I am currently a Juan de la Cierva researcher at the Department of Mathematics of the Universitat Autònoma de Barcelona. I work mainly on existence theory and asymptotic behavior of kinetic equations, especially for coagulation and fragmentation models.
My office is -164 at the C1 tower of the Faculty of Science at the campus of Bellaterra. Notice that's minus 164 (floor -1; luckily not floor -164).
The address is:
Departament de Matemàtiques
Facultat de Ciències
Universitat Autònoma de Barcelona
08193 Bellaterra (Barcelona)
Spain
Tel. +34 93 581 31 04
Fax +34 93 581 27 90
Email: canizo@mat.uab.cat
We show in this work that gelation does not occur for a class of discrete coagulation-fragmentation models with size-dependent diffusion. We do not assume here that the diffusion rates of clusters are bounded below. The proof uses a duality argument first devised for reaction-diffusion systems with a finite number of equations due to M. Pierre.
We present existence, uniqueness and continuous dependence results for some kinetic equations motivated by models for the collective behavior of large groups of individuals. Models of this kind have been recently proposed to study the behavior of large groups of animals, such as flocks of birds, swarms, or schools of fish. Our aim is to give a well-posedness theory for general models which possibly include a variety of effects: an interaction through a potential, such as a short-range repulsion and long-range attraction; a velocity-averaging effect where individuals try to adapt their own velocity to that of other individuals in their surroundings; and self-propulsion effects, which take into account effects on one individual that are independent of the others. We develop our theory in a space of measures, using mass transportation distances. As consequences of our theory we show also the convergence of particle systems to their corresponding kinetic equations, and the local-in-time convergence to the hydrodynamic limit for one of the models.
We present a new a-priori estimate for discrete
coagulation-fragmentation systems with size-dependent diffusion
within a bounded, regular domain confined by homogeneous Neumann
boundary conditions. Following from a duality argument, this
a-priori estimate provides a global L2 bound
on the mass density and was previously used, for instance, in the
context of reaction-diffusion equations.
In this paper we demonstrate two lines of applications for
such an estimate: On the one hand, it enables to simplify parts of
the known existence theory and allows to show existence of
solutions for generalised models involving collision-induced,
quadratic fragmentation terms for which the previous existence
theory seems difficult to apply. On the other hand and most
prominently, it proves mass conservation (and thus the absence of
gelation) for almost all the coagulation coefficients for which
mass conservation is known to hold true in the space homogeneous
case.
We show that solutions to Smoluchowski's equation with a constant coagulation kernel and an initial datum with some regularity and exponentially decaying tail converge exponentially fast to a self-similar profile. This convergence holds in a weighted Sobolev norm which implies the L2 convergence of derivatives up to a certain order k depending on the regularity of the initial condition. We prove these results through the study of the linearized coagulation equation in self-similar variables, for which we show a spectral gap in a scale of weighted Sobolev spaces. We also take advantage of the fact that the Laplace or Fourier transforms of this equation can be explicitly solved in this case.
We consider Smoluchowski's equation with a homogeneous kernel of the form a(x,y) = xα yβ + yα xβ, with -1 < α ≤ β < 1, and -1 < α + β < 1. We first show that self-similar solutions of this equation are infinitely differentiable and prove sharp results on the behavior of self-similar profiles at y = 0 in the case α < 0. We also give some partial uniqueness results for self-similar profiles: in the case α = 0 we prove that two profiles with the same mass and moment of order α+β are necessarily equal, while in the case α < 0 we prove that two profiles with the same moments of order α and β, and which are asymptotic at y=0, are equal. Our methods include a new representation of the coagulation operator, and estimates of its regularity using derivatives of fractional order.
Under the condition of detailed balance and some additional restrictions on the size of the coefficients, we identify the equilibrium distribution to which solutions of the discrete coagulation-fragmentation system of equations converge for large times, thus showing that there is a critical mass which marks a change in the behavior of the solutions. This was previously known only for particular cases as the generalized Becker-Döring equations. Our proof is based on an inequality between the entropy and the entropy production which also gives some information on the rate of convergence to equilibrium for solutions under the critical mass.
We prove the following asymptotic behavior for solutions to the generalized Becker-Döring system for general initial data: under a detailed balance assumption and in situations where density is conserved in time, there is a critical density ρs such that solutions with an initial density ρ0 ≤ ρs converge strongly to the equilibrium with density ρ0, and solutions with initial density ρ0 > ρs converge (in a weak sense) to the equilibrium with density ρs. This extends the previous knowledge that this behavior happens under more restrictive conditions on the initial data. The main tool is a new estimate on the tail of solutions with density below the critical density.
A global existence, uniqueness and regularity theorem is proved for the simplest Markovian Wigner–Poisson–Fokker–Planck model incorporating friction and dissipation mechanisms. The proof relies on Green function and energy estimates under mild formulation, making essential use of the Husimi function and the elliptic regularization of the Fokker–Planck operator.
Micellization is the precipitation of lipids from aqueous solution into aggregates with a broad distribution of aggregation number. Three eras of micellization are characterized in a simple kinetic model of Becker-Döring type. The model asigns the same constant energy to the (k-1) monomer-monomer bonds in a linear chain of k particles. The number of monomers decreases sharply and many clusters of small size are produced during the first era. During the second era, nucleii are increasing steadily in size until their distribution becomes a self-similar solution of the diffusion equation. Lastly, when the average size of the nucleii becomes comparable to its equilibrium value, a simple mean-field Fokker-Planck equation describes the final era until the equilibrium distribution is reached.
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