2223\u2223x\u2223\u2223\u2212N\u22121. Consider the potential u=K\u2217m where m is a finite Radon measure. We prove that u is differentiable in the capacitary sense a.e. , which means that for almost all a the normalized weak capacitary \"norm\" of the first order remainder of u in a ball of radius r centered at a tends to 0 with r. This implies differentiability in the weak N\/(N\u22121) norm, thus differentiability in Lp for p larger than or equal to 1 and less that N\/(N\u22121), which in turn implies approximate differentiability (which is a result of Hajlasz from 1996). As a second result we prove that u satisfies a Lipschitz pointwise condition, for almost all pairs of points x and y, with Lipschitz constant less than L(x)+L(y) for a weak L1 function L. In fact, there is a canonical choice for L, namely the sum of the Hardy-Littlewood maximal function of the measure m and the maximal singular integral associated with the gradient of K convolved with m. Note that the gradient of K has the growth and cancellation properties of a Calder\\`{o}n -Zygmund kernel. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('44','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_44\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We present alternative proofs of two results proven in a recent preprint of Ambrosio, Ponce and Rodiac arXiv:1810.03924 . Each proof provides, in addition, improvements on the original statements. The context is the following. We have a kernel K of class C2 off the origin of RN, whose absolute value is less than or equal to \u2223\u2223x\u2223\u2223\u2212N+1. Similarly its gradient is controlled by \u2223\u2223x\u2223\u2223\u2212N and its second order derivatives by \u2223\u2223x\u2223\u2223\u2212N\u22121. Consider the potential u=K\u2217m where m is a finite Radon measure. We prove that u is differentiable in the capacitary sense a.e. , which means that for almost all a the normalized weak capacitary &quot;norm&quot; of the first order remainder of u in a ball of radius r centered at a tends to 0 with r. This implies differentiability in the weak N\/(N\u22121) norm, thus differentiability in Lp for p larger than or equal to 1 and less that N\/(N\u22121), which in turn implies approximate differentiability (which is a result of Hajlasz from 1996). As a second result we prove that u satisfies a Lipschitz pointwise condition, for almost all pairs of points x and y, with Lipschitz constant less than L(x)+L(y) for a weak L1 function L. In fact, there is a canonical choice for L, namely the sum of the Hardy-Littlewood maximal function of the measure m and the maximal singular integral associated with the gradient of K convolved with m. Note that the gradient of K has the growth and cancellation properties of a Calder\u00f2n -Zygmund kernel. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('44','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_44\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiabilty_Potentials-1.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiabilty_[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiabilty_[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('44','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2018\">2018<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Juli\u00e0 Cuf\u00ed; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('42','tp_links')\" style=\"cursor:pointer;\">Differentiability properties of Riesz potentials of finite measures, and non-doubling Calder\u00f3n-Zygmund theory<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Annali della Scuola Normale Superiore di Pisa, <\/span><span class=\"tp_pub_additional_volume\">vol. 5, <\/span><span class=\"tp_pub_additional_pages\">pp. 1081-1123, <\/span><span class=\"tp_pub_additional_year\">2018<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_42\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('42','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_42\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('42','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_42\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('42','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_42\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Differentiability properties of Riesz potentials of finite measures, and non-doubling Calder\\'{o}n-Zygmund theory},<br \/>\r\nauthor = {Juli\\`{a} Cuf\\'{i} and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiability_Equilibrium.pdf},<br \/>\r\nyear  = {2018},<br \/>\r\ndate = {2018-01-01},<br \/>\r\nurldate = {2018-01-01},<br \/>\r\njournal = {Annali della Scuola Normale Superiore di Pisa},<br \/>\r\nvolume = {5},<br \/>\r\npages = {1081-1123},<br \/>\r\nabstract = {We study differentiability properties of Riesz potentials of finite Borel measures in dimension d larger than 2. The Riesz kernel has homogeneity 2-d. In dimension 2 we consider logarithmic potentials. We introduce a notion of differentiability in the capacity sense, capacity being Newtonian capacity in dimension larger than 2 and Wiener capacity in the plane. It turns out that differentiability in the capacity sense at a point is related to the existence of principal values of the measure with respect to the vector valued Riesz potential x\/|x|^d of homogeneity 1-d. This leads to Calder'on-Zygmund theory for non-doubling measures. We prove that the Riesz potential of a finite Borel measure is differentiable in the capacity sense except for a set of zero C^1-harmonic capacity. This result is sharp. Surprisingly in the plane there are two distinct notions of differentiability in the capacity sense. For each of them we obtain the best possible result on the size of the exceptional set in terms of Hausdorff measures. We obtain for dimension larger than 2 results on Peano second order differentiability in the capacity sense with exceptional sets of zero Lebesgue measure. As an application of our differentiability results we present a new proof of the well-known fact that the equilibrium measure is singular with respect to Lebesgue measure.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('42','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_42\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We study differentiability properties of Riesz potentials of finite Borel measures in dimension d larger than 2. The Riesz kernel has homogeneity 2-d. In dimension 2 we consider logarithmic potentials. We introduce a notion of differentiability in the capacity sense, capacity being Newtonian capacity in dimension larger than 2 and Wiener capacity in the plane. It turns out that differentiability in the capacity sense at a point is related to the existence of principal values of the measure with respect to the vector valued Riesz potential x\/|x|^d of homogeneity 1-d. This leads to Calder'on-Zygmund theory for non-doubling measures. We prove that the Riesz potential of a finite Borel measure is differentiable in the capacity sense except for a set of zero C^1-harmonic capacity. This result is sharp. Surprisingly in the plane there are two distinct notions of differentiability in the capacity sense. For each of them we obtain the best possible result on the size of the exceptional set in terms of Hausdorff measures. We obtain for dimension larger than 2 results on Peano second order differentiability in the capacity sense with exceptional sets of zero Lebesgue measure. As an application of our differentiability results we present a new proof of the well-known fact that the equilibrium measure is singular with respect to Lebesgue measure.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('42','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_42\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiability_Equilibrium.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiability[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Differentiability[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('42','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2016\">2016<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">A. Bertozzi, J. Garnett, T. Laurent; J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('41','tp_links')\" style=\"cursor:pointer;\">The regularity of the boundary of a multidimensional aggregation patch <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">SIAM Journal on Mathematical Analysis, <\/span><span class=\"tp_pub_additional_volume\">vol. 48, <\/span><span class=\"tp_pub_additional_issue\">iss. 6, <\/span><span class=\"tp_pub_additional_pages\">pp. 3789-3819, <\/span><span class=\"tp_pub_additional_year\">2016<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_41\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('41','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_41\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('41','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_41\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('41','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_41\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The regularity of the boundary of a multidimensional aggregation patch },<br \/>\r\nauthor = {A. Bertozzi, J. Garnett, T. Laurent and J. Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/BGLV_July_2016.pdf},<br \/>\r\nyear  = {2016},<br \/>\r\ndate = {2016-07-01},<br \/>\r\nurldate = {2016-07-01},<br \/>\r\njournal = {SIAM Journal on Mathematical Analysis},<br \/>\r\nvolume = {48},<br \/>\r\nissue = {6},<br \/>\r\npages = {3789-3819},<br \/>\r\nabstract = {We study weak solutions of the aggregation equation with velocity field given by convolution of the density with minus the gradient of the fundamental solution of the Laplacian in d-dimensional euclidean space, with initial density the characteristic function of a domain with smooth boundary. Thus the divergence of the field is minus the density. It is known that the density at time t is given by the characteristic function of a domain D_t divided by 1-t, so that at time t=1 we have a blow up. The purpose of the article is to show that the domain D_t preserves boundary smoothness up to the blow up time and going backwards in time till minus infinity. The result may be understood as an aggregation analogue of Chemin's boundary regularity theorem for vortex patches for the vorticity form of Euler's equation. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('41','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_41\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We study weak solutions of the aggregation equation with velocity field given by convolution of the density with minus the gradient of the fundamental solution of the Laplacian in d-dimensional euclidean space, with initial density the characteristic function of a domain with smooth boundary. Thus the divergence of the field is minus the density. It is known that the density at time t is given by the characteristic function of a domain D_t divided by 1-t, so that at time t=1 we have a blow up. The purpose of the article is to show that the domain D_t preserves boundary smoothness up to the blow up time and going backwards in time till minus infinity. The result may be understood as an aggregation analogue of Chemin's boundary regularity theorem for vortex patches for the vorticity form of Euler's equation. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('41','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_41\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/BGLV_July_2016.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/BGLV_July_2016.pd[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/BGLV_July_2016.pd[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('41','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Dorina Mitrea, Marius Mitrea; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('40','tp_links')\" style=\"cursor:pointer;\">Characterizing Lyapunov domains via Riesz transforms on H\u00f6lder spaces<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Analysis &amp; Partial Differential Equations, <\/span><span class=\"tp_pub_additional_volume\">vol. 9, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 955-1018, <\/span><span class=\"tp_pub_additional_year\">2016<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_40\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('40','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_40\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('40','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_40\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('40','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_40\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Characterizing Lyapunov domains via Riesz transforms on H\\\"{o}lder spaces},<br \/>\r\nauthor = {Dorina Mitrea, Marius Mitrea and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/SIO_Holder16.pdf},<br \/>\r\nyear  = {2016},<br \/>\r\ndate = {2016-01-02},<br \/>\r\nurldate = {2016-01-02},<br \/>\r\njournal = {Analysis \\& Partial Differential Equations},<br \/>\r\nvolume = {9},<br \/>\r\nnumber = {4},<br \/>\r\npages = {955-1018},<br \/>\r\nabstract = {Under mild geometric measure theoretic assumptions on an open set \u03a9\u2282\u211dn, we show that the Riesz transforms on its boundary are continuous mappings on the H\\\"{o}lder space \u2102\u03b1(\u2202\u03a9) if and only if \u03a9 is a Lyapunov domain of order \u03b1 (i.e., a domain of class \ud835\udc9e1+\u03b1). In the category of Lyapunov domains we also establish the boundedness on H\\\"{o}lder spaces of singular integral operators with kernels of the form P(x\u2212y)\/\u2223\u2223x\u2212y\u2223\u2223n\u22121+l, where P is any odd homogeneous polynomial of degree l in \u211dn. This family of singular integral operators, which may be thought of as generalized Riesz transforms, includes the boundary layer potentials associated with basic PDE's of mathematical physics, such as the Laplacian, the Lam'e system, and the Stokes system. We also consider the limiting case \u03b1=0 (with VMO(\u2202\u03a9) as the natural replacement of \ud835\udc9e\u03b1(\u2202\u03a9)), and discuss an extension to the scale of Besov spaces. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('40','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_40\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Under mild geometric measure theoretic assumptions on an open set \u03a9\u2282\u211dn, we show that the Riesz transforms on its boundary are continuous mappings on the H\u00f6lder space \u2102\u03b1(\u2202\u03a9) if and only if \u03a9 is a Lyapunov domain of order \u03b1 (i.e., a domain of class \ud835\udc9e1+\u03b1). In the category of Lyapunov domains we also establish the boundedness on H\u00f6lder spaces of singular integral operators with kernels of the form P(x\u2212y)\/\u2223\u2223x\u2212y\u2223\u2223n\u22121+l, where P is any odd homogeneous polynomial of degree l in \u211dn. This family of singular integral operators, which may be thought of as generalized Riesz transforms, includes the boundary layer potentials associated with basic PDE's of mathematical physics, such as the Laplacian, the Lam'e system, and the Stokes system. We also consider the limiting case \u03b1=0 (with VMO(\u2202\u03a9) as the natural replacement of \ud835\udc9e\u03b1(\u2202\u03a9)), and discuss an extension to the scale of Besov spaces. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('40','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_40\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/SIO_Holder16.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/SIO_Holder16.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/SIO_Holder16.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('40','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Taoufik Hmidi, Francisco de la Hoz, Joan Mateu; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('39','tp_links')\" style=\"cursor:pointer;\">Doubly connected V-states for the planar Euler equations<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">SIAM Journal on Mathematical Analysis, <\/span><span class=\"tp_pub_additional_volume\">vol. 48, <\/span><span class=\"tp_pub_additional_number\">no. 3, <\/span><span class=\"tp_pub_additional_pages\">pp. 1892-1928, <\/span><span class=\"tp_pub_additional_year\">2016<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_39\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('39','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_39\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('39','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_39\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('39','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_39\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Doubly connected V-states for the planar Euler equations},<br \/>\r\nauthor = {Taoufik Hmidi, Francisco de la Hoz, Joan Mateu and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Doubly_Connected_V_States.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1137\/140992801},<br \/>\r\nyear  = {2016},<br \/>\r\ndate = {2016-01-01},<br \/>\r\nurldate = {2016-01-01},<br \/>\r\njournal = {SIAM Journal on Mathematical Analysis},<br \/>\r\nvolume = {48},<br \/>\r\nnumber = {3},<br \/>\r\npages = {1892-1928},<br \/>\r\nabstract = {We prove existence of doubly connected V-states for the planar Euler equations which are not annuli. The proof proceeds by bifurcation from annuli at simple \"eigenvalues\". The bifurcated V -states we obtain enjoy a m-fold symmetry for some m larger than or equal to 3: The existence of doubly connected V -states of strict 2-fold symmetry remains an open question. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('39','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_39\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We prove existence of doubly connected V-states for the planar Euler equations which are not annuli. The proof proceeds by bifurcation from annuli at simple &quot;eigenvalues&quot;. The bifurcated V -states we obtain enjoy a m-fold symmetry for some m larger than or equal to 3: The existence of doubly connected V -states of strict 2-fold symmetry remains an open question. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('39','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_39\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Doubly_Connected_V_States.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Doubly_Connected_[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Doubly_Connected_[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1137\/140992801\" title=\"Follow DOI:https:\/\/doi.org\/10.1137\/140992801\" target=\"_blank\">doi:https:\/\/doi.org\/10.1137\/140992801<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('39','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2015\">2015<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Juli\u00e0 Cuf\u00ed; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('38','tp_links')\" style=\"cursor:pointer;\">A general form of Green Formula and Cauchy Integral Theorem<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Proceedings of the American Mathematical Society, <\/span><span class=\"tp_pub_additional_volume\">vol. 143, <\/span><span class=\"tp_pub_additional_pages\">pp. 2091-2102, <\/span><span class=\"tp_pub_additional_year\">2015<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_38\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('38','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_38\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('38','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_38\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('38','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_38\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {A general form of Green Formula and Cauchy Integral Theorem},<br \/>\r\nauthor = {Juli\\`{a} Cuf\\'{i} and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Green_Cauchy.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1090\/S0002-9939-2014-12418-X},<br \/>\r\nyear  = {2015},<br \/>\r\ndate = {2015-01-02},<br \/>\r\nurldate = {2015-01-02},<br \/>\r\njournal = {Proceedings of the American Mathematical Society},<br \/>\r\nvolume = {143},<br \/>\r\npages = {2091-2102},<br \/>\r\nabstract = {We prove a general form of Green\u00b4s formula for arbitrary rectifiable curves involving the index function. The function f to which the formula applies is continuous on the complement of the open set where the index vanishes and its d-bar derivative is square integrable on the open set where the index in non-zero. The formula states that the integral of f(z) on the curve is, modulo multiplicative constants, the integral of the index function times the d-bar derivative of f. It is well-known that the index is square integrable in the plane, and this explains the hypothesis on the square integrability of the d-bar derivative of f. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('38','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_38\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We prove a general form of Green\u00b4s formula for arbitrary rectifiable curves involving the index function. The function f to which the formula applies is continuous on the complement of the open set where the index vanishes and its d-bar derivative is square integrable on the open set where the index in non-zero. The formula states that the integral of f(z) on the curve is, modulo multiplicative constants, the integral of the index function times the d-bar derivative of f. It is well-known that the index is square integrable in the plane, and this explains the hypothesis on the square integrability of the d-bar derivative of f. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('38','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_38\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Green_Cauchy.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Green_Cauchy.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Green_Cauchy.pdf<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1090\/S0002-9939-2014-12418-X\" title=\"Follow DOI:https:\/\/doi.org\/10.1090\/S0002-9939-2014-12418-X\" target=\"_blank\">doi:https:\/\/doi.org\/10.1090\/S0002-9939-2014-12418-X<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('38','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Taoufik Hmidi, Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('37','tp_links')\" style=\"cursor:pointer;\">On rotating doubly connected vortices<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Journal of differential equations, <\/span><span class=\"tp_pub_additional_volume\">vol. 258, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 1395-1429, <\/span><span class=\"tp_pub_additional_year\">2015<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_37\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('37','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_37\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('37','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_37\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('37','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_37\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {On rotating doubly connected vortices},<br \/>\r\nauthor = {Joan Mateu, Taoufik Hmidi, Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/On_rotating_doubly_connected_vortices2.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1016\/j.jde.2014.10.021},<br \/>\r\nyear  = {2015},<br \/>\r\ndate = {2015-01-01},<br \/>\r\nurldate = {2015-01-01},<br \/>\r\njournal = {Journal of differential equations},<br \/>\r\nvolume = {258},<br \/>\r\nnumber = {4},<br \/>\r\npages = {1395-1429},<br \/>\r\nabstract = {In this paper we consider rotating doubly connected vortex patches for the Euler equations in the plane. When the inner interface is an ellipse we show that the exterior interface must be a confocal ellipse. We then discuss some relations, first found by Flierl and Polvani, between the parameters of the ellipses, the velocity of rotation and the magnitude of the vorticity in the domain enclosed by the inner ellipse. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('37','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_37\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we consider rotating doubly connected vortex patches for the Euler equations in the plane. When the inner interface is an ellipse we show that the exterior interface must be a confocal ellipse. We then discuss some relations, first found by Flierl and Polvani, between the parameters of the ellipses, the velocity of rotation and the magnitude of the vorticity in the domain enclosed by the inner ellipse. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('37','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_37\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/On_rotating_doubly_connected_vortices2.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/On_rotating_doubl[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/On_rotating_doubl[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1016\/j.jde.2014.10.021\" title=\"Follow DOI:https:\/\/doi.org\/10.1016\/j.jde.2014.10.021\" target=\"_blank\">doi:https:\/\/doi.org\/10.1016\/j.jde.2014.10.021<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('37','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2013\">2013<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Taoufik Hmidi Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('35','tp_links')\" style=\"cursor:pointer;\"> Boundary Regularity of Rotating Vortex Patches<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Archive for Rational Mechanics and Analysis, <\/span><span class=\"tp_pub_additional_volume\">vol. 209, <\/span><span class=\"tp_pub_additional_number\">no. 1, <\/span><span class=\"tp_pub_additional_pages\">pp. 171-208, <\/span><span class=\"tp_pub_additional_year\">2013<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_35\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('35','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_35\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('35','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_35\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('35','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_35\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = { Boundary Regularity of Rotating Vortex Patches},<br \/>\r\nauthor = {Joan Mateu, Taoufik Hmidi Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_regularity_ARMA_2013.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1007\/s00205-013-0618-8},<br \/>\r\nyear  = {2013},<br \/>\r\ndate = {2013-01-01},<br \/>\r\nurldate = {2013-01-01},<br \/>\r\njournal = {Archive for Rational Mechanics and Analysis},<br \/>\r\nvolume = {209},<br \/>\r\nnumber = {1},<br \/>\r\npages = {171-208},<br \/>\r\nabstract = {A vortex patch is a special solution of the vorticity equation in the plane corresponding to an initial condition which is the characteristic function of a domain D0. In other words, at time 0 vorticity is 1 in D0 and 0 in the complement. Since vorticity is preserved along trajectories at time t vorticity is 1 on a domain Dt and 0 elsewhere. Numerical simulations show that Dt develops a very complicated structure. For instance the boundary ejects filaments and lenght increases much faster than exponentially. In spite of that, Kirchhoff had showed at the end of the nineteenth century that ellipses just rotate around the center of mass with a constant angular velocity determined by the lengths of the semi-axes. Other \"rotating vortex patches\" were discovered numerically by Deem and Zabusky (who called them \"V-states\") in the early eighties. Burbea succeeded in giving an analytic existence proof by bifurcation. In the pictures coming from the simulations one sees V-states bifurcating from the circle with m-fold symmetry, m=2, 3, ... which evolve till corners appear at the end of the bifurcation branch. These corners are at right angles and nobody knows the mechanism by which they are created. In this paper we show that the bifurcated V-state has smooth boundary provided it is close enough to the bifurcation circle in a Lipschitz sense. The proof uses classical regularity theorems for conformal mappings, estimates of singular integral operators on H\\\"{o}lder spaces and the special form of the boundary equation of V-states, which allows a subtle boot strap argument. Many interesting questions arise. For example, why corners are formed ? Can one find new V-states by new methods not involving bifurcation ? This is a modified version of the paper published in Arch. Ration. Mech. Anal. 209 (2013), no. 1, 171-208, which contains some simplified proofs (see at the end on the introduction a detailed account of the modifications). },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('35','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_35\" style=\"display:none;\"><div class=\"tp_abstract_entry\">A vortex patch is a special solution of the vorticity equation in the plane corresponding to an initial condition which is the characteristic function of a domain D0. In other words, at time 0 vorticity is 1 in D0 and 0 in the complement. Since vorticity is preserved along trajectories at time t vorticity is 1 on a domain Dt and 0 elsewhere. Numerical simulations show that Dt develops a very complicated structure. For instance the boundary ejects filaments and lenght increases much faster than exponentially. In spite of that, Kirchhoff had showed at the end of the nineteenth century that ellipses just rotate around the center of mass with a constant angular velocity determined by the lengths of the semi-axes. Other &quot;rotating vortex patches&quot; were discovered numerically by Deem and Zabusky (who called them &quot;V-states&quot;) in the early eighties. Burbea succeeded in giving an analytic existence proof by bifurcation. In the pictures coming from the simulations one sees V-states bifurcating from the circle with m-fold symmetry, m=2, 3, ... which evolve till corners appear at the end of the bifurcation branch. These corners are at right angles and nobody knows the mechanism by which they are created. In this paper we show that the bifurcated V-state has smooth boundary provided it is close enough to the bifurcation circle in a Lipschitz sense. The proof uses classical regularity theorems for conformal mappings, estimates of singular integral operators on H\u00f6lder spaces and the special form of the boundary equation of V-states, which allows a subtle boot strap argument. Many interesting questions arise. For example, why corners are formed ? Can one find new V-states by new methods not involving bifurcation ? This is a modified version of the paper published in Arch. Ration. Mech. Anal. 209 (2013), no. 1, 171-208, which contains some simplified proofs (see at the end on the introduction a detailed account of the modifications). <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('35','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_35\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_regularity_ARMA_2013.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_regulari[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Boundary_regulari[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1007\/s00205-013-0618-8\" title=\"Follow DOI:https:\/\/doi.org\/10.1007\/s00205-013-0618-8\" target=\"_blank\">doi:https:\/\/doi.org\/10.1007\/s00205-013-0618-8<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('35','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Kari Astala, Albert Clop, Ignacio Uriarte-Tuero, Xavier Tolsa Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('36','tp_links')\" style=\"cursor:pointer;\">Quasiconformal distorsion of Riesz capacities and Hausdorff measures in the plane<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">American Journal of Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 135, <\/span><span class=\"tp_pub_additional_number\">no. 1, <\/span><span class=\"tp_pub_additional_pages\">pp. 17-52, <\/span><span class=\"tp_pub_additional_year\">2013<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_36\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('36','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_36\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('36','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_36\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('36','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_36\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Quasiconformal distorsion of Riesz capacities and Hausdorff measures in the plane},<br \/>\r\nauthor = {Kari Astala, Albert Clop, Ignacio Uriarte-Tuero, Xavier Tolsa Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ACUTV.pdf},<br \/>\r\nyear  = {2013},<br \/>\r\ndate = {2013-01-01},<br \/>\r\nurldate = {2013-01-01},<br \/>\r\njournal = {American Journal of Mathematics},<br \/>\r\nvolume = {135},<br \/>\r\nnumber = {1},<br \/>\r\npages = {17-52},<br \/>\r\nabstract = {In this paper we prove sharp distortion estimates for quasi-conformal mappings in the plane, both in terms of the Riesz capacities from non linear potential theory and in terms of Hausdorff measures. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('36','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_36\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we prove sharp distortion estimates for quasi-conformal mappings in the plane, both in terms of the Riesz capacities from non linear potential theory and in terms of Hausdorff measures. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('36','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_36\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ACUTV.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ACUTV.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ACUTV.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('36','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2012\">2012<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Roc Alabern, Joan Mateu; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('34','tp_links')\" style=\"cursor:pointer;\">A new characterization of Sobolev spaces on R^n<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Mathematische Annalen, <\/span><span class=\"tp_pub_additional_volume\">vol. 354, <\/span><span class=\"tp_pub_additional_number\">no. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 589-626, <\/span><span class=\"tp_pub_additional_year\">2012<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_34\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('34','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_34\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('34','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_34\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('34','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_34\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {A new characterization of Sobolev spaces on R^n},<br \/>\r\nauthor = {Roc Alabern, Joan Mateu and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Sobolev_Corrected.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1007\/s00208-011-0738-0},<br \/>\r\nyear  = {2012},<br \/>\r\ndate = {2012-01-01},<br \/>\r\nurldate = {2012-01-01},<br \/>\r\njournal = {Mathematische Annalen},<br \/>\r\nvolume = {354},<br \/>\r\nnumber = {2},<br \/>\r\npages = {589-626},<br \/>\r\nabstract = {In this paper we present a new characterization of Sobolev spaces on the Euclidean spaces Rn. Our characterizing condition is obtained via a quadratic multiscale expression which exploits the particular symmetry properties of Euclidean space. The most interesting feature of our condition is that depends only on the metric of Rn and the Lebesgue measure, so that one can define in a relatively simple way Sobolev spaces of any order of smoothness on any metric measure space. It is an open question whether our condition characterizes Sobolev spaces on subdomains of Rn with smooth boundary. It is also not known for which metric measure spaces our condition for first order Sobolev spaces is equivalent to Hajlasz's definition. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('34','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_34\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we present a new characterization of Sobolev spaces on the Euclidean spaces Rn. Our characterizing condition is obtained via a quadratic multiscale expression which exploits the particular symmetry properties of Euclidean space. The most interesting feature of our condition is that depends only on the metric of Rn and the Lebesgue measure, so that one can define in a relatively simple way Sobolev spaces of any order of smoothness on any metric measure space. It is an open question whether our condition characterizes Sobolev spaces on subdomains of Rn with smooth boundary. It is also not known for which metric measure spaces our condition for first order Sobolev spaces is equivalent to Hajlasz's definition. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('34','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_34\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Sobolev_Corrected.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Sobolev_Corrected[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Sobolev_Corrected[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1007\/s00208-011-0738-0\" title=\"Follow DOI:https:\/\/doi.org\/10.1007\/s00208-011-0738-0\" target=\"_blank\">doi:https:\/\/doi.org\/10.1007\/s00208-011-0738-0<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('34','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2011\">2011<\/h3><div class=\"tp_publication tp_publication_proceedings\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('32','tp_links')\" style=\"cursor:pointer;\">The Maximal Singular Integral: estimates in terms of the Singular Integral<\/a> <span class=\"tp_pub_type tp_  proceedings\">Proceedings<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_howpublished\">XXXI Conference in Harmonic Analysis, <\/span><span class=\"tp_pub_additional_year\">2011<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_32\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('32','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_32\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('32','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_32\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('32','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_32\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@proceedings{nokey,<br \/>\r\ntitle = {The Maximal Singular Integral: estimates in terms of the Singular Integral},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Sing_Proc_Roma.pdf},<br \/>\r\nyear  = {2011},<br \/>\r\ndate = {2011-06-01},<br \/>\r\nurldate = {2011-06-01},<br \/>\r\nissue = {Springer Verlag, Rome},<br \/>\r\nabstract = {In this expository paper we consider the problem of estimating the maximal singular integral T\u2217f in terms of the singular Tf only. The most basic instance of the estimates we look for is the L2(Rn) estimate of T\u2217f in terms of Tf. We describe the complete characterization, recently been obtained by Mateu, Orobitg, P\\'{e}rez and the author, of the smooth homogeneous convolution Calder\\'{o}n-Zygmund operators for which such inequality holds. We concentrate on special cases of the general statement to convey the main ideas of the proofs in a transparent way, as free as possible of the technical complications inherent to the general case. Particular attention is devoted to higher Riesz transforms. },<br \/>\r\nhowpublished = {XXXI Conference in Harmonic Analysis},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {proceedings}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('32','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_32\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this expository paper we consider the problem of estimating the maximal singular integral T\u2217f in terms of the singular Tf only. The most basic instance of the estimates we look for is the L2(Rn) estimate of T\u2217f in terms of Tf. We describe the complete characterization, recently been obtained by Mateu, Orobitg, P\u00e9rez and the author, of the smooth homogeneous convolution Calder\u00f3n-Zygmund operators for which such inequality holds. We concentrate on special cases of the general statement to convey the main ideas of the proofs in a transparent way, as free as possible of the technical complications inherent to the general case. Particular attention is devoted to higher Riesz transforms. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('32','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_32\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Sing_Proc_Roma.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Sing_Proc[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Sing_Proc[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('32','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Laura Prat, Joan Mateu; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('30','tp_links')\" style=\"cursor:pointer;\">Capacities associated with scalar signed Riesz kernels, and analytic capacity<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Indiana university mathematics journal, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 1319\u20131361, <\/span><span class=\"tp_pub_additional_year\">2011<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_30\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('30','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_30\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('30','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_30\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('30','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_30\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Capacities associated with scalar signed Riesz kernels, and analytic capacity},<br \/>\r\nauthor = {Laura Prat, Joan Mateu and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MPV_Indiana_Preprint.pdf},<br \/>\r\nyear  = {2011},<br \/>\r\ndate = {2011-01-01},<br \/>\r\nurldate = {2011-01-01},<br \/>\r\njournal = {Indiana university mathematics journal},<br \/>\r\nnumber = {4},<br \/>\r\npages = {1319\\textendash1361},<br \/>\r\nabstract = {The real and imaginary parts of the Cauchy kernel in the plane are scalar Riesz kernels of homogeneity -1. One can associate with each of them a natural notion of capacity related to bounded potentials. A simple argument combined with a deep result of Tolsa shows that each of the capacities associated with the real or imaginary parts of the Cauchy kernel is comparable to analytic capacity. This stresses the real variables nature of analytic capacity. Higher dimensional versions of this result are considered in this paper. We replace the Cauchy kernel with the vector valued Riesz kernel of homogeneity -1 in the n-dimensional euclidean space. One needs to work with n-1 distinct components of the vector valued Riesz kernel. A capacity is associated with these n-1 components and bounded potentials. As it turns out, boundedness of distinct n-1 scalar Riesz potentials of a distribution does not guarantee that the distribution satisfies any growth condition. Thus one has to require the natural growth condition to the distributions used to define the capacity. Our main result deals with the comparability of the vector valued Riesz capacity and that arising by considering the n-1 distinct components chosen. It is a curious fact that the Hardy space H1(Rn) enters naturally the scene in odd dimensions when one defines the appropriate notion of growth condition on a distribution. In even dimensions the growth condition can be formulated in terms of L1 only. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('30','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_30\" style=\"display:none;\"><div class=\"tp_abstract_entry\">The real and imaginary parts of the Cauchy kernel in the plane are scalar Riesz kernels of homogeneity -1. One can associate with each of them a natural notion of capacity related to bounded potentials. A simple argument combined with a deep result of Tolsa shows that each of the capacities associated with the real or imaginary parts of the Cauchy kernel is comparable to analytic capacity. This stresses the real variables nature of analytic capacity. Higher dimensional versions of this result are considered in this paper. We replace the Cauchy kernel with the vector valued Riesz kernel of homogeneity -1 in the n-dimensional euclidean space. One needs to work with n-1 distinct components of the vector valued Riesz kernel. A capacity is associated with these n-1 components and bounded potentials. As it turns out, boundedness of distinct n-1 scalar Riesz potentials of a distribution does not guarantee that the distribution satisfies any growth condition. Thus one has to require the natural growth condition to the distributions used to define the capacity. Our main result deals with the comparability of the vector valued Riesz capacity and that arising by considering the n-1 distinct components chosen. It is a curious fact that the Hardy space H1(Rn) enters naturally the scene in odd dimensions when one defines the appropriate notion of growth condition on a distribution. In even dimensions the growth condition can be formulated in terms of L1 only. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('30','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_30\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MPV_Indiana_Preprint.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MPV_Indiana_Prepr[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MPV_Indiana_Prepr[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('30','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Joan Orobitg, Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('31','tp_links')\" style=\"cursor:pointer;\">Estimates for the maximal singular integral in terms of the singular integral: the case of even kernels <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Annals of Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 174, <\/span><span class=\"tp_pub_additional_issue\">iss. 3, <\/span><span class=\"tp_pub_additional_pages\">pp. 1429-1483, <\/span><span class=\"tp_pub_additional_year\">2011<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_31\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('31','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_31\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('31','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_31\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('31','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_31\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Estimates for the maximal singular integral in terms of the singular integral: the case of even kernels },<br \/>\r\nauthor = {Joan Mateu, Joan Orobitg, Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MaximalSingular_2010.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.4007\/annals.2011.174.3.2},<br \/>\r\nyear  = {2011},<br \/>\r\ndate = {2011-01-01},<br \/>\r\nurldate = {2011-01-01},<br \/>\r\njournal = {Annals of Mathematics},<br \/>\r\nvolume = {174},<br \/>\r\nissue = {3},<br \/>\r\npages = {1429-1483},<br \/>\r\nabstract = {Let T be a homogeneous smooth Calder\\'{o}n-Zygmund operator in Euclidean space and let T^\u2217 stand for the maximal singular integral, i. e., the supremum of the truncations of T. In this paper we consider the problem of controlling T^\u2217(f) by T(f). We are mostly interested in estimating the L2 norm of T^\u2217(f) by the L^2 norm of T(f). The problem arose when trying to obtain existence of principal values from the L^2 boundedness of the singular integral in a rather general context in which the underlying measure in much more general than Lebesgue measure (see the paper \"Convergence of singular integrals with general measures\", by P.Mattila and J.Verdera). This in turn was motivated by a problem of David and Semmes, which asks whether rectifiability of the support of the underlying measure follows from L^2 boundedness for the Riesz kernels. In our problem the parity of the kernel plays an essential role and in this paper we deal only with even kernels. The odd case is, in some ways, easier and will be treated in a subsequent article. Our first result is that for even higher order Riesz transforms one has a pointwise estimate of T^\u2217(f) by a constant times M(T(f)), where M is the Hardy-Littlewood maximal function. This fails for odd kernels (indeed for the Hilbert Transform), as was shown by Mateu and Verdera (Math.Research Letters (2006)). Clearly the above pointwise estimate implies the L^2 estimate of T^\u2217(f) by T(f). Notice that our pointwise estimate improves substantially classical Cotlar's inequality, because the term M(f) is missing in the right hand side. We may then informally call it Super Cotlar's inequality. There are simple polynomial homogeneous Calder\\'{o}n-Zygmund operators for which the L^2 control of T^\u2217(f) by T(f) is not possible. For example, for T=B+B^2, where B is the Beurling transform. Showing this requires some work involving multipliers. The question then arises of how one may characterize those T for which the above L^2 control is possible. The main result of the paper gives such a condition. The characterization is as follows: T must be of the form R composed with U, where R is a higher order Riesz transform associated with some harmonic polynomial P(x) and U is an invertible operator in the Calder\\'{o}n-Zygmund algebra of all operators of the type \u03bb I+S, where S is a smooth homogeneous Calder\\'{o}n-Zygmund operator and \u03bb a real number. Moreover the polynomial P(x) must divide, in the algebra of polynomials, all spherical harmonics appearing in the spherical harmonics expansion of the kernel of T. Thus the condition is purely algebraic and very simple to check in practice. One first shows that the L^2 control of T^\u2217(f) by T(f) implies the structure condition for T. Then that this condition implies Super Cotlar's inequality. Therefore Super Cotlar's inequality is equivalent to the L^2 control, a fact for which we do not have a direct proof. The proof of the main Theorem is somehow involved. In both the necessary and the sufficient conditions one has to first deal with polynomial operators (i.e., the kernel restricted to the unit sphere in given by a homogeneous polynomial). At this stage one works mainly with multipliers of operators and the new ideas required emerge rather naturally. In proving the necessary condition one resorts to a division process in which Hilbert's Nullstellensatz is used, although our polynomials are real. What saves us is that in our context the real polynomials involved have many more zeroes than one would expect a priori. Finally, to make the whole approach work smoothly one needs also to perform an intricate combinatorial work to compute explicitly certain constants which appear naturally along the proof. The sufficient condition follows from an elaborate argument part of which is performed in the Fourier Transform side. It is worth remarking that we use a lemma, which was already known to people working in regularity problems for the Euler equation, stating that the image of the characteristic function of a smoothly bounded domain under a smooth homogeneous even Calder\\'{o}n -Zygmund operator is a bounded function. In a second step we must face the problem of obtaining estimates independent on the degree of the polynomial generating the kernel, because we need to use a compactness argument to pass to the general case. One of the main ingredients here is an old lemma of Calder\\'{o}n and Zygmund concerning Bessel functions, which combines perfectly with our new ideas to complete the argument. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('31','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_31\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Let T be a homogeneous smooth Calder\u00f3n-Zygmund operator in Euclidean space and let T^\u2217 stand for the maximal singular integral, i. e., the supremum of the truncations of T. In this paper we consider the problem of controlling T^\u2217(f) by T(f). We are mostly interested in estimating the L2 norm of T^\u2217(f) by the L^2 norm of T(f). The problem arose when trying to obtain existence of principal values from the L^2 boundedness of the singular integral in a rather general context in which the underlying measure in much more general than Lebesgue measure (see the paper &quot;Convergence of singular integrals with general measures&quot;, by P.Mattila and J.Verdera). This in turn was motivated by a problem of David and Semmes, which asks whether rectifiability of the support of the underlying measure follows from L^2 boundedness for the Riesz kernels. In our problem the parity of the kernel plays an essential role and in this paper we deal only with even kernels. The odd case is, in some ways, easier and will be treated in a subsequent article. Our first result is that for even higher order Riesz transforms one has a pointwise estimate of T^\u2217(f) by a constant times M(T(f)), where M is the Hardy-Littlewood maximal function. This fails for odd kernels (indeed for the Hilbert Transform), as was shown by Mateu and Verdera (Math.Research Letters (2006)). Clearly the above pointwise estimate implies the L^2 estimate of T^\u2217(f) by T(f). Notice that our pointwise estimate improves substantially classical Cotlar's inequality, because the term M(f) is missing in the right hand side. We may then informally call it Super Cotlar's inequality. There are simple polynomial homogeneous Calder\u00f3n-Zygmund operators for which the L^2 control of T^\u2217(f) by T(f) is not possible. For example, for T=B+B^2, where B is the Beurling transform. Showing this requires some work involving multipliers. The question then arises of how one may characterize those T for which the above L^2 control is possible. The main result of the paper gives such a condition. The characterization is as follows: T must be of the form R composed with U, where R is a higher order Riesz transform associated with some harmonic polynomial P(x) and U is an invertible operator in the Calder\u00f3n-Zygmund algebra of all operators of the type \u03bb I+S, where S is a smooth homogeneous Calder\u00f3n-Zygmund operator and \u03bb a real number. Moreover the polynomial P(x) must divide, in the algebra of polynomials, all spherical harmonics appearing in the spherical harmonics expansion of the kernel of T. Thus the condition is purely algebraic and very simple to check in practice. One first shows that the L^2 control of T^\u2217(f) by T(f) implies the structure condition for T. Then that this condition implies Super Cotlar's inequality. Therefore Super Cotlar's inequality is equivalent to the L^2 control, a fact for which we do not have a direct proof. The proof of the main Theorem is somehow involved. In both the necessary and the sufficient conditions one has to first deal with polynomial operators (i.e., the kernel restricted to the unit sphere in given by a homogeneous polynomial). At this stage one works mainly with multipliers of operators and the new ideas required emerge rather naturally. In proving the necessary condition one resorts to a division process in which Hilbert's Nullstellensatz is used, although our polynomials are real. What saves us is that in our context the real polynomials involved have many more zeroes than one would expect a priori. Finally, to make the whole approach work smoothly one needs also to perform an intricate combinatorial work to compute explicitly certain constants which appear naturally along the proof. The sufficient condition follows from an elaborate argument part of which is performed in the Fourier Transform side. It is worth remarking that we use a lemma, which was already known to people working in regularity problems for the Euler equation, stating that the image of the characteristic function of a smoothly bounded domain under a smooth homogeneous even Calder\u00f3n -Zygmund operator is a bounded function. In a second step we must face the problem of obtaining estimates independent on the degree of the polynomial generating the kernel, because we need to use a compactness argument to pass to the general case. One of the main ingredients here is an old lemma of Calder\u00f3n and Zygmund concerning Bessel functions, which combines perfectly with our new ideas to complete the argument. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('31','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_31\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MaximalSingular_2010.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MaximalSingular_2[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MaximalSingular_2[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.4007\/annals.2011.174.3.2\" title=\"Follow DOI:https:\/\/doi.org\/10.4007\/annals.2011.174.3.2\" target=\"_blank\">doi:https:\/\/doi.org\/10.4007\/annals.2011.174.3.2<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('31','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Fulvio Ricci; Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('33','tp_links')\" style=\"cursor:pointer;\">Duality in spaces of finite linear combinations of atoms<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Transactions of the American Mathematical Society, <\/span><span class=\"tp_pub_additional_volume\">vol. 363, <\/span><span class=\"tp_pub_additional_number\">no. 2011, <\/span><span class=\"tp_pub_additional_pages\">pp. 1311-1323, <\/span><span class=\"tp_pub_additional_year\">2011<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_33\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('33','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_33\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('33','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_33\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('33','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_33\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Duality in spaces of finite linear combinations of atoms},<br \/>\r\nauthor = {Fulvio Ricci and Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Ricci-Verdera.pdf},<br \/>\r\nyear  = {2011},<br \/>\r\ndate = {2011-01-01},<br \/>\r\nurldate = {2011-01-01},<br \/>\r\njournal = {Transactions of the American Mathematical Society},<br \/>\r\nvolume = {363},<br \/>\r\nnumber = {2011},<br \/>\r\npages = {1311-1323},<br \/>\r\nabstract = {An operator which is uniformly bounded on (1,\u221e)\u2212atoms does not need to be bounded on H1. This has been recently proved by Bownik (2005), who even showed that there exists a bounded linear functional on the space F1 of finite linear combinations of (1,\u221e)\u2212atoms which does not extend to a linear bounded functional on H1. His elegant argument combines a well known result of Taibleson, Meyer and Weiss with an appropriate use of Hahn -Banach Theorem. Therefore the dual of F1 is strictly larger than BMO. In this paper we determine the dual of F1. Let Fp be the space of finite linear combinations of (p,\u221e)\u2212atoms. A surprising byproduct of our approach is that for p strictly between 0 and 1 Fp and Hp have the same dual. As a consequence, if an operator T maps continuously Fp into some Banach space B, with p strictly between 0 and 1, then T extends to a bounded operator from Hp into B. In other words, for p strictly between 0 and 1, it is true that uniform boundedness on (p,\u221e)\u2212atoms implies boundedness on Hp. We work in the Euclidean space and no attempt has been made to extend the results to more general settings. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('33','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_33\" style=\"display:none;\"><div class=\"tp_abstract_entry\">An operator which is uniformly bounded on (1,\u221e)\u2212atoms does not need to be bounded on H1. This has been recently proved by Bownik (2005), who even showed that there exists a bounded linear functional on the space F1 of finite linear combinations of (1,\u221e)\u2212atoms which does not extend to a linear bounded functional on H1. His elegant argument combines a well known result of Taibleson, Meyer and Weiss with an appropriate use of Hahn -Banach Theorem. Therefore the dual of F1 is strictly larger than BMO. In this paper we determine the dual of F1. Let Fp be the space of finite linear combinations of (p,\u221e)\u2212atoms. A surprising byproduct of our approach is that for p strictly between 0 and 1 Fp and Hp have the same dual. As a consequence, if an operator T maps continuously Fp into some Banach space B, with p strictly between 0 and 1, then T extends to a bounded operator from Hp into B. In other words, for p strictly between 0 and 1, it is true that uniform boundedness on (p,\u221e)\u2212atoms implies boundedness on Hp. We work in the Euclidean space and no attempt has been made to extend the results to more general settings. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('33','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_33\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Ricci-Verdera.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Ricci-Verdera.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Ricci-Verdera.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('33','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2010\">2010<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Carlos P\u00e9rez, Joan Orobitg, Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('29','tp_links')\" style=\"cursor:pointer;\">New estimates for the maximal singular integral <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">International Mathematics Research Notices, <\/span><span class=\"tp_pub_additional_volume\">vol. 19, <\/span><span class=\"tp_pub_additional_pages\">pp. 3658\u20133722, <\/span><span class=\"tp_pub_additional_year\">2010<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_29\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('29','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_29\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('29','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_29\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('29','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_29\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {New estimates for the maximal singular integral },<br \/>\r\nauthor = {Joan Mateu, Carlos P\\'{e}rez, Joan Orobitg, Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/OddKernelsDef.pdf},<br \/>\r\nyear  = {2010},<br \/>\r\ndate = {2010-01-01},<br \/>\r\nurldate = {2010-01-01},<br \/>\r\njournal = {International Mathematics Research Notices},<br \/>\r\nvolume = {19},<br \/>\r\npages = {3658\\textendash3722},<br \/>\r\nabstract = {In this paper we pursue the study of the problem of controlling the maximal singular integral T\u2217f by the singular integral Tf. Here T is a smooth homogeneous Calder\\'{o}n-Zygmund singular integral of convolution type. We consider two forms of control, namely, in the L2(Rn) norm and via pointwise estimates of T\u2217f by M(Tf) or M2(Tf) , where M is the Hardy-Littlewood maximal operator and M2 its iteration. It is known that the parity of the kernel plays an essential role in this question. In a previous article we considered the case of even kernels and here we deal with the odd case. Along the way, the question of estimating composition operators of the type T\u2217 composed with T arises. It turns out that, again, there is a remarkable difference between even and odd kernels. For even kernels we obtain, quite unexpectedly, weak (1, 1) estimates, which are no longer true for odd kernels. For odd kernels we obtain sharp weaker inequalities involving a weak L1 estimate for functions in LLogL.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('29','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_29\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we pursue the study of the problem of controlling the maximal singular integral T\u2217f by the singular integral Tf. Here T is a smooth homogeneous Calder\u00f3n-Zygmund singular integral of convolution type. We consider two forms of control, namely, in the L2(Rn) norm and via pointwise estimates of T\u2217f by M(Tf) or M2(Tf) , where M is the Hardy-Littlewood maximal operator and M2 its iteration. It is known that the parity of the kernel plays an essential role in this question. In a previous article we considered the case of even kernels and here we deal with the odd case. Along the way, the question of estimating composition operators of the type T\u2217 composed with T arises. It turns out that, again, there is a remarkable difference between even and odd kernels. For even kernels we obtain, quite unexpectedly, weak (1, 1) estimates, which are no longer true for odd kernels. For odd kernels we obtain sharp weaker inequalities involving a weak L1 estimate for functions in LLogL.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('29','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_29\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/OddKernelsDef.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/OddKernelsDef.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/OddKernelsDef.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('29','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2009\">2009<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\"> Pertti Mattila; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('27','tp_links')\" style=\"cursor:pointer;\">Convergence of singular integrals with general measures<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Journal of the European Mathematical Society, <\/span><span class=\"tp_pub_additional_volume\">vol. 11, <\/span><span class=\"tp_pub_additional_number\">no. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 257-272, <\/span><span class=\"tp_pub_additional_year\">2009<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_27\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('27','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_27\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('27','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_27\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('27','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_27\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Convergence of singular integrals with general measures},<br \/>\r\nauthor = { Pertti Mattila and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Mattil_Verdera_JEMS.pdf},<br \/>\r\nyear  = {2009},<br \/>\r\ndate = {2009-01-01},<br \/>\r\nurldate = {2009-01-01},<br \/>\r\njournal = {Journal of the European Mathematical Society},<br \/>\r\nvolume = {11},<br \/>\r\nnumber = {2},<br \/>\r\npages = {257-272},<br \/>\r\nabstract = {In this paper we study singular integrals in fairly general metric spaces endowed with a measure which is not necessarily doubling. Our main goal in to show that under favorable circumstances L2 boundedness of the singular integral operator yields almost everywhere existence of principal values. The motivation comes from a longstanding open problem of David and Semmes, on the rectifiability of the support of Ahlfors regular measures (on subsets of the Euclidean space) for which the Riesz transforms are L2 bounded. One may have L2 boundedness of the operator associated with fairly good antisymmetric kernels (not the Riesz kernels !) and nowhere existence of principal values. However we show that for general antisymmetric kernels L2 boundedness of the corresponding operator implies a kind of average convergence almost everywhere. For measures with zero density we prove that this yields almost everywhere existence of principal values. The result on average convergence may also be obtained from the martingale convergence Theorem from a special martingale associated to the the antisymmetric operator.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('27','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_27\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we study singular integrals in fairly general metric spaces endowed with a measure which is not necessarily doubling. Our main goal in to show that under favorable circumstances L2 boundedness of the singular integral operator yields almost everywhere existence of principal values. The motivation comes from a longstanding open problem of David and Semmes, on the rectifiability of the support of Ahlfors regular measures (on subsets of the Euclidean space) for which the Riesz transforms are L2 bounded. One may have L2 boundedness of the operator associated with fairly good antisymmetric kernels (not the Riesz kernels !) and nowhere existence of principal values. However we show that for general antisymmetric kernels L2 boundedness of the corresponding operator implies a kind of average convergence almost everywhere. For measures with zero density we prove that this yields almost everywhere existence of principal values. The result on average convergence may also be obtained from the martingale convergence Theorem from a special martingale associated to the the antisymmetric operator.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('27','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_27\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Mattil_Verdera_JEMS.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Mattil_Verdera_JE[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Mattil_Verdera_JE[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('27','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">J. Mateu, J. Orobitg; J. Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('28','tp_links')\" style=\"cursor:pointer;\">Extra cancellation of even Calder\u00f3n-Zygmund operators and Quasiconformal mappings Authors<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Journal de Math\u00e9matiques Pures et Appliqu\u00e9s, <\/span><span class=\"tp_pub_additional_volume\">vol. 91, <\/span><span class=\"tp_pub_additional_issue\">iss. 9, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 402-431, <\/span><span class=\"tp_pub_additional_year\">2009<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_28\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('28','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_28\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('28','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_28\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('28','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_28\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Extra cancellation of even Calder\\'{o}n-Zygmund operators and Quasiconformal mappings Authors},<br \/>\r\nauthor = {J. Mateu, J. Orobitg and J. Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MOV_2009_JMPA.pdf},<br \/>\r\nyear  = {2009},<br \/>\r\ndate = {2009-01-01},<br \/>\r\nurldate = {2009-01-01},<br \/>\r\njournal = {Journal de Math\\'{e}matiques Pures et Appliqu\\'{e}s},<br \/>\r\nvolume = {91},<br \/>\r\nnumber = {4},<br \/>\r\nissue = {9},<br \/>\r\npages = {402-431},<br \/>\r\nabstract = {In this paper we discuss Lipschitz regularity for the Beltrami equation. An old result of Morrey states that there is a solution \u03a6 of the Beltrami equation which is a homeomorphism of the plane. This homeomorphic solution is unique modulo simple normalizations. The standard proof shows immediately that \u03a6 belongs locally to W(1,p), for some p larger than 2, and thus \u03a6 satisfies a Holder condition of some positive order less than one. This extends to all quasiregular functions (i.e., solutions of the Beltarmi equation belonging locally to W(1,2)), via Stoilov's factorization theorem. This regularity result for the Beltrami equation may be understood as a precursor of the De Giorgi-Nash Theorem, since is not difficult to see that the real and imaginary parts of a quasiregular function satisfy a second order elliptic equation in divergence form with bounded mesurable coefficients. The question addressed in this paper in to find conditions on the Beltrami coefficient so that \u03a6 is Lipschitz . In fact, under our hypothesis \u03a6 turns out to be bilipischitz. The requirement on the Beltrami coefficient is that it must live in a domain with smooth boundary of class C1+\u03b5 and satisfy a Holder condition of order \u03b5 there. In fact, one may allow Beltrami coefficients supported on the closure of finitely many disjoint domains with boundary of class C1+\u03b5, which satisfy a Holder condition of order \u03b5 in each domain. In particular, the boundaries of the domains may touch, as in the case of two tangent discs, or even have a piece in common of positive length. The result depends on the special cancellation properties of even Calder\\'{o}n-Zygmund kernels, which yield mapping properties of the corresponding operators that fail in the odd case. We use the index theory for Fredholm operators for Banach spaces to study the invertibility of some operators. One also needs to show compactness of some natural operators on smoothtly bounded domains. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('28','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_28\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we discuss Lipschitz regularity for the Beltrami equation. An old result of Morrey states that there is a solution \u03a6 of the Beltrami equation which is a homeomorphism of the plane. This homeomorphic solution is unique modulo simple normalizations. The standard proof shows immediately that \u03a6 belongs locally to W(1,p), for some p larger than 2, and thus \u03a6 satisfies a Holder condition of some positive order less than one. This extends to all quasiregular functions (i.e., solutions of the Beltarmi equation belonging locally to W(1,2)), via Stoilov's factorization theorem. This regularity result for the Beltrami equation may be understood as a precursor of the De Giorgi-Nash Theorem, since is not difficult to see that the real and imaginary parts of a quasiregular function satisfy a second order elliptic equation in divergence form with bounded mesurable coefficients. The question addressed in this paper in to find conditions on the Beltrami coefficient so that \u03a6 is Lipschitz . In fact, under our hypothesis \u03a6 turns out to be bilipischitz. The requirement on the Beltrami coefficient is that it must live in a domain with smooth boundary of class C1+\u03b5 and satisfy a Holder condition of order \u03b5 there. In fact, one may allow Beltrami coefficients supported on the closure of finitely many disjoint domains with boundary of class C1+\u03b5, which satisfy a Holder condition of order \u03b5 in each domain. In particular, the boundaries of the domains may touch, as in the case of two tangent discs, or even have a piece in common of positive length. The result depends on the special cancellation properties of even Calder\u00f3n-Zygmund kernels, which yield mapping properties of the corresponding operators that fail in the odd case. We use the index theory for Fredholm operators for Banach spaces to study the invertibility of some operators. One also needs to show compactness of some natural operators on smoothtly bounded domains. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('28','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_28\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MOV_2009_JMPA.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MOV_2009_JMPA.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/MOV_2009_JMPA.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('28','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2007\">2007<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('26','tp_links')\" style=\"cursor:pointer;\">Classical potential theory and analytic capacity<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">World Scientific, <\/span><span class=\"tp_pub_additional_volume\">vol. 2007, <\/span><span class=\"tp_pub_additional_pages\">pp. 174-192, <\/span><span class=\"tp_pub_additional_year\">2007<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_26\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('26','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_26\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('26','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_26\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('26','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_26\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Classical potential theory and analytic capacity},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Granada-Verdera.pdf},<br \/>\r\nyear  = {2007},<br \/>\r\ndate = {2007-01-01},<br \/>\r\nbooktitle = {Advanced Courses of Mathematical Analysis II},<br \/>\r\njournal = {World Scientific},<br \/>\r\nvolume = {2007},<br \/>\r\npages = {174-192},<br \/>\r\nabstract = {This paper is an article version of a plenary lecture that I delivered at the Seminar on Mathematical Analysis in Andalusia,\u201d held in Granada in the summer of 2004. In preparing the lecture I was first tempted to talk about the solution of the semi-additivity problem for analytic capacity, but I quickly realized that this would have necessarily brought the exposition into a jungle of technicalities with limited interest for the audience. Then I remembered that classical potential theory is a beautiful and powerful branch of analysis, which has been a permanent source of inspiration for many problems on analytic capacity. Therefore I planned the exposition so that it could serve as an introduction to classical potential theory for part of the audience and as an explanation of the difficulties connected with the study of analytic capacity for others. The present article follows this plan faithfully. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('26','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_26\" style=\"display:none;\"><div class=\"tp_abstract_entry\">This paper is an article version of a plenary lecture that I delivered at the Seminar on Mathematical Analysis in Andalusia,\u201d held in Granada in the summer of 2004. In preparing the lecture I was first tempted to talk about the solution of the semi-additivity problem for analytic capacity, but I quickly realized that this would have necessarily brought the exposition into a jungle of technicalities with limited interest for the audience. Then I remembered that classical potential theory is a beautiful and powerful branch of analysis, which has been a permanent source of inspiration for many problems on analytic capacity. Therefore I planned the exposition so that it could serve as an introduction to classical potential theory for part of the audience and as an explanation of the difficulties connected with the study of analytic capacity for others. The present article follows this plan faithfully. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('26','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_26\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Granada-Verdera.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Granada-Verdera.p[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Granada-Verdera.p[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('26','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2006\">2006<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('24','tp_links')\" style=\"cursor:pointer;\">Lp and weak L1 estimates for the maximal Riesz transform and the maximal Beurling transform<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Mathematical Research Letters, <\/span><span class=\"tp_pub_additional_volume\">vol. 13, <\/span><span class=\"tp_pub_additional_number\">no. 5-6, <\/span><span class=\"tp_pub_additional_year\">2006<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_resource_link\"><a id=\"tp_links_sh_24\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('24','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_24\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('24','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_24\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Lp and weak L1 estimates for the maximal Riesz transform and the maximal Beurling transform},<br \/>\r\nauthor = {Joan Mateu Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Riesz.pdf},<br \/>\r\nyear  = {2006},<br \/>\r\ndate = {2006-09-01},<br \/>\r\nurldate = {2006-09-01},<br \/>\r\njournal = {Mathematical Research Letters},<br \/>\r\nvolume = {13},<br \/>\r\nnumber = {5-6},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('24','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_24\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Riesz.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Riesz.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Maximal_Riesz.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('24','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\"> Xavier Tolsa, Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('25','tp_links')\" style=\"cursor:pointer;\">May the Cauchy transform of a non-trivial finite measure vanish on the support of the measure? <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Annales Academi\u00e6 Scientiarum Fennic\u00e6, <\/span><span class=\"tp_pub_additional_volume\">vol. 31, <\/span><span class=\"tp_pub_additional_pages\">pp. 479-494, <\/span><span class=\"tp_pub_additional_year\">2006<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_25\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('25','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_25\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('25','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_25\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('25','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_25\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {May the Cauchy transform of a non-trivial finite measure vanish on the support of the measure? },<br \/>\r\nauthor = { Xavier Tolsa, Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Paperambxt.pdf},<br \/>\r\nyear  = {2006},<br \/>\r\ndate = {2006-01-01},<br \/>\r\nurldate = {2006-01-01},<br \/>\r\njournal = {Annales Academi\\ae Scientiarum Fennic\\ae},<br \/>\r\nvolume = {31},<br \/>\r\npages = {479-494},<br \/>\r\nabstract = {Consider a finite complex Radon measure \u03bc in the plane whose Cauchy transform vanishes \u03bc-almost everywhere on the support of \u03bc. It looks like, excluding some trivial cases, \u03bc should be the zero measure. We show that this is the case if certain additional conditions hold. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('25','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_25\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Consider a finite complex Radon measure \u03bc in the plane whose Cauchy transform vanishes \u03bc-almost everywhere on the support of \u03bc. It looks like, excluding some trivial cases, \u03bc should be the zero measure. We show that this is the case if certain additional conditions hold. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('25','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_25\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Paperambxt.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Paperambxt.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Paperambxt.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('25','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2005\">2005<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu, Laura Prat; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('23','tp_links')\" style=\"cursor:pointer;\">The capacities associated to signed Riesz kernels and Wolff potentials<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Journal f\u00fcr die reine und angewandte Mathematik, <\/span><span class=\"tp_pub_additional_volume\">vol. 2005, <\/span><span class=\"tp_pub_additional_number\">no. 578, <\/span><span class=\"tp_pub_additional_pages\">pp. 201-223, <\/span><span class=\"tp_pub_additional_year\">2005<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_23\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('23','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_23\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('23','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_23\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('23','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_23\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The capacities associated to signed Riesz kernels and Wolff potentials},<br \/>\r\nauthor = {Joan Mateu, Laura Prat and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Wolffultim.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1515\/crll.2005.2005.578.201},<br \/>\r\nyear  = {2005},<br \/>\r\ndate = {2005-07-01},<br \/>\r\nurldate = {2005-07-01},<br \/>\r\njournal = {Journal f\\\"{u}r die reine und angewandte Mathematik},<br \/>\r\nvolume = {2005},<br \/>\r\nnumber = {578},<br \/>\r\npages = {201-223},<br \/>\r\nabstract = {We show that, for 0\\&lt;\u03b1\\&lt;1, the capacity \u03b3\u03b1 associated with the signed vector valued Riesz kernel x\u2223\u2223x\u2223\u22231+\u03b1 in \u211dn is comparable to the Riesz capacity C23(n\u2212\u03b1),32 of non-linear potential theory. The result is surprising because the definition of \u03b3\u03b1 involves a kernel with many cancellations, while the Riesz capacities are related to positive kernels. One would have expected a situation similar to that arising for analytic capacity. Recall that the analytic capacity of a segment is positive. Instead all existing possible Riesz capacities of homogeneity 1 or larger vanish on a segment or, more generally, on sets of \u03c3 finite length. The reason which explains the different behavior of \u03b3\u03b1,0\\&lt;\u03b1\\&lt;1, is that its homogeneity (or dimension) is \u03b1 and thus non-integer for the range considered. In other words, there are no rectifiable sets in fractional dimensions. The proof uses special positivity properties of the Riesz kernels of the dimensions considered, which are very well known for the Cauchy kernel. This allows us to bring in Wolff's potentials and thus the capacities of non linear potential theory. The special relation of the indexes of the relevant non-linear capacity is intriguing. It is rather natural to conjecture that our main result holds for all non-integer indexes \u03b1 betweeen 0 and n. For \u03b1\\&gt;1 this should be a difficult result, because one looses the positivity properties of the corresponding Riesz kernel alluded to before. In the proof we use Tolsa's scheme for the proof that analytic capacity and its positive counterpart are comparable. There is a major difficulty, which consists in showing that convolution with the kernel localizes uniform estimates. By this we mean that if T is a distribution such that xx1+\u03b1\u2217T is bounded in \u211d\ud835\udd5f, then xx1+\u03b1\u2217\u03c6T is also bounded in \u211d\ud835\udd5f for each test function \u03c6 . For \u03b1=1 and n=2 this is a classical fact, easy to prove because the kernel is related to a first order differential operator, which is not the case for fractional \u03b1 . },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('23','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_23\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We show that, for 0&lt;\u03b1&lt;1, the capacity \u03b3\u03b1 associated with the signed vector valued Riesz kernel x\u2223\u2223x\u2223\u22231+\u03b1 in \u211dn is comparable to the Riesz capacity C23(n\u2212\u03b1),32 of non-linear potential theory. The result is surprising because the definition of \u03b3\u03b1 involves a kernel with many cancellations, while the Riesz capacities are related to positive kernels. One would have expected a situation similar to that arising for analytic capacity. Recall that the analytic capacity of a segment is positive. Instead all existing possible Riesz capacities of homogeneity 1 or larger vanish on a segment or, more generally, on sets of \u03c3 finite length. The reason which explains the different behavior of \u03b3\u03b1,0&lt;\u03b1&lt;1, is that its homogeneity (or dimension) is \u03b1 and thus non-integer for the range considered. In other words, there are no rectifiable sets in fractional dimensions. The proof uses special positivity properties of the Riesz kernels of the dimensions considered, which are very well known for the Cauchy kernel. This allows us to bring in Wolff's potentials and thus the capacities of non linear potential theory. The special relation of the indexes of the relevant non-linear capacity is intriguing. It is rather natural to conjecture that our main result holds for all non-integer indexes \u03b1 betweeen 0 and n. For \u03b1&gt;1 this should be a difficult result, because one looses the positivity properties of the corresponding Riesz kernel alluded to before. In the proof we use Tolsa's scheme for the proof that analytic capacity and its positive counterpart are comparable. There is a major difficulty, which consists in showing that convolution with the kernel localizes uniform estimates. By this we mean that if T is a distribution such that xx1+\u03b1\u2217T is bounded in \u211d\ud835\udd5f, then xx1+\u03b1\u2217\u03c6T is also bounded in \u211d\ud835\udd5f for each test function \u03c6 . For \u03b1=1 and n=2 this is a classical fact, easy to prove because the kernel is related to a first order differential operator, which is not the case for fractional \u03b1 . <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('23','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_23\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Wolffultim.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Wolffultim.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Wolffultim.pdf<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1515\/crll.2005.2005.578.201\" title=\"Follow DOI:https:\/\/doi.org\/10.1515\/crll.2005.2005.578.201\" target=\"_blank\">doi:https:\/\/doi.org\/10.1515\/crll.2005.2005.578.201<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('23','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2004\">2004<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('21','tp_links')\" style=\"cursor:pointer;\">Ensembles effa\u00e7ables, ensembles invisibles et le probl\u00e8me du voyageur du commerce, ou comment l\u2019analyse r\u00e9elle aide l\u2019analyse complexe<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Gazette des Math\u00e9maticiens, <\/span><span class=\"tp_pub_additional_volume\">vol. 101, <\/span><span class=\"tp_pub_additional_year\">2004<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_21\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('21','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_21\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('21','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_21\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('21','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_21\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Ensembles effa\\c{c}ables, ensembles invisibles et le probl\\`{e}me du voyageur du commerce, ou comment l\u2019analyse r\\'{e}elle aide l\u2019analyse complexe},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Gazetterevue.pdf},<br \/>\r\nyear  = {2004},<br \/>\r\ndate = {2004-07-01},<br \/>\r\njournal = {Gazette des Math\\'{e}maticiens},<br \/>\r\nvolume = {101},<br \/>\r\nabstract = {L\u2019objectif de cet article est d\u2019expliquer comment les m\\'{e}thodes d\u2019analyse r\\'{e}elle aident \\`{a} la r\\'{e}solution de probl\\`{e}mes d\u2019analyse complexe pos\\'{e}s il y a environ 35 ans. Les outils d\u2019analyse r\\'{e}elle utilis\\'{e}s dans la r\\'{e}solution de ces probl\\`{e}mes ont \\'{e}t\\'{e} developp\\'{e}s ind\\'{e}pendamment de l\u2019analyse complexe. Ce sont la th\\'{e}orie de Besicovitch des ensembles du plan de longueur finie, une version du probl\\`{e}me du voyageur de commerce et les int\\'{e}grales singuli\\`{e}res de Calder\\'{o}n-Zygmund. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('21','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_21\" style=\"display:none;\"><div class=\"tp_abstract_entry\">L\u2019objectif de cet article est d\u2019expliquer comment les m\u00e9thodes d\u2019analyse r\u00e9elle aident \u00e0 la r\u00e9solution de probl\u00e8mes d\u2019analyse complexe pos\u00e9s il y a environ 35 ans. Les outils d\u2019analyse r\u00e9elle utilis\u00e9s dans la r\u00e9solution de ces probl\u00e8mes ont \u00e9t\u00e9 developp\u00e9s ind\u00e9pendamment de l\u2019analyse complexe. Ce sont la th\u00e9orie de Besicovitch des ensembles du plan de longueur finie, une version du probl\u00e8me du voyageur de commerce et les int\u00e9grales singuli\u00e8res de Calder\u00f3n-Zygmund. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('21','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_21\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Gazetterevue.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Gazetterevue.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Gazetterevue.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('21','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_unpublished\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('22','tp_links')\" style=\"cursor:pointer;\">Dalfsen slides<\/a> <span class=\"tp_pub_type tp_  unpublished\">Unpublished<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_year\">2004<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_22\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('22','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_22\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('22','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_22\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('22','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_22\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@unpublished{nokey,<br \/>\r\ntitle = {Dalfsen slides},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Dalfsen.pdf},<br \/>\r\nyear  = {2004},<br \/>\r\ndate = {2004-05-01},<br \/>\r\nabstract = {These slides were prepared for a course I gave at the Fourth annual Meeting of the European Research Network \u201cAnalysis and Operstors\u201d Netherlands, May 2004. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {unpublished}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('22','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_22\" style=\"display:none;\"><div class=\"tp_abstract_entry\">These slides were prepared for a course I gave at the Fourth annual Meeting of the European Research Network \u201cAnalysis and Operstors\u201d Netherlands, May 2004. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('22','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_22\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Dalfsen.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Dalfsen.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Dalfsen.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('22','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2003\">2003<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('11','tp_links')\" style=\"cursor:pointer;\">Conjunts evitables, conjunts invisibles i el viatjant de comer\u00e7 o com l'an\u00e0lisi real ajuda l'an\u00e0lisi complexa<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Butllet\u00ed de la Societat Catalana de Matem\u00e0tiques, <\/span><span class=\"tp_pub_additional_volume\">vol. 18, <\/span><span class=\"tp_pub_additional_issue\">iss. 2, <\/span><span class=\"tp_pub_additional_year\">2003<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_11\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('11','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_11\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('11','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_11\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('11','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_11\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Conjunts evitables, conjunts invisibles i el viatjant de comer\\c{c} o com l'an\\`{a}lisi real ajuda l'an\\`{a}lisi complexa},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/SurveyButlleti.pdf},<br \/>\r\nyear  = {2003},<br \/>\r\ndate = {2003-01-03},<br \/>\r\nurldate = {2003-01-03},<br \/>\r\njournal = {Butllet\\'{i} de la Societat Catalana de Matem\\`{a}tiques},<br \/>\r\nvolume = {18},<br \/>\r\nissue = {2},<br \/>\r\nabstract = {Recentment s\u2019han demostrat diversos teoremes d\u2019an\\`{a}lisi complexa que resolen problemes que varen ser plantejats fa aproximadament trenta-cinc anys ([7], [8], [16] i [23]). La q\\\"{u}esti\\'{o} general, que \\'{e}s molt b\\`{a}sica, consisteix a entendre la natura dels conjunts que s\\'{o}n singularitats evitables per a les funcions anal\\'{i}tiques i fitades. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('11','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_11\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Recentment s\u2019han demostrat diversos teoremes d\u2019an\u00e0lisi complexa que resolen problemes que varen ser plantejats fa aproximadament trenta-cinc anys ([7], [8], [16] i [23]). La q\u00fcesti\u00f3 general, que \u00e9s molt b\u00e0sica, consisteix a entendre la natura dels conjunts que s\u00f3n singularitats evitables per a les funcions anal\u00edtiques i fitades. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('11','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_11\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/SurveyButlleti.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/SurveyButlleti.pd[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/SurveyButlleti.pd[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('11','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Mateu; Xavier Tolsa; Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('9','tp_links')\" style=\"cursor:pointer;\">On the semiadditivity of analytic capacity and planar Cantor sets<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Contemporary Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 320, <\/span><span class=\"tp_pub_additional_pages\">pp. 259-278, <\/span><span class=\"tp_pub_additional_year\">2003<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_9\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('9','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_9\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('9','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_9\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('9','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_9\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {On the semiadditivity of analytic capacity and planar Cantor sets},<br \/>\r\nauthor = {Joan Mateu and Xavier Tolsa and Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/mh123.pdf},<br \/>\r\nyear  = {2003},<br \/>\r\ndate = {2003-01-02},<br \/>\r\nurldate = {2003-01-02},<br \/>\r\njournal = {Contemporary Mathematics},<br \/>\r\nvolume = {320},<br \/>\r\npages = {259-278},<br \/>\r\nabstract = {It has been recently proved that analytic capacity, \u03b3, is semiadditive. This result is a consequence of the comparability between \u03b3 and \u03b3+, a version of \u03b3 originated by bounded Cauchy potentials of positive measures. In this paper we describe the main ideas involved in the proof of this result and we give a complete proof of it in the particular case of the N-th approximation of the corner quarters Cantor set. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('9','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_9\" style=\"display:none;\"><div class=\"tp_abstract_entry\">It has been recently proved that analytic capacity, \u03b3, is semiadditive. This result is a consequence of the comparability between \u03b3 and \u03b3+, a version of \u03b3 originated by bounded Cauchy potentials of positive measures. In this paper we describe the main ideas involved in the proof of this result and we give a complete proof of it in the particular case of the N-th approximation of the corner quarters Cantor set. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('9','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_9\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/mh123.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/mh123.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/mh123.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('9','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera; Xavier Tolsa; Joan Mateu<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('8','tp_links')\" style=\"cursor:pointer;\">The planar Cantor sets of zero analytic capacity and the local T(b) theorem<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Journal of the American Mathematical Society, <\/span><span class=\"tp_pub_additional_volume\">vol. 16, <\/span><span class=\"tp_pub_additional_pages\">pp. 19-28, <\/span><span class=\"tp_pub_additional_year\">2003<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_8\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('8','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_8\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('8','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_8\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('8','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_8\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The planar Cantor sets of zero analytic capacity and the local T(b) theorem},<br \/>\r\nauthor = {Joan Verdera and Xavier Tolsa and Joan Mateu},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/cantset12.pdf},<br \/>\r\nyear  = {2003},<br \/>\r\ndate = {2003-01-01},<br \/>\r\nurldate = {2003-01-01},<br \/>\r\njournal = {Journal of the American Mathematical Society},<br \/>\r\nvolume = {16},<br \/>\r\npages = {19-28},<br \/>\r\nabstract = {n this paper we obtain rather precise estimates for the analytic capacity of a big class of planar Cantors sets. In fact, we show that analytic capacity and positive analytic capacity are comparable for these sets. As a consequence, we characterize the Cantor sets that are removable by bounded analytic functions. The main tool for the proof is an appropriate version of the T(b)-Theorem. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('8','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_8\" style=\"display:none;\"><div class=\"tp_abstract_entry\">n this paper we obtain rather precise estimates for the analytic capacity of a big class of planar Cantors sets. In fact, we show that analytic capacity and positive analytic capacity are comparable for these sets. As a consequence, we characterize the Cantor sets that are removable by bounded analytic functions. The main tool for the proof is an appropriate version of the T(b)-Theorem. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('8','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_8\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/cantset12.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/cantset12.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/cantset12.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('8','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">John Garnett, Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('20','tp_links')\" style=\"cursor:pointer;\">Analytic capacity, bilipschitz mappings and Cantor sets<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Mathematical Research Letters 10 (2003), 515--522, <\/span><span class=\"tp_pub_additional_volume\">vol. 10, <\/span><span class=\"tp_pub_additional_number\">no. 4, <\/span><span class=\"tp_pub_additional_pages\">pp. 515-522, <\/span><span class=\"tp_pub_additional_year\">2003<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_20\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('20','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_20\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('20','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_20\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('20','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_20\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Analytic capacity, bilipschitz mappings and Cantor sets},<br \/>\r\nauthor = {John Garnett, Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ABC.pdf},<br \/>\r\ndoi = {https:\/\/dx.doi.org\/10.4310\/MRL.2003.v10.n4.a10},<br \/>\r\nyear  = {2003},<br \/>\r\ndate = {2003-01-01},<br \/>\r\nurldate = {2003-01-01},<br \/>\r\njournal = {Mathematical Research Letters 10 (2003), 515--522},<br \/>\r\nvolume = {10},<br \/>\r\nnumber = {4},<br \/>\r\npages = {515-522},<br \/>\r\nabstract = {We show that for planar Cantor sets analytic capacity is a bilipschitz invariant. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('20','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_20\" style=\"display:none;\"><div class=\"tp_abstract_entry\">We show that for planar Cantor sets analytic capacity is a bilipschitz invariant. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('20','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_20\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ABC.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ABC.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/ABC.pdf<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/dx.doi.org\/10.4310\/MRL.2003.v10.n4.a10\" title=\"Follow DOI:https:\/\/dx.doi.org\/10.4310\/MRL.2003.v10.n4.a10\" target=\"_blank\">doi:https:\/\/dx.doi.org\/10.4310\/MRL.2003.v10.n4.a10<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('20','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2002\">2002<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('10','tp_links')\" style=\"cursor:pointer;\">The fall of the doubling condition in Calder\u00f3n-Zygmund Theory<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Publicacions Matem\u00e0tiques, <\/span><span class=\"tp_pub_additional_pages\">pp. 275-292, <\/span><span class=\"tp_pub_additional_year\">2002<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_10\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('10','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_10\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('10','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_10\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('10','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_10\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {The fall of the doubling condition in Calder\\'{o}n-Zygmund Theory},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/Escorial00.pdf},<br \/>\r\nyear  = {2002},<br \/>\r\ndate = {2002-01-01},<br \/>\r\nurldate = {2002-01-01},<br \/>\r\njournal = {Publicacions Matem\\`{a}tiques},<br \/>\r\npages = {275-292},<br \/>\r\nabstract = {The most important results of standard Calder\\'{o}n-Zygmund Theory have recently been extended to very general non-homogeneous contexts. In this survey paper we describe these extensions and their striking applications to removability problems for bounded analytic functions. We also discuss some of the techniques that allow us to dispense with the doubling condition in dealing with singular integrals. Special attention is paid to the Cauchy Integral. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('10','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_10\" style=\"display:none;\"><div class=\"tp_abstract_entry\">The most important results of standard Calder\u00f3n-Zygmund Theory have recently been extended to very general non-homogeneous contexts. In this survey paper we describe these extensions and their striking applications to removability problems for bounded analytic functions. We also discuss some of the techniques that allow us to dispense with the doubling condition in dealing with singular integrals. Special attention is paid to the Cauchy Integral. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('10','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_10\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/Escorial00.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/Escorial00.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/Escorial00.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('10','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2001\">2001<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('7','tp_links')\" style=\"cursor:pointer;\">L^2 boundedness of the Cauchy Integral and Menger curvature<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Contemporary Mathematics, <\/span><span class=\"tp_pub_additional_volume\">vol. 277, <\/span><span class=\"tp_pub_additional_pages\">pp. 139-158, <\/span><span class=\"tp_pub_additional_year\">2001<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_7\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('7','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_7\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('7','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_7\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('7','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_7\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {L^2 boundedness of the Cauchy Integral and Menger curvature},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/paper4.pdf},<br \/>\r\nyear  = {2001},<br \/>\r\ndate = {2001-01-01},<br \/>\r\nurldate = {2001-01-01},<br \/>\r\njournal = {Contemporary Mathematics},<br \/>\r\nvolume = {277},<br \/>\r\npages = {139-158},<br \/>\r\nabstract = {In this paper we explain the relevance of Menger curvature in understanding the $L^2$ boundedness properties of the Cauchy Integral Operator. After introducing Menger curvature and describing its basic properties we proceed to prove the Coifman-McIntosh-Meyer Theorem on the Cauchy Integral on a Lipschitz graph. From this circle of ideas comes a new simple approach to the $L^2$ boundedness of the first Calder\\'{o}n commutator. We point out that the $L^2$ boundedness of the Cauchy Integral on a Lipschitz graph can be easily reduced to the boundedness of the first commutator. In the last section we describe the various steps in the solution of Vitushkin\u2019s conjecture on analytic capacity paying special attention to the role played by Menger curvature.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('7','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_7\" style=\"display:none;\"><div class=\"tp_abstract_entry\">In this paper we explain the relevance of Menger curvature in understanding the $L^2$ boundedness properties of the Cauchy Integral Operator. After introducing Menger curvature and describing its basic properties we proceed to prove the Coifman-McIntosh-Meyer Theorem on the Cauchy Integral on a Lipschitz graph. From this circle of ideas comes a new simple approach to the $L^2$ boundedness of the first Calder\u00f3n commutator. We point out that the $L^2$ boundedness of the Cauchy Integral on a Lipschitz graph can be easily reduced to the boundedness of the first commutator. In the last section we describe the various steps in the solution of Vitushkin\u2019s conjecture on analytic capacity paying special attention to the role played by Menger curvature.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('7','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_7\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/paper4.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/paper4.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/paper4.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('7','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_2000\">2000<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('1','tp_links')\" style=\"cursor:pointer;\">On the T(1)-Theorem for the Cauchy Integral<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Ark Mat, <\/span><span class=\"tp_pub_additional_volume\">vol. 38, <\/span><span class=\"tp_pub_additional_issue\">iss. 1, <\/span><span class=\"tp_pub_additional_pages\">pp. 183-199, <\/span><span class=\"tp_pub_additional_year\">2000<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_1\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('1','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_1\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('1','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_1\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('1','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_1\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {On the T(1)-Theorem for the Cauchy Integral},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/T1theorem.pdf},<br \/>\r\nyear  = {2000},<br \/>\r\ndate = {2000-03-01},<br \/>\r\nurldate = {2000-03-01},<br \/>\r\njournal = {Ark Mat},<br \/>\r\nvolume = {38},<br \/>\r\nissue = {1},<br \/>\r\npages = {183-199},<br \/>\r\nabstract = {The main goal of this paper is to present an alternative, real variable proof of the T(1)-Theorem for the Cauchy Integral. We then prove that the estimate from below of analytic capacity in terms of total Menger curvature is a direct consequence of the T(1)-Theorem. An example shows that the L\u221e\u2212BMO estimate for the Cauchy Integral does not follow from L2 boundedness when the underlying measure is not doubling.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('1','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_1\" style=\"display:none;\"><div class=\"tp_abstract_entry\">The main goal of this paper is to present an alternative, real variable proof of the T(1)-Theorem for the Cauchy Integral. We then prove that the estimate from below of analytic capacity in terms of total Menger curvature is a direct consequence of the T(1)-Theorem. An example shows that the L\u221e\u2212BMO estimate for the Cauchy Integral does not follow from L2 boundedness when the underlying measure is not doubling.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('1','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_1\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/T1theorem.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/T1theorem.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2023\/09\/T1theorem.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('1','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_1998\">1998<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\"> Joan Orobitg, Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('19','tp_links')\" style=\"cursor:pointer;\">Choquet Integrals, Hausdorff Content and the Hardy\u2013Littlewood Maximal Operator<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Bulletin of the London Mathematical Society, <\/span><span class=\"tp_pub_additional_volume\">vol. 30, <\/span><span class=\"tp_pub_additional_issue\">iss. 2, <\/span><span class=\"tp_pub_additional_pages\">pp. 145-150, <\/span><span class=\"tp_pub_additional_year\">1998<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_resource_link\"><a id=\"tp_links_sh_19\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('19','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_19\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('19','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_19\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Choquet Integrals, Hausdorff Content and the Hardy\\textendashLittlewood Maximal Operator},<br \/>\r\nauthor = { Joan Orobitg, Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper2.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1112\/S0024609397003688},<br \/>\r\nyear  = {1998},<br \/>\r\ndate = {1998-01-01},<br \/>\r\nurldate = {1998-01-01},<br \/>\r\njournal = {Bulletin of the London Mathematical Society},<br \/>\r\nvolume = {30},<br \/>\r\nissue = {2},<br \/>\r\npages = {145-150},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('19','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_19\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper2.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper2.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper2.pdf<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1112\/S0024609397003688\" title=\"Follow DOI:https:\/\/doi.org\/10.1112\/S0024609397003688\" target=\"_blank\">doi:https:\/\/doi.org\/10.1112\/S0024609397003688<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('19','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_1995\">1995<\/h3><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Mark Melnikov, Joan Verdera <\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('18','tp_links')\" style=\"cursor:pointer;\">A geometyric proof of the L2 Boundedness of the Cauchy Integral on Lipschitz graphs <\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">International Mathematics Research Notices, <\/span><span class=\"tp_pub_additional_volume\">vol. 7, <\/span><span class=\"tp_pub_additional_pages\">pp. 325-331, <\/span><span class=\"tp_pub_additional_year\">1995<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_18\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('18','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_18\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('18','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_18\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('18','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_18\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {A geometyric proof of the L2 Boundedness of the Cauchy Integral on Lipschitz graphs },<br \/>\r\nauthor = {Mark Melnikov, Joan Verdera },<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/A_Geometric-_Proof_IMRN1.pdf},<br \/>\r\nyear  = {1995},<br \/>\r\ndate = {1995-01-01},<br \/>\r\nurldate = {1995-01-01},<br \/>\r\njournal = {International Mathematics Research Notices},<br \/>\r\nvolume = {7},<br \/>\r\npages = {325-331},<br \/>\r\nabstract = {A new proof of the L2 boundedness of The Cauchy Integral operator on Lipschitz graphs is presented. After some arguments of a geometric flavor using Menger's notion of curvature, we end up using the Fourier Transform and Plancherel identity to conclude the proof. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('18','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_18\" style=\"display:none;\"><div class=\"tp_abstract_entry\">A new proof of the L2 boundedness of The Cauchy Integral operator on Lipschitz graphs is presented. After some arguments of a geometric flavor using Menger's notion of curvature, we end up using the Fourier Transform and Plancherel identity to conclude the proof. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('18','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_18\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/A_Geometric-_Proof_IMRN1.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/A_Geometric-_Proo[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/A_Geometric-_Proo[...]<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('18','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><h3 class=\"tp_h3\" id=\"tp_h3_1994\">1994<\/h3><div class=\"tp_publication tp_publication_unpublished\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('17','tp_links')\" style=\"cursor:pointer;\">A new elementary proof of L2 estimates for the Cauchy Integral on Lipschitz graphs<\/a> <span class=\"tp_pub_type tp_  unpublished\">Unpublished<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_year\">1994<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_17\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('17','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_17\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('17','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_17\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('17','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_17\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@unpublished{nokey,<br \/>\r\ntitle = {A new elementary proof of L2 estimates for the Cauchy Integral on Lipschitz graphs},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper1-1.pdf},<br \/>\r\nyear  = {1994},<br \/>\r\ndate = {1994-09-01},<br \/>\r\nurldate = {1994-09-01},<br \/>\r\nabstract = {Subtle simple positivity properties of the Cauchy kernel have been discovered recently by M. S. Melnikov. Given distinct 3 points in the plane, certain symmetrization of the Cauchy kernel involving only these 3 points turns out to be exactly the inverse of the square of the radius of the circle determined by the points. The following is a sketch of the author's short proof of the Coifman-McIntosh-Meyer Theorem on L2 boundedness of the Cauchy Integral on Lipschitz graphs.Take a Lipschitz graph in the plane and transform the Cauchy integral on the graph into an integral operator T on the line via the obvious parametrization of the graph. Given an interval I, the L2(I) norm of the Cauchy integral of the characteristic function of I may be expressed as the triple integral on I of the symmetrization of the Cauchy kernel plus an error term that may be estimated by a constant time the length of I . Using the geometric expression in terms of the radius and a Fourier transform computation one estimates the main term by constant times the length of I. The second step consists in showing that atoms are mapped into L1(R). By duality this implies that L\u221e(R) is mapped into BMO(R) and by interpolation that L2(R) is mapped into itself. In particular, one shows that the triple integral of the inverse of the square of the radius of the circle through 3 arbitrary points on an arc of a Lipschitz graph is finite. This may be understood as an L2 version of total curvature with respect to arc length measure. The same result holds for arcs of chord-arc curves. These are the first non-trivial examples of measures whose total curvature in the above sense is finite. },<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {unpublished}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('17','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_17\" style=\"display:none;\"><div class=\"tp_abstract_entry\">Subtle simple positivity properties of the Cauchy kernel have been discovered recently by M. S. Melnikov. Given distinct 3 points in the plane, certain symmetrization of the Cauchy kernel involving only these 3 points turns out to be exactly the inverse of the square of the radius of the circle determined by the points. The following is a sketch of the author's short proof of the Coifman-McIntosh-Meyer Theorem on L2 boundedness of the Cauchy Integral on Lipschitz graphs.Take a Lipschitz graph in the plane and transform the Cauchy integral on the graph into an integral operator T on the line via the obvious parametrization of the graph. Given an interval I, the L2(I) norm of the Cauchy integral of the characteristic function of I may be expressed as the triple integral on I of the symmetrization of the Cauchy kernel plus an error term that may be estimated by a constant time the length of I . Using the geometric expression in terms of the radius and a Fourier transform computation one estimates the main term by constant times the length of I. The second step consists in showing that atoms are mapped into L1(R). By duality this implies that L\u221e(R) is mapped into BMO(R) and by interpolation that L2(R) is mapped into itself. In particular, one shows that the triple integral of the inverse of the square of the radius of the circle through 3 arbitrary points on an arc of a Lipschitz graph is finite. This may be understood as an L2 version of total curvature with respect to arc length measure. The same result holds for arcs of chord-arc curves. These are the first non-trivial examples of measures whose total curvature in the above sense is finite. <\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('17','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_17\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper1-1.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper1-1.pdf\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/paper1-1.pdf<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('17','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><div class=\"tp_publication tp_publication_article\"><div class=\"tp_pub_info\"><p class=\"tp_pub_author\">Joan Verdera<\/p><p class=\"tp_pub_title\"><a class=\"tp_title_link\" onclick=\"teachpress_pub_showhide('16','tp_links')\" style=\"cursor:pointer;\">Removability, capacity and approximation<\/a> <span class=\"tp_pub_type tp_  article\">Journal Article<\/span> <\/p><p class=\"tp_pub_additional\"><span class=\"tp_pub_additional_in\">In: <\/span><span class=\"tp_pub_additional_journal\">Complex Potential Theory, Nato ASI series, vol 439. Springer, Dordrecht., <\/span><span class=\"tp_pub_additional_volume\">vol. 439, <\/span><span class=\"tp_pub_additional_pages\">pp. 419-473, <\/span><span class=\"tp_pub_additional_year\">1994<\/span>.<\/p><p class=\"tp_pub_menu\"><span class=\"tp_abstract_link\"><a id=\"tp_abstract_sh_16\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('16','tp_abstract')\" title=\"Show abstract\" style=\"cursor:pointer;\">Abstract<\/a><\/span> | <span class=\"tp_resource_link\"><a id=\"tp_links_sh_16\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('16','tp_links')\" title=\"Show links and resources\" style=\"cursor:pointer;\">Links<\/a><\/span> | <span class=\"tp_bibtex_link\"><a id=\"tp_bibtex_sh_16\" class=\"tp_show\" onclick=\"teachpress_pub_showhide('16','tp_bibtex')\" title=\"Show BibTeX entry\" style=\"cursor:pointer;\">BibTeX<\/a><\/span><\/p><div class=\"tp_bibtex\" id=\"tp_bibtex_16\" style=\"display:none;\"><div class=\"tp_bibtex_entry\"><pre>@article{nokey,<br \/>\r\ntitle = {Removability, capacity and approximation},<br \/>\r\nauthor = {Joan Verdera},<br \/>\r\nurl = {http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Removability_Capacity_Approximation.pdf},<br \/>\r\ndoi = {https:\/\/doi.org\/10.1007\/978-94-011-0934-5_10},<br \/>\r\nyear  = {1994},<br \/>\r\ndate = {1994-01-01},<br \/>\r\nurldate = {1994-01-01},<br \/>\r\njournal = {Complex Potential Theory, Nato ASI series, vol 439. Springer, Dordrecht.},<br \/>\r\nvolume = {439},<br \/>\r\npages = {419-473},<br \/>\r\nabstract = {This are the notes of a course I gave at Montreal in June 1993 on approximation by analytic and harmonic functions (and solutions of other differential operators) in different norms. The notions of removability and capacity are discussed and, in particular, a chapter is devoted to analytic capacity.},<br \/>\r\nkeywords = {},<br \/>\r\npubstate = {published},<br \/>\r\ntppubtype = {article}<br \/>\r\n}<br \/>\r\n<\/pre><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('16','tp_bibtex')\">Close<\/a><\/p><\/div><div class=\"tp_abstract\" id=\"tp_abstract_16\" style=\"display:none;\"><div class=\"tp_abstract_entry\">This are the notes of a course I gave at Montreal in June 1993 on approximation by analytic and harmonic functions (and solutions of other differential operators) in different norms. The notions of removability and capacity are discussed and, in particular, a chapter is devoted to analytic capacity.<\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('16','tp_abstract')\">Close<\/a><\/p><\/div><div class=\"tp_links\" id=\"tp_links_16\" style=\"display:none;\"><div class=\"tp_links_entry\"><ul class=\"tp_pub_list\"><li><i class=\"fas fa-file-pdf\"><\/i><a class=\"tp_pub_list\" href=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Removability_Capacity_Approximation.pdf\" title=\"http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Removability_Capa[...]\" target=\"_blank\">http:\/\/mat.uab.cat\/web\/jvm\/wp-content\/uploads\/sites\/35\/2024\/01\/Removability_Capa[...]<\/a><\/li><li><i class=\"ai ai-doi\"><\/i><a class=\"tp_pub_list\" href=\"https:\/\/dx.doi.org\/https:\/\/doi.org\/10.1007\/978-94-011-0934-5_10\" title=\"Follow DOI:https:\/\/doi.org\/10.1007\/978-94-011-0934-5_10\" target=\"_blank\">doi:https:\/\/doi.org\/10.1007\/978-94-011-0934-5_10<\/a><\/li><\/ul><\/div><p class=\"tp_close_menu\"><a class=\"tp_close\" onclick=\"teachpress_pub_showhide('16','tp_links')\">Close<\/a><\/p><\/div><\/div><\/div><\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":48,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-46","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/pages\/46","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/users\/48"}],"replies":[{"embeddable":true,"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/comments?post=46"}],"version-history":[{"count":4,"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/pages\/46\/revisions"}],"predecessor-version":[{"id":425,"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/pages\/46\/revisions\/425"}],"wp:attachment":[{"href":"https:\/\/mat.uab.cat\/web\/jvm\/wp-json\/wp\/v2\/media?parent=46"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}