2011-2012 FAWG Seminar

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The Fields Analysis Working Group Seminar takes place (usually) at the Fields Institute Room 210 on Thursdays at 12h10. The seminar is co-organized by J. Colliander, R.J. McCann, M. Muñoz.

The seminar also has a page at the Fields Institute.

Of related interest in Toronto (and sometimes cross-listed):

Archive: 2008-2009_FAWG_Seminar, 2007-2008_FAWG_Seminar, 2006-2007_FAWG_Seminar. 2008-2009 FAWG Seminar, 2009-2010_FAWG_Seminar, 2010-2011 FAWG Seminar.





Contents

April 12, Doering, 12:10-13:00 @Fields Institute Room 210

Charles Doering [1] (University of Michigan) Fields Analysis Working Group Thursday April 12 12:10-13:00 Fields Institute Room 210
Title: TBA
Abstract: Professor Doering will be giving a Fields Applied Math Colloquium during the usual FAWG timeslot. We hope the regular FAWG participants will be interested! Also, there will be an additional talk given at 2:10pm by Dr. Evelyn Lunasin.
[{{{arxiv}}} arXiv] 2012_4_12_Doering_Notes 2012_4_12






April 5, Liu, 12:10-13:00 @Fields Institute Room 210

Zhuomin Liu (University of Pittsburgh) Fields Analysis Working Group Thursday April 5 12:10-13:00 Fields Institute Room 210
Title: The Liouville Theorem on Conformal Mappings
Abstract: The celebrated Liouville Theorem from $1850$ states that in dimension $n\geq 3$, the only conformal maps are M\"obius transforms. Liouville's proof, as well as many subsequent proofs, required the mappings to be diffeomorphisms of class $C^3$. However, since $C^1$ regularity is sufficient to define conformal maps, one may inquire whether the Liouville theorem remains true under that, or even weaker conditions, e.g. Sobolev functions. The reduction from $C^3$ regularity turned out to be very difficult. It this talk we will discuss the development of the Liouville Theorem under weaker and weaker regularity assumptions, including results of Gerhing, Reshnetyak, Bojarski and Iwaniec, Iwaniec and Martin on $W_{\rm loc}^{1,n}$ conformal mappings. Furthermore, Iwanice and Martin proved that in even dimensions $n \geq 4$, $W_{\rm loc}^{1,n/2}$ conformal mappings are M\"{o}bious transforms and they conjectured that it should also be true in odd dimensions. We also discuss a proof of the Liouville Theorem $f\in W_{\rm loc}^{1,1}$ in dimension $n\geq 3$ under one additional assumption that the norm of the first order derivative $
[{{{arxiv}}} arXiv] 2012_4_5_Liu_Notes 2012_4_5





March 29, Colliander, 12:10-13:00 @Fields Institute Room 210

James Colliander http://www.math.toronto.edu/colliand (University of Toronto) Fields Analysis Working Group Thursday March 29 12:10-13:00 Fields Institute Room 210
Title: Big frequency cascades in the cubic nonlinear Schrödinger flow on the 2-torus
Abstract: Smooth solutions of the cubic nonlinear Schrödinger equation on the 2-torus which display a big frequency cascade were constructed in joint work with M. Keel, G. Staffilani, H. Takaoka and T. Tao. These solutions start off oscillating on long spatial scales. Over time, through nonlinear resonant interactions, these solutions begins to oscillate on smaller and smaller spatial scales exhibiting an arbitrary increment in high regularity Sobolev spaces. A strategy has recently been put forward by Z. Hani which aims to construct solutions with an infinite cascade. Recent work by M. Guardia and V. Kaloshin has quantified the speed of the transient cascade. This talk will describe these developments.
[{{{arxiv}}} arXiv] 2012_3_29_Colliander_Notes 2012_3_29






March 8, Shao, 12:10-13:00 @Fields Institute Room 210

Arick Shao (University of Toronto) Fields Analysis Working Group Thursday March 8 12:10-13:00 Fields Institute Room 210
Title: A Generalized Representation Formula for Covariant Tensor Wave Equations on Curved Spacetimes
Abstract: In the Minkowksi space ${\Bbb R}^{1+3}$, the solution to an inhomogeneous wave equation is given explicitly by Kirchhoff's Formula. In this talk, we aim to extend Kirchhoff's Formula into a local first-order representation formula for covariant tensorial wave equations on arbitrary curved $(1+3)$-dimensional Lorentzian spacetimes. This formula is a generalization of an analogous Kirchhoff-Sobolev parametrix derived by Klainerman and Rodnianski, both in terms of the types of equations that can be treated as well as the assumptions required. Furthermore, the formula can be directly generalized to certain abstract vector bundles on the spacetime.
[{{{arxiv}}} arXiv] 2012_3_8_Shao_Notes 2012_3_8






March 1, Kishimoto, 12:10-13:00 @Fields Institute Room 210

Nobu Kishimoto (Kyoto University) Fields Analysis Working Group Thursday March 1 12:10-13:00 Fields Institute Room 210
Title: Well-posedness and finite-time blowup for the Zakharov system on two-dimensional torus
Abstract: We consider the Zakharov system on two-dimensional torus. First, we show the local well-posedness of the Cauchy problem in the energy space by a standard iteration argument using the $X^{s,b}$ norms. Our result does not depend on the period of torus. Conservation laws and a sharp Gagliardo-Nirenberg inequality imply an a priori bound of solutions, which enables us to extend the local-in-time solution to a global one if its $L^2$ norm is less than that of the ground state solution of the cubic NLS on $R^2$. We then show that the $L^2$ norm of the ground state is actually the threshold for global solvability, namely, that there exists a finite-time blow-up solution to the Zakharov system on 2d torus with the $L^2$ norm greater than but arbitrarily close to that of the ground state. This is joint work with Masaya Maeda (Tohoku University, Japan).
[{{{arxiv}}} arXiv] 2012_3_1_Kishimoto_Notes 2012_3_1






January 05, Goldman, 12:10-13:00 @Fields Institute Room 210

Dorian Goldman [2] (New York University) Fields Analysis Working Group Thursday January 05 12:10-13:00 Fields Institute Room 210
Title: The Gamma-limit of the Ohta-Kawasaki energy. Derivation of the renormalized energy.
Abstract: We study the asymptotic behavior of the screened sharp interface Ohta-Kawasaki energy in dimension 2 using the framework of $\Gamma$-convergence. In that model, two phases appear, and they interact via a nonlocal Coulomb type energy. We focus on the regime where one of the phases has very small volume fraction, thus creating ``droplets" of that phase in a sea of the other phase. We consider perturbations to the critical volume fraction where droplets first appear, show the number of droplets increases monotonically with respect to the perturbation factor, and describe their arrangement in all regimes, whether their number is bounded or unbounded. When their number is unbounded, the most interesting case we compute the $\Gamma$-limit of the `zeroth' order energy and yield averaged information for almost minimizers, namely that the density of droplets should be uniform. We then go to the next order, and derive a next order $\Gamma$-limit energy, which is exactly the ``Coulombian renormalized energy $W$" introduced in the work of Sandier/Serfaty, and obtained there as a limiting interaction energy for vortices in Ginzburg-Landau. The derivation is based on their abstract scheme, that serves to obtain lower bounds for 2-scale energies and express them through some probabilities on patterns via the multiparameter ergodic theorem. Without thus appealing at all to the Euler-Lagrange equation, we establish here for all configurations which have ``almost minimal energy," the asymptotic roundness and radius of the droplets as done by Muratov, and the fact that they asymptotically shrink to points whose arrangement should minimize the renormalized energy $W$, in some averaged sense. This leads to expecting to see hexagonal lattices of droplets.
[{{{arxiv}}} arXiv] 2012_01_05_Goldman_Notes 2012_01_05






November 24, McCann, 12:10-13:00 @Fields Institute Room 210

Robert McCann [3] (University of Toronto) Fields Analysis Working Group Thursday November 24 12:10-13:00 Fields Institute Room 210
Title: Higher-order time asymptotics of fast diffusion in Euclidean space: a dynamical systems approach
Abstract: With Jochen Denzler (UT Knoxville) and Herbert Koch (Bonn), we quantify the speed of convergence and higher asymptotics of fast diffusion dynamics on Euclidean space to the Barenblatt (self similar) profile. The degeneracy in the parabolicity of the equation is cured by re-expressing the dynamics on a manifold with a cylindrical end, called the cigar. The nonlinear evolution semigroup becomes differentiable with respect to Hoelder initial data on the cigar. The linearization of the dynamics is given by Laplace-Beltrami operator plus a drift term (which can be suppressed by the introduction of appropriate weights into the function space norm), plus a finite-depth potential well with a universal profile. In the limiting case of the (linear) heat equation, the depth diverges, the number of eigenstates increases without bound, and the continuous spectrum recedes to infinity. We provide a detailed study of the linear and nonlinear problems in Hoelder spaces on the cigar, including a sharp boundedness estimate for the semigroup, and use this as a tool to obtain sharp convergence results toward the Barenblatt solution. In finer convergence results (after modding out symmetries of the problem), a subtle interplay between convergence rates and tail behavior is revealed. The difficulties involved in choosing the right functional analytic spaces in which to carry out the analysis can be interpreted as genuine features of the equation rather than mere annoying technicalities.
[{{{arxiv}}} arXiv] 2011_11_24_McCann_Notes 2011_11_24






November 17, Chugunova, 12:10-13:00 @Fields Institute Room 210

Marina Chugunova [4] (University of Toronto) Fields Analysis Working Group Thursday November 17 12:10-13:00 Fields Institute Room 210
Title: On uniqueness of the waiting-time type solution of the thin film equation
Abstract: By formal asymptotic methods we analyze persistence and loss of zeros in generalized weak solutions of the thin film equation. We use a new dissipated functional recently constructed by Laugesen to prove an auxiliary energy equality that leads to the proof of the uniqueness of the waiting-type thin film solution under some additional assumptions about the initial data and regularity. Joint work with John King and Roman Taranets.
[{{{arxiv}}} arXiv] 2011_11_17_Chugunova_Notes 2011_11_17






November 10, Pass, 12:10-13:00 @Fields Institute Room 210

Brendan Pass [5] (University of Alberta) Fields Analysis Working Group Thursday November 10 12:10-13:00 Fields Institute Room 210
Title: Optimal transportation with infinitely many marginals
Abstract: I will discuss work in progress on an optimal transportation problem with infinitely many prescribed marginals. After formulating the problem and stating the main result, I will show that this result can be interpreted as a type of rearrangement inequality for stochastic processes. I will then discuss some connections with parabolic PDE, derivative pricing in mathematical finance and phase space bounds in quantum physics.
[{{{arxiv}}} arXiv] 2011_11_10_Pass_Notes 2011_11_10






November 03, Seis, 12:10-13:00 @Fields Institute Room 210

Christian Seis (University of Toronto) Fields Analysis Working Group Thursday November 03 12:10-13:00 Fields Institute Room 210
Title: On the coarsening rates in demixing binary viscous liquids
Abstract: We consider the demixing process of a binary mixture of two liquids after a temperature quench. In viscous liquids, demixing is mediated by diffusion and convection. The typical particle size grows as a function of time t, a phenomenon called coarsening. Simple scaling arguments based on the assumption of statistical self-similarity of the domain morphology suggest the coarsening rates: from ? t^{1/3} for diffusion-mediated to ? t for flow-mediated coarsening. In joint works with Y. Brenier, F. Otto, and D. Slepcev, we derive the crossover of both scaling regimes in the sense of lower bounds on the energy, which scales, heuristically at least, as an inverse length. The mathematical model is a Cahn-Hilliard equation with an additional convection term. The velocity of the convecting fluid is determined by a Stokes equation. Our analysis follows closely a method proposed by R. V. Kohn and F. Otto, which is based on the gradient flow structure of the evolution.
[{{{arxiv}}} arXiv] 2011_11_03_Seis_Notes 2011_11_03






October 27, Alexakis, 12:10-13:00 @Fields Institute Room 210

Spyros Alexakis [6] (University of Toronto) Fields Analysis Working Group Thursday October 27 12:10-13:00 Fields Institute Room 210
Title: Loss of compactness and bubbling for complete minimal surfaces in hyperbolic space
Abstract: We consider the Willmore energy on the space of complete minimal surfaces in $H^3$ and study the possible loss of compactness in the space of such surfaces with energy bounded above. This question has been extensively studied for various energy functionals for closed manifolds. The first such study was that of Sacks and Uhlenbeck for harmonic maps. The key tools to study the loss of compactness in that case are epsilon-regularity and removability of singularities; the loss of compactness can then occur due to bubbling at a finite number of points where energy concentrates. We find the analogous results in our setting of complete surfaces. These are the first results in this direction for surfaces with a free boundary. Joint with R. Mazzeo.
[{{{arxiv}}} arXiv] 2011_10_27_Alexakis_Notes 2011_10_27






October 20, Moradifam, 12:10-13:00 @Fields Institute Room 210

Amir Moradifam [7] (University of Toronto) Fields Analysis Working Group Thursday October 20 12:10-13:00 Fields Institute Room 210
Title: Conductivity imaging from one interior measurement in the presence of perfectly conducting and insulating inclusions
Abstract: We consider the problem of recovering an isotropic conductivity outside some perfectly conducting or insulating inclusions from the interior measurement of the magnitude of one current density field $\mid J\mid $. We prove that the conductivity outside the inclusions, and the shape and position of the perfectly conducting and insulating inclusions are uniquely determined (except in an exceptional case) by the magnitude of the current generated by imposing a given boundary voltage. We have found an extension of the notion of admissibility to the case of possible presence of perfectly conducting and insulating inclusions. This makes it possible to extend the results on uniqueness of the minimizers of the least gradient problem $F(u)=\int_{\Omega} a \mid \nabla u\mid$ with $u \mid_{\partial \Omega}=f$ to cases where $u$ has flat regions (is constant on open sets). This is a joint work with Adrian Nachman and Alexandru Tamasam.
[{{{arxiv}}} arXiv] 2011_10_20_Moradifam_Notes 2011_10_20






October 13, Korman, 12:10-13:00 @Fields Institute Room 210

Jonathan Korman (University of Toronto) Fields Analysis Working Group Thursday October 13 12:10-13:00 Fields Institute Room 210
Title: Optimal transportation with capacity constraints
Abstract: The classical problem of optimal transportation can be formulated as a linear optimization problem on a convex domain: among all joint measures with fixed marginals find the optimal one, where optimality is measured against a cost function. Here we consider a variant of this problem by imposing a constraint on the joint measures: among all joint measures with fixed marginals and which are dominated by a given measure find the optimal one. We show uniqueness of the solution, and compute a surprising example.
[{{{arxiv}}} arXiv] 2011_10_13_Korman_Notes 2011_10_13





October 06, Kamalinejad, 12:10-13:00 @Fields Institute Room 210

Ehsan Kamalinejad (University of Toronto) Fields Analysis Working Group Thursday October 06 12:10-13:00 Fields Institute Room 210
Title: Gradient flow methods for thin-film and related higher order equations
Abstract: We will discuss recent results on a class of higher-order evolution equations that can be viewed as gradient flows on the space of probability measures with respect to the Wasserstein metric. The simplest of these equations is the thin-film equation $\partial_tu=\partial_x(u \partial_x^3u)$, which corresponds to the Dirichlet energy. We will consider questions of existence and uniqueness of these gradient flows. A key probem in the analysis is the lack of convexity of the relevant energy functionals. This is a joint work with Almut Burchard.
[{{{arxiv}}} arXiv] 2011_10_06_Kamalinejad_Notes 2011_10_06





September 29, Cotar, 12:10-13:00 @Fields Institute Room 210

Codina Cotar [8] (University of Toronto) Fields Analysis Working Group Thursday September 29 12:10-13:00 Fields Institute Room 210
Title: Density functional theory and optimal transportation with Coulomb cost
Abstract: We present here novel insight into exchange-correlation functionals in density functional theory, based on the viewpoint of optimal transport. We show that in the case of two electrons and in the semiclassical limit, the exact exchange-correlation functional reduces to a very interesting functional of novel form, which depends on an optimal transport map T associated with a given density . Since the above limit is strongly correlated, the limit functional yields insightinto electron correlations. We prove the existence and uniqueness of such an optimal map for any number of electrons and each , and determine the map explicitly in the case when is radially symmetric. This is joint work with Gero Friesecke and Claudia Klueppelberg.
arXiv 2011_09_29_Cotar_Notes 2011_09_29





September 22, Seis, 12:10-13:00 @Fields Institute Room 210

Christian Seis (University of Toronto) Fields Analysis Working Group Thursday September 22 12:10-13:00 Fields Institute Room 210
Title: Rayleigh--Bénard convection. A new bound on the Nusselt number
Abstract: This talk may be viewed as a follow-up to the UofT analysis seminar from Sept. 16, but also aspires to be self-contained!

We consider Rayleigh--B\'enard convection as modeled by the Boussinesq equations in the infinite-Prandtl-number limit. We are interested in the scaling of the average upward heat transport, the Nusselt number $Nu$, in terms of the non-dimensionalized temperature forcing, the Rayleigh number $Ra$. Experiments, asymptotics and heuristics suggest that $Nu \sim Ra^{1/3}$.

This work is mostly inspired by two earlier rigorous work on upper bounds of $Nu$ in terms of $Ra$: 1.) The work of Constantin and Doering establishing $Nu \sim Ra^{1/3}\ln^{2/3}Ra$ with help of a (logarithmically failing) maximal regularity estimate in $L^{\infty}$ on the level of the Stokes equation. 2.) The work of Doering, Reznikoff and Otto establishing $Nu \sim Ra^{1/3}\ln^{1/3}Ra$ with help of the background field method. We present a new bound on the Nusselt number: Etimates behind the background field method can be combined with the maximal regularity in $L^{\infty}$ to yield $Nu \sim Ra^{1/3}\ln^{1/3}\ln Ra$ --- an estimate that is only a double logarithm away from the supposed optimal scaling.

This is joint work with Felix Otto.

[{{{arxiv}}} arXiv] 2011_09_22_Seis_Notes 2011_09_22



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