Organizing Committee
 Diego Cordoba
ICMAT  Erwan Faou
INRIA Rennes  Patrick Gerard
ParisSud University, Orsay  Pierre Germain
NYU  Courant Institute  Alexandru Ionescu
Princeton University  Alex Kiselev
Duke University  Andrea Nahmod
University of Massachusetts Amherst  Kenji Nakanishi
Research Institute for Mathematical Sciences, Kyoto University  Benoit Pausader
Brown University  Themistoklis Sapsis
MIT  Gigliola Staffilani
Massachusetts Institute of Technology
Abstract
Dispersive equations are ubiquitous in nature. They govern the motion of waves in plasmas, ferromagnets, and elastic bodies, the propagation of light in optical fibers and of water in canals. They are relevant from the ocean scale down to atom condensates. There has been much recent progress in different directions, in particular in the exploration of the phase space of solutions of semilinear equations, advances towards a soliton resolution conjecture, the study of asymptotic stability of physical systems, the theoretical and numerical study of weak turbulence and transfer of energy in systems out of equilibrium, the introduction of tools from probability and the recent incorporation of computer assisted proofs. This semester aims to bring together these new developments and to explore their possible interconnection.
Dispersive phenomena appear in physical situations, where some energy is conserved, and are naturally related to Hamiltonian systems. This semester proposes to explore this link further by bringing together experimentalists, scientists, computational scientists and mathematicians with a common interest in exploring the various aspects of dispersive equations, from their analysis to their applications, and developing tools to facilitate experimentation. One key focus will be on global approaches, either in the sense of analyzing the overall landscape of the phase space, or in the study of generic solutions (e.g. of properties “almost surely true” in an appropriate sense). Another key focus will be experimental, in the sense of developing and analyzing instructive toymodels, implementing numerical experiments, and in some cases, simply of looking at interesting special cases.
The main events will be centered around three workshops
 one workshop on numerics, modeling and experiments in wave phenomena
 one workshop on generic behavior of dispersive solutions and wave turbulence
 one workshop on Hamiltonian methods and asymptotic dynamics
Confirmed Speakers & Participants
Talks will be presented virtually or inperson as indicated in the schedule below.
 Speaker
 Poster Presenter
 Attendee
 Virtual Attendee

Siddhant Agrawal
University of Massachusetts AmherstSep 7Oct 15, 2021

Yvonne Alama Bronsard
Sorbonne UniversitéSep 18Nov 2, 2021

Patricia Alonso Ruiz
Texas A&M UniversityOct 1531, 2021; Nov 29Dec 11, 2021

Ioakeim Ampatzoglou
Courant Institute of Mathematical Sciences, New York UniversityOct 1822, 2021; Dec 610, 2021

Xinliang An
National University of SingaporeSep 8Dec 10, 2021

Gerard Awanou
University of Illinois, ChicagoSep 2024, 2021

Aidan Backus
Brown UniversitySep 9Dec 10, 2021

ByeongHo Bahn
University of Massachusetts AmherstSep 8Dec 10, 2021

Hajer Bahouri
Université ParisEst  CréteilSep 8Dec 10, 2021

Valeria Banica
Sorbonne UniversitéSep 1925, 2021; Nov 1526, 2021

Weizhu Bao
National University of SingaporeSep 8Dec 10, 2021; Sep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Marius Beceanu
University at Albany SUNYSep 13Dec 10, 2021

Jacob Bedrossian
University of MarylandOct 1822, 2021

Bekarys Bekmaganbetov
Brown UniversityDec 610, 2021

Massimiliano Berti
SISSAOct 14Dec 10, 2021

Roberta Bianchini
Italian National Research Council, CNROct 18Nov 5, 2021

Lydia Bieri
University of MichiganSep 8Dec 10, 2021

Piotr Bizon
Jagiellonian UniversityOct 1822, 2021; Dec 610, 2021

Bjoern Bringmann
Institute for Advanced StudyOct 17Dec 10, 2021

Nicolas Burq
University ParisSudOct 1822, 2021

Nicolas Camps
Université Paris SaclaySep 7Dec 10, 2021

Esteban Cardenas
University of Texas at AustinOct 1822, 2021

Amin Chabchoub
University of SydneySep 2024, 2021

Andreia Chapouto
UCLADec 610, 2021

Jehanzeb Chaudhary
University of New MexicoSep 7Dec 11, 2021

IHsun Chen
Brown UniversityDec 610, 2021

Xuantao Chen
Johns Hopkins UniversityDec 610, 2021

Gong Chen
Fields instituteSep 8Dec 8, 2021; Sep 2024, 2021; Oct 1822, 2021

Brian Choi
Southern Methodist UniversityDec 610, 2021

Charles Collot
CergyParis UniversitéOct 1822, 2021

Diego Cordoba
ICMATSep 8Dec 10, 2021

Stefan Czimek
Brown University (ICERM)Sep 8, 2021May 31, 2022

Magdalena Czubak
University of Colorado at BoulderSep 13Dec 10, 2021

Constantine Dafermos
Brown UniversityDec 710, 2021

Joel Dahne
Uppsala UniversitySep 8Dec 10, 2021

David Damanik
Rice UniversityDec 610, 2021

Pierre de Roubin
University of EdinburghDec 610, 2021

AnneSophie de Suzzoni
Ecole PolytechniqueOct 1822, 2021

Yu Deng
University of Southern CaliforniaSep 15Dec 15, 2021

Yu Deng
University of Southern CaliforniaOct 1822, 2021

Giuseppe Di Fazio
University of CataniaSep 9Dec 10, 2021

Benjamin Dodson
John Hopkins UniversityDec 610, 2021

Michele Dolce
Imperial College LondonSep 13Dec 10, 2021

Hongjie Dong
Brown UniversitySep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Emmanuel Dormy
ENSSep 2024, 2021; Nov 1225, 2021

Jinqiao Duan
Illinois Institute of TechnologySep 13Dec 10, 2021

Sergey Dyachenko
University at BuffaloSep 2024, 2021

Daniel Eceizabarrena
University of Massachusetts AmherstSep 8Dec 10, 2021

Debbie Eeltink
MITSep 2024, 2021

Chenjie Fan
Academy of Mathematics and Systems Science, CASSep 8Dec 10, 2021

Allen Fang
Sorbonne UniversityDec 610, 2021

Erwan Faou
INRIA RennesSep 19Dec 10, 2021

Anxo Fariña Biasi
Jagiellonian UniversitySep 2024, 2021; Oct 1Dec 10, 2021

Serena Federico
Ghent UniversityOct 16Nov 6, 2021

Patrick Flynn
BrownSep 8Dec 10, 2021

Luigi Forcella
HeriotWatt UniversityOct 1822, 2021; Dec 610, 2021

Gilles Francfort
Universite Paris 13Oct 47, 2021

Rupert Frank
LMU MunichDec 610, 2021

Irene Gamba
University of Texas at AustinSep 2024, 2021

Claudia García
Universitat de BarcelonaSep 8Dec 11, 2021

Eduardo GarciaJuarez
Universitat de BarcelonaSep 8Dec 11, 2021

Louise Gassot
Laboratoire de Mathématiques d'Orsay  Université ParisSaclaySep 1, 2021Mar 4, 2022

Patrick Gerard
ParisSud University, OrsaySep 15Nov 15, 2021

Pierre Germain
NYU  Courant InstituteSep 8Dec 10, 2021

Elena Giorgi
Columbia UniversityDec 610, 2021

Tainara Gobetti Borges
Brown UniversitySep 10Dec 10, 2021

Javier Gomez Serrano
Princeton UniversitySep 13Dec 10, 2021

Sigal Gottlieb
University of Massachusetts DartmouthSep 2024, 2021

Ricardo Grande Izquierdo
University of MichiganSep 8Dec 10, 2021

Benoît Grébert
University of NantesSep 8Dec 11, 2021

Sandrine Grellier
Université d'OrléansSep 13Dec 10, 2021

Marcel Guardia
Universitat Politècnica de CatalunyaOct 1822, 2021

Zihua Guo
Monash UniversityDec 610, 2021

Yan Guo
Brown UniversityDec 610, 2021

Zaher Hani
University of MichiganSep 18Dec 11, 2021

Amirali Hannani
CEREMADE, Université Paris Dauphine, PSLSep 8Dec 10, 2021; Sep 2024, 2021

Benjamin HarropGriffiths
University of California, Los AngelesOct 1822, 2021; Dec 610, 2021

Susanna Haziot
Brown University MathematicsSep 8Dec 10, 2021

Siming He
Duke UniversityOct 1822, 2021

Jiao He
Laboratoire de Mathématiques d'OrsayDec 610, 2021

Lili He
Johns Hopkins UniversityDec 610, 2021

Sebastian Herr
Bielefeld UniversityDec 610, 2021

Justin Holmer
Brown UniversitySep 15Dec 10, 2021

Slim IBRAHIM
University of VictoriaSep 8Dec 10, 2021

Alexandru Ionescu
Princeton UniversitySep 8Dec 17, 2021

Sameer Iyer
UC DavisDec 610, 2021

Olaniyi Iyiola
Clarkson UniversitySep 2024, 2021

Jonathan Jaquette
Boston UniversitySep 2024, 2021

Pranava Jayanti
University Of Maryland College ParkSep 2024, 2021; Oct 1822, 2021

Hao Jia
University of MinnesotaNov 14Dec 10, 2021

Istvan Kadar
University of CambridgeOct 1822, 2021

Adilbek Kairzhan
University of TorontoSep 8Dec 11, 2021

Thomas Kappeler
Universität ZürichSep 10Dec 10, 2021

George Karniadakis
Brown UniversitySep 2024, 2021

Dean Katsaros
UMass amherstSep 8Dec 10, 2021

Panayotis Kevrekidis
University of Massachusetts AmherstSep 8Dec 10, 2021

Alex Kiselev
Duke UniversitySep 8Dec 10, 2021

Friedrich Klaus
Karlsruhe Institute of TechnologyOct 1822, 2021; Dec 610, 2021

Haram Ko
Brown UniversitySep 10Dec 10, 2021

Herbert Koch
University of BonnSep 8Dec 10, 2021

Sudipta Kolay
ICERMSep 1, 2021May 31, 2022

Kristin Kurianski
California State University, FullertonSep 1925, 2021

Christophe Lacave
Universite Grenoble AlpesSep 2024, 2021; Nov 1525, 2021

Oussama Landoulsi
Florida International UniversityDec 610, 2021

Thierry Laurens
University of California, Los AngelesOct 1822, 2021; Dec 610, 2021

Gyu Eun Lee
University of EdinburghSep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Tristan Leger
Princeton UniversityOct 17Nov 13, 2021

Jichun Li
University of Nevada Las VegasSep 2024, 2021

Guopeng Li
University of EdinburghOct 1822, 2021; Dec 610, 2021

Yao Li
University of Massachusetts AmherstSep 8Dec 10, 2021

Felipe Linares
IMPAOct 1822, 2021; Dec 610, 2021

Hans Lindblad
John Hopkins UniversityDec 610, 2021

Kyle Liss
University of Maryland, College ParkSep 8Dec 15, 2021

Ruoyuan Liu
University of EdinburghOct 1822, 2021; Dec 610, 2021

Jonas Luhrmann
Texas A&M UniversityOct 1531, 2021; Nov 28Dec 11, 2021

Jani Lukkarinen
University of HelsinkiDec 610, 2021

Brad Marston
Brown UniversitySep 2024, 2021

Yvan Martel
École PolytechniqueDec 610, 2021

Jeremy Marzuola
University of North CarolinaSep 9Dec 10, 2021

Nader Masmoudi
Courant Institute of Mathematical Sciences at NYUSep 13Dec 10, 2021

Alberto Maspero
Scuola Internazionale Superiore di Studi Avanzati (SISSA)Oct 1822, 2021

Jonathan Mattingly
Duke UniversityOct 1822, 2021

Joseph Miller
University of Texas at AustinOct 17Dec 11, 2021

Peter Miller
University of MichiganDec 610, 2021

Jose Morales E.
UTSASep 2024, 2021

Adam Morgan
University of TorontoDec 610, 2021

Lin Mu
University of GeorgiaSep 8Dec 10, 2021

Jason Murphy
Missouri University of Science and TechnologySep 21Dec 10, 2021

Andrea Nahmod
University of Massachusetts AmherstSep 8Dec 10, 2021

Kenji Nakanishi
Research Institute for Mathematical Sciences, Kyoto UniversitySep 8Dec 10, 2021

Maria Ntekoume
Rice UniversityDec 610, 2021

Tadahiro Oh
The University of EdinburghDec 610, 2021

Miguel Onorato
Università di TorinoSep 2024, 2021

Ludivine Oruba
Sorbonne UniversiteSep 8Dec 10, 2021; Nov 1220, 2021

José Palacios
Institut Denis Poisson, Université de ToursSep 8Dec 10, 2021

Yulin Pan
University of Michigan, Ann ArborSep 2024, 2021; Oct 1822, 2021

Jaemin Park
Universitat de BarcelonaSep 8Dec 10, 2021

Benoit Pausader
Brown UniversitySep 8Dec 10, 2021

Nataša Pavlović
University of Texas at AustinOct 1822, 2021; Dec 610, 2021

Dmitry Pelinovsky
McMaster UniversityDec 610, 2021

Galina Perelman
LAMASep 8Dec 10, 2021

Thi Thao Phuong Hoang
Auburn UniversitySep 2024, 2021

Leonardo Pollini
Politecnico di TorinoDec 511, 2021

Samuel PunshonSmith
Institute for Advanced StudyOct 1822, 2021

Fabio Pusateri
University of TorontoSep 8Dec 10, 2021

Raaghav Ramani
University of California, DavisSep 2024, 2021

Oscar Riano
Florida International UniversitySep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Tristan Robert
Université de LorraineOct 1822, 2021; Dec 610, 2021

Igor Rodnianski
Princeton UniversityDec 610, 2021

Casey Rodriguez
University of North CarolinaDec 610, 2021

Matthew Rosenzweig
Massachusetts Institute of TechnologySep 8Dec 10, 2021

Svetlana Roudenko
Florida International UniversitySep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Frédéric Rousset
Département de Mathématiques d’OrsayOct 15Nov 15, 2021

Themistoklis Sapsis
MITSep 8Dec 10, 2021

Nancy Scherich
University of TorontoSep 1, 2021May 31, 2022

Wilhelm Schlag
Yale UniversityDec 610, 2021

Birgit Schoerkhuber
University of Innsbruck, AustriaDec 610, 2021

Katharina Schratz
HeriotWatt UniversitySep 2024, 2021

Diaraf Seck
University Cheikh Anta Diop of DakarSep 8Dec 10, 2021

Anastassiya Semenova
ICERM, Brown UniversitySep 1, 2021May 31, 2022

Chengyang Shao
Massachusetts Institute of TechnologySep 13Dec 10, 2021

Jalal Shatah
New York UniversityOct 1822, 2021

Jie Shen
Purdue UniversitySep 2024, 2021

Jia Shi
Princeton UniversityNov 2025, 2021

Yeonjong Shin
Brown UniversityDec 610, 2021

Gigliola Staffilani
Massachusetts Institute of TechnologySep 8Dec 10, 2021

Noah Stevenson
Princeton UniversityDec 610, 2021

Annalaura Stingo
University of California DavisSep 8Dec 10, 2021

Walter Strauss
Brown UniversitySep 8Dec 10, 2021

Catherine Sulem
University of TorontoSep 8Dec 10, 2021

Ruoci Sun
Karlsruhe Institute of TechnologyOct 1822, 2021; Dec 610, 2021

changzhen Sun
University of ParisSaclaySep 9Dec 10, 2021

Chenmin Sun
CY CergyParis UniversitéSep 8Dec 10, 2021

Mouhamadou Sy
Imperial College LondonOct 1822, 2021

Tomoyuki Tanaka
Nagoya UniversityOct 1822, 2021; Dec 610, 2021

Maja Taskovic
Emory UniversitySep 9Dec 10, 2021

Daniel Tataru
University of California, BerkeleyDec 610, 2021

Leonardo Tolomeo
Universität BonNov 23, 2021; Dec 610, 2021

MinhBinh Tran
Southern Methodist UniversityOct 1822, 2021; Dec 610, 2021

Nikolay Tzvetkov
University of CergyPontoiseSep 8Dec 10, 2021

Tim Van Hoose
Missouri University of Science and TechnologyOct 1723, 2021

Luis Vega
Basque Center for Applied Mathematics (BCAM)Sep 17Dec 10, 2021

Paolo Ventura
SISSAOct 1822, 2021; Dec 610, 2021

Mats Vermeeren
University of LeedsDec 610, 2021

Monica Visan
University of California, Los AngelesSep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Weinan Wang
University of ArizonaSep 8Dec 10, 2021

Xuecheng Wang
Tsinghua UniversitySep 8Dec 10, 2021

Yuzhao Wang
University of BirminghamDec 610, 2021

Hong Wang
Institute for Advanced Study (IAS)Dec 610, 2021

Li Wang
University of MinnesotaSep 2024, 2021

Billy Warner
University of Texas at AustinOct 1822, 2021

Klaus Widmayer
EPFL, SwitzerlandOct 12Nov 15, 2021

Jon Wilkening
University of California, BerkeleySep 2024, 2021

Bobby Wilson
University of WashingtonSep 8Dec 10, 2021

Xiaoxu Wu
Rutgers UniversityDec 610, 2021

Sijue Wu
University of MichiganDec 610, 2021

Lei Wu
Lehigh UniversityOct 1822, 2021

Zoe Wyatt
University of CambridgeDec 610, 2021

Zhuolun Yang
Brown UniversitySep 8Dec 10, 2021

Jiaqi Yang
ICERMSep 1, 2021May 31, 2022

Kai Yang
Florida International UniversitySep 2024, 2021

Yao Yao
Georgia TechSep 2024, 2021

Jia Yin
Lawrence Berkeley National LaboratoryDec 610, 2021

Xueying Yu
University of WashingtonSep 8Dec 10, 2021

Lei Yu
Tongji UniversitySep 2024, 2021; Oct 1822, 2021

Haitian Yue
University of Southern CaliforniaSep 14Dec 10, 2021

Zhiyuan Zhang
New York UniversitySep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Chenyu Zhang
Brown UniversitySep 2024, 2021

Junyan Zhang
Johns Hopkins UniversityDec 610, 2021

Guangqu Zheng
University of EdinburghOct 1822, 2021; Dec 610, 2021

SHIJUN ZHENG
Georgia Southern UniversitySep 2024, 2021; Oct 1822, 2021; Dec 610, 2021

Jiqiang Zheng
Institute of Applied Physics and Computational MathematicsDec 610, 2021

Hui Zhu
University of MichiganOct 1822, 2021

Younes Zine
University of EdinburghDec 610, 2021
Visit dates listed on the participant list may be tentative and subject to change without notice.
Semester Schedule
Wednesday, September 8, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, September 9, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTLocal wellposedness for dispersive equationsTutorial  11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Abstract
This is a short introduction to the classical techniques for dispersive equations. We will present various equations and some methods to obtain local and global wellposedness and study the asymptotics.

11:00 am  12:30 pm EDTErgodicity of Markov processes: theory and computationTutorial  11th Floor Lecture Hall
 Yao Li, University of Massachusetts Amherst
Abstract
In this short course, I’ll cover the ergodicity of Markov processes on measurable state spaces. Both theoretical results and computational methods are based on the coupling technique. The following topics will be covered. 1, Markov process, transition kernel, and coupling. 2, Renewal theory with focusing on simultaneous renewal time. 3, Lyapunov criterion for geometric/polynomial ergodicity. 4, How to construct a Lyapunov function? 5, Numerical estimation of geometric/polynomial ergodicity. 6, Numerical estimation of invariant probability measure (if time permits).

1:30  2:00 pm EDTICERM WelcomeWelcome  11th Floor Lecture Hall
 Brendan Hassett, ICERM/Brown University

2:00  3:00 pm EDTGrad Student/ PostDoc IntroductionsIntroductions  11th Floor Lecture Hall
 Yvonne Alama Bronsard, Sorbonne Université
 Nicolas Camps, Université Paris Saclay
 Patrick Flynn, Brown
 Louise Gassot, Laboratoire de Mathématiques d'Orsay  Université ParisSaclay
 Dean Katsaros, UMass amherst
 Sudipta Kolay, ICERM
 Kyle Liss, University of Maryland, College Park
 Jaemin Park, Universitat de Barcelona
 Nancy Scherich, University of Toronto

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, September 10, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTLocal wellposedness for dispersive equationsTutorial  11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Abstract
This is a short introduction to the classical techniques for dispersive equations. We will present various equations and some methods to obtain local and global wellposedness and study the asymptotics.

11:00 am  12:30 pm EDTErgodicity of Markov processes: theory and computationTutorial  11th Floor Lecture Hall
 Yao Li, University of Massachusetts Amherst
Abstract
In this short course, I’ll cover the ergodicity of Markov processes on measurable state spaces. Both theoretical results and computational methods are based on the coupling technique. The following topics will be covered. 1, Markov process, transition kernel, and coupling. 2, Renewal theory with focusing on simultaneous renewal time. 3, Lyapunov criterion for geometric/polynomial ergodicity. 4, How to construct a Lyapunov function? 5, Numerical estimation of geometric/polynomial ergodicity. 6, Numerical estimation of invariant probability measure (if time permits).

2:00  3:30 pm EDTGrad Student/ PostDoc IntroductionsIntroductions  11th Floor Lecture Hall
 Bjoern Bringmann, Institute for Advanced Study
 Stefan Czimek, Brown University (ICERM)
 Daniel Eceizabarrena, University of Massachusetts Amherst
 Eduardo GarciaJuarez, Universitat de Barcelona
 Claudia García, Universitat de Barcelona
 Susanna Haziot, Brown University Mathematics
 Anastassiya Semenova, ICERM, Brown University
 Annalaura Stingo, University of California Davis
 Jiaqi Yang, ICERM
 Xueying Yu, University of Washington
 Haitian Yue, University of Southern California

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, September 13, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTComputerassisted proofs in PDEsTutorial  11th Floor Lecture Hall
 Javier Gomez Serrano, Princeton University
Abstract
In this minicourse we will present some recent results concerning computerassisted proofs in partial differential equations, starting from the basics of interval arithmetics. Particular emphasis will be put on the techniques, as opposed to the results themselves. There will be focus both on theory (lectures) and implementation (tutorial by Joel Dahne).

11:00 am  12:30 pm EDTErgodicity of Markov processes: theory and computationTutorial  11th Floor Lecture Hall
 Yao Li, University of Massachusetts Amherst
Abstract
In this short course, I’ll cover the ergodicity of Markov processes on measurable state spaces. Both theoretical results and computational methods are based on the coupling technique. The following topics will be covered. 1, Markov process, transition kernel, and coupling. 2, Renewal theory with focusing on simultaneous renewal time. 3, Lyapunov criterion for geometric/polynomial ergodicity. 4, How to construct a Lyapunov function? 5, Numerical estimation of geometric/polynomial ergodicity. 6, Numerical estimation of invariant probability measure (if time permits).

3:00  4:30 pm EDTWelcoming ReceptionReception  Hemenway's patio
Tuesday, September 14, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTLocal wellposedness for dispersive equationsTutorial  11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Abstract
This is a short introduction to the classical techniques for dispersive equations. We will present various equations and some methods to obtain local and global wellposedness and study the asymptotics.

11:00 am  12:30 pm EDTComputerassisted proofs in PDEsTutorial  11th Floor Lecture Hall
 Javier Gomez Serrano, Princeton University
Abstract
In this minicourse we will present some recent results concerning computerassisted proofs in partial differential equations, starting from the basics of interval arithmetics. Particular emphasis will be put on the techniques, as opposed to the results themselves. There will be focus both on theory (lectures) and implementation (tutorial by Joel Dahne).

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, September 15, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTLocal wellposedness for dispersive equationsTutorial  11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Abstract
This is a short introduction to the classical techniques for dispersive equations. We will present various equations and some methods to obtain local and global wellposedness and study the asymptotics.

11:00 am  12:30 pm EDTComputerassisted proofs in PDEsTutorial  11th Floor Lecture Hall
 Javier Gomez Serrano, Princeton University
Abstract
In this minicourse we will present some recent results concerning computerassisted proofs in partial differential equations, starting from the basics of interval arithmetics. Particular emphasis will be put on the techniques, as opposed to the results themselves. There will be focus both on theory (lectures) and implementation (tutorial by Joel Dahne).

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space

3:15  4:15 pm EDTGrads/Postdocs Meet with ICERM Directorate11th Floor Lecture Hall
 Brendan Hassett, ICERM/Brown University
 Misha Kilmer, Tufts University
Thursday, September 16, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, September 17, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:30 am EDTLocal wellposedness for dispersive equationsTutorial  11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Abstract
This is a short introduction to the classical techniques for dispersive equations. We will present various equations and some methods to obtain local and global wellposedness and study the asymptotics.

11:00 am  12:30 pm EDTComputerassisted proofs in PDEsTutorial  11th Floor Lecture Hall
 Javier Gomez Serrano, Princeton University
Abstract
In this minicourse we will present some recent results concerning computerassisted proofs in partial differential equations, starting from the basics of interval arithmetics. Particular emphasis will be put on the techniques, as opposed to the results themselves. There will be focus both on theory (lectures) and implementation (tutorial by Joel Dahne).

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, September 20, 2021

9:50  10:00 am EDTWelcome11th Floor Lecture Hall
 Brendan Hassett, ICERM/Brown University

10:00  10:40 am EDTQuasilinear Diffusion of magnetized fast electrons in a mean field of quasiparticle waves packets11th Floor Lecture Hall
 Speaker
 Irene Gamba, University of Texas at Austin
 Session Chair
 Luis Vega, Basque Center for Applied Mathematics (BCAM)
Abstract
Quasilinear diffusion of magnetized fast electrons in momentum space results from stimulated emission and absorption of waves packets via waveparticle resonances. Such model consists in solving the dynamics of a system of classical kinetic diffusion processes described by the balance equations for electron probability density functions (electron pdf) coupled to the time dynamics waves (quasiparticles) in a quantum process of their resonant interaction. Such description results in a Mean Field model where diffusion coefficients are determined by the local spectral energy density of excited waves whose perturbations depend on flux averages of the electron pdf.
We will discuss the model and a mean field iteration scheme that simulates the dynamics of the space average model, where the energy spectrum of the excited wave time dynamics is calculated with a coefficient that depends on the electron pdf flux at a previous time step; while the time dynamics of the quasilinear model for the electron pdf is calculated by the spectral average of the quasiparticle wave under a classical resonant condition where the plasma wave frequencies couples the spectral energy to the momentum variable of the electron pdf. Recent numerical simulations will be presented showing a strong hot tail anisotropy formation and stabilization for the iteration in a 3 dimensional cylindrical model.
This is work in collaboration with Kun Huang, Michael Abdelmalik at UT Austin. 
10:55  11:15 am EDTCoffee Break11th Floor Collaborative Space

11:15 am  12:00 pm EDTModeling inviscid water waves11th Floor Lecture Hall
 Virtual Speaker
 Christophe Lacave, Universite Grenoble Alpes
 Session Chair
 Luis Vega, Basque Center for Applied Mathematics (BCAM)
Abstract
We consider numerical strategies to handle twodimensional water waves in a fully nonlinear regime. The freesurface is discretized via lagrangian tracers and the numerical strategy is constructed carefully to include desingularizations, but no artificial regularizations. We approach the formation of singularities in the wave breaking problem and also model solitary waves and the effect of an abruptly changing bottom. We present a rigorous analysis of the singular kernel operators involved in these methods.

12:15  1:15 pm EDTLunch/Free Time

1:15  1:55 pm EDTAnomalous conduction in one dimensional chains: a wave turbulence approach.11th Floor Lecture Hall
 Miguel Onorato, Università di Torino
Abstract
Heat conduction in 3D macroscopic solids is in general well described by the Fourier's law. However, low dimensional systems, like for example nanotubes, may be characterized by a conductivity that is sizedependent. This phenomena, known as anomalous conduction, has been widely studied in one dimensional chains like FPUT, mostly using deterministic simulations of the microscopic model. Here, I will present a mesoscopic approach based on the wave turbulence theory and give the evidence, through extensive numerical simulations and theoretical arguments, that the anomalous conduction is the result of the presence of long waves that rapidly propagate from one thermostat to the other without interacting with other modes. I will also show that the scaling of the conductivity with the length of the chain obtained from the mesoscopic approach is consistent with the one obtained from microscopic simulations.

2:10  2:50 pm EDTOn the asymptotic stability of shear flows and vortices11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
Abstract
I will talk about some recent work on the global linear and nonlinear asymptotic stability of two families of solutions of the 2D Euler equations: shear flows on bounded channels and vortices in the plane. This is joint work with Hao Jia.

3:00  4:30 pm EDTReceptionHemenway's Patio (weather permitting)
Tuesday, September 21, 2021

10:00  10:40 am EDTSmall scale formations in the incompressible porous media equation11th Floor Conference Room
 Virtual Speaker
 Yao Yao, Georgia Tech
Abstract
The incompressible porous media (IPM) equation describes the evolution of density transported by an incompressible velocity field given by Darcy’s law. Here the velocity field is related to the density via a singular integral operator, which is analogous to the 2D SQG equation. The question of global regularity vs finitetime blowup remains open for smooth initial data, although numerical evidence suggests that small scale formation can happen as time goes to infinity. In this talk, I will discuss rigorous examples of small scale formations in the IPM equation: we construct solutions to IPM that exhibit infiniteintime growth of Sobolev norms, provided that they remain globally smooth in time. As an application, this allows us to obtain nonlinear instability of certain stratified steady states of IPM. This is a joint work with Alexander Kiselev.

10:55  11:15 am EDTCoffee Break11th Floor Collaborative Space

11:15 am  12:00 pm EDTPINNs and DeepOnets for Wave Systems11th Floor Lecture Hall
 Virtual Speaker
 George Karniadakis, Brown University

12:15  1:45 pm EDTLunch/Free Time

1:45  2:25 pm EDTThe second boundary value problem for a discrete MongeAmpere equation11th Floor Conference Room
 Gerard Awanou, University of Illinois, Chicago
Abstract
In this work we propose a natural discretization of the second boundary condition for the MongeAmpere equation of geometric optics and optimal transport. It is the natural generalization of the popular OlikerPrussner method proposed in 1988. For the discretization of the differential operator, we use a discrete analogue of the subdifferential. Existence, unicity and stability of the solutions to the discrete problem are established. Convergence results to the continuous problem are given.

2:40  3:45 pm EDTLightning Talks11th Floor Lecture Hall

3:45  4:15 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, September 22, 2021

10:00  10:40 am EDTEfficient and accurate structure preserving schemes for complex nonlinear systems11th Floor Conference Room
 Jie Shen, Purdue University
Abstract
Many complex nonlinear systems have intrinsic structures such as energy dissipation or conservation, and/or positivity/maximum principle preserving. It is desirable, sometimes necessary, to preserve these structures in a numerical scheme. I will present some recent advances on using the scalar auxiliary variable (SAV) approach to develop highly efficient and accurate structure preserving schemes for a large class of complex nonlinear systems. These schemes can preserve energy dissipation/conservation as well as other global constraints and/or are positivity/bound preserving, only require solving decoupled linear equations with constant coefficients at each time step, and can achieve higherorder accuracy.

10:55  11:15 am EDTCoffee Break11th Floor Collaborative Space

11:15 am  12:00 pm EDTEnergy growth for the Schrödinger map and the binormal flow11th Floor Lecture Hall
 Valeria Banica, Sorbonne Université
Abstract
In this talk I shall present a result of blow up of a density energy associated to the Schrödinger map and the binormal flow, a classical model for the dynamics of vortex filaments in Euler equations. This is a joint work with Luis Vega.

12:15  1:45 pm EDTLunch/Free Time

1:45  2:25 pm EDTWater Waves with Background Flow over Obstacles and Topography11th Floor Lecture Hall
 Virtual Speaker
 Jon Wilkening, University of California, Berkeley
Abstract
We present two accurate and efficient algorithms for solving the incompressible, irrotational Euler equations with a free surface in two dimensions with background flow over a periodic, multiplyconnected fluid domain that includes stationary obstacles and variable bottom topography. One approach is formulated in terms of the surface velocity potential while the other evolves the vortex sheet strength. Both methods employ layer potentials in the form of periodized Cauchy integrals to compute the normal velocity of the free surface. We also propose a new algorithm to dynamically vary the spacing of gridpoints on the free surface to efficiently resolve regions of high curvature as they develop. We study singularity formation and capillary effects and compare our numerical results with lab experiments.

2:45  3:15 pm EDTCoffee Break11th Floor Collaborative Space

3:15  3:55 pm EDTTopological Origin of Certain Fluid and Plasma Waves11th Floor Lecture Hall
 Brad Marston, Brown University
Abstract
Symmetries and topology play central roles in our understanding of physical systems. Topology, for instance, explains the precise quantization of the Hall effect and the protection of surface states in topological insulators against scattering from disorder or bumps. However discrete symmetries and topology have so far played little role in thinking about the fluid dynamics of oceans and atmospheres. In this talk I show that, as a consequence of the rotation of the Earth that breaks time reversal symmetry, equatorially trapped Kelvin and Yanai waves emerge as topologically protected edge modes. The nontrivial structure of the bulk Poincare ́ waves encoded through the first Chern number of value 2 guarantees the existence of these waves. Thus the oceans and atmosphere of Earth naturally share basic physics with topological insulators. As equatorially trapped Kelvin waves in the Pacific ocean are an important component of El Niño Southern Oscillation and other climate oscillations, these new results demonstrate that topology plays a surprising role in Earth’s climate system. We also predict that waves of topological origin will arise in magnetized plasmas. A planned experiment at UCLA’s Basic Plasma Science Facility to look for the waves is described.
Thursday, September 23, 2021

10:00  10:40 am EDTResonances as a Computational Tool11th Floor Lecture Hall
 Katharina Schratz, HeriotWatt University

10:55  11:15 am EDTCoffee Break11th Floor Collaborative Space

11:15 am  12:00 pm EDTEfficient timestepping methods for the rotating shallow water equations11th Floor Lecture Hall
 Virtual Speaker
 Thi Thao Phuong Hoang, Auburn University
Abstract
Numerical modeling of geophysical flows is challenging due to the presence of various coupled processes that occur at different spatial and temporal scales. It is critical for the numerical schemes to capture such a wide range of scales in both space and time to produce accurate and robust simulations over long time horizons.
In this talk, we will discuss efficient timestepping methods for the rotating shallow water equations discretized on spatial meshes with variable resolutions. Two different approaches will be considered: the first approach is a fully explicit local timestepping algorithm based on the strong stability preserving RungeKutta schemes, which allows different time step sizes in different regions of the computational domain. The second approach, namely the localized exponential time differencing method, is based on spatial domain decomposition and exponential time integrators, which makes possible the use of much larger time step sizes compared to explicit schemes and avoids solving nonlinear systems. Numerical results on various test cases will be presented to demonstrate the performance of the proposed methods. 
12:15  1:45 pm EDTLunch/Free Time

1:45  2:25 pm EDTDynamics in particle suspension flow11th Floor Conference Room
 Li Wang, University of Minnesota
Abstract
In this talk, I will consider two set up of particle suspension flow. One is a gravity driven flow down an incline, and the other is a pressure driven flow in a HeleShaw cell. In the former case, the interesting phenomena is the formation of singular shock that appears in the high particle concentration case that relates to the particlerich ridge observed in the experiments. We analyze the formation of the singular shock as well as its local structure. In the latter case, we rationalize a selfsimilar accumulation of particles at the interface between suspension and air. Our results demonstrate that the combination of the shear induced migration, the advancing fluidfluid interface, and Taylor dispersion yield the selfsimilar and gradual accumulation of particles.

2:45  3:15 pm EDTCoffee Break11th Floor Collaborative Space

3:15  3:55 pm EDTSeparatrix crossing and symmetry breaking in NLSElike systems due to forcing and damping11th Floor Conference Room
 Debbie Eeltink, MIT
Abstract
The nonlinear Schrödinger equation (NLSE) is a workhorse for many different fields (e.g. optical fibers, BoseEinstein condensates, water waves). It describes the evolution of the envelope of a field in time or space, taking into account the nonlinear interaction of the components of the spectrum of the envelope. While the NLSE is wellstudied in its conservative form, a relevant question to ask is how does it respond to damping and forcing? Limiting the spectrum to only three components allows one to construct a phasespace for the NLSE, spanned by the relative phase of the sidebands, and the energy fraction in the sidebands. Using wavetank measurements, we show that forcing and damping the NLSE induces separatrix crossing: switching from one solutiontype to the other in the phasespace. Our experiments are performed on deep water waves, which are better described by the higherorder NLSE, the Dysthe equation. We, therefore, extend our threewave analysis to this system. However, our conclusions are general as the dynamics are driven by the leading order terms. To our knowledge, it is the first phase evolution extraction from waterwave measurements. Furthermore, we observe a growth and decay cycle for modulated plane waves that are conventionally considered stable. Finally, we give a theoretical demonstration that forcing the NLSE system can induce symmetry breaking during the evolution.
Friday, September 24, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space

10:00  10:40 am EDTExtreme Wave Events in Reflective Environments11th Floor Lecture Hall
 Amin Chabchoub, University of Sydney
Abstract
Waves dynamics in coastal zones is known to comprise incident and reflective wave motion. We report an experimental study in which several incident JONSWAP wave trains have been generated in a unidirectional water wave tank while the artificial beach inclination and its permeability have been varied to allow a variety of reflective wave conditions. Key statistical features obtained from an adaptive coupled nonlinear Schrödinger model simulations show an excellent agreement with the laboratory data collected near the beach.

10:55  11:15 am EDTCoffee Break11th Floor Collaborative Space

11:15  11:55 am EDTSymmetry in stationary and uniformly rotating solutions of the Euler equations11th Floor Lecture Hall
 Javier Gomez Serrano, Princeton University

12:10  12:50 pm EDTHigh order strong stability preserving multiderivative implicit and IMEX RungeKutta methods with asymptotic preserving properties11th Floor Lecture Hall
 Sigal Gottlieb, University of Massachusetts Dartmouth
Abstract
In this talk we present a class of high order unconditionally strong stability preserving (SSP) implicit twoderivative RungeKutta schemes, and SSP implicitexplicit (IMEX) multiderivative RungeKutta schemes where the timestep restriction is independent of the stiff term. The unconditional SSP property for a method of order $p>2$ is unique among SSP methods, and depends on a backwardintime assumption on the derivative of the operator. We show that this backward derivative condition is satisfied in many relevant cases where SSP IMEX schemes are desired. We devise unconditionally SSP implicit RungeKutta schemes of order up to $p=4$, and IMEX RungeKutta schemes of order up to $p=3$. For the multiderivative IMEX schemes, we also derive and present the order conditions, which have not appeared previously. The unconditional SSP condition ensures that these methods are positivity preserving, and we present sufficient conditions under which such methods are also asymptotic preserving when applied to a range of problems, including a hyperbolic relaxation system, the Broadwell model, and the BhatnagarGrossKrook (BGK) kinetic equation.
Monday, September 27, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Tuesday, September 28, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am EDTRIEMANN’S NONDIFFERENTIABLE FUNCTION AND THE BINORMAL CURVATURE FLOW (Joint work with Valeria Banica)11th Floor Lecture Hall
 Luis Vega, Basque Center for Applied Mathematics (BCAM)
Abstract
We make a connection between a famous analytical object introduced in the 1860s by Riemann, as well as some variants of it, and a nonlinear geometric PDE, the binormal curvature flow. As a consequence this analytical object has a nonobvious non linear geometric interpretation. We recall that the binormal flow is a standard model for the evolution of vortex filaments. We prove the existence of solutions of the binormal flow with smooth trajectories that are as close as desired to curves with a multifractal behavior. Finally, we show that this behavior falls within the multifractal formalism of Frisch and Parisi, which is conjectured to govern turbulent fluids.

11:30 am  12:30 pm EDTALMOSTGLOBAL WELLPOSEDNESS FOR 2D STRONGLYCOUPLED WAVEKLEINGORDON SYSTEMS11th Floor Lecture Hall
 Annalaura Stingo, University of California Davis
Abstract
(Joint with Mihaela Ifrim) In this talk we discuss the almostglobal wellposedness of a wide class of coupled WaveKleinGordon equations in 2+1 spacetime dimensions, when initial data are small and localized. The WaveKleinGordon systems arise from several physical models especially related to General Relativity but few results are known at present in lower spacetime dimensions. Compared with prior related results, we here consider a strong quadratic quasilinear coupling between the wave and the KleinGordon equation and no restriction is made on the support of the initial data which only have a mild decay at infinity and very limited regularity.

2:30  3:00 pm EDTCoffee Break11th Floor Collaborative Space

3:00  4:00 pm EDTSemilinear Dispersive Equations11th Floor Lecture Hall
 Alexandru Ionescu, Princeton University
 Benoit Pausader, Brown University
Wednesday, September 29, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:30 am  12:15 pm EDTGender Diversity and the Mathematical Community11th Floor Lecture Hall
 Andrea Nahmod, University of Massachusetts Amherst
 Gigliola Staffilani, Massachusetts Institute of Technology
Abstract
Followed by a “brownbag lunch” (provided by ICERM) to be taken outside, where the discussion is expected to continue among smaller groups. RSVP required.

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, September 30, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm EDTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall
 Daniel Eceizabarrena, University of Massachusetts Amherst
 Claudia García, Universitat de Barcelona
 Haitian Yue, University of Southern California

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, October 1, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, October 4, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Tuesday, October 5, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am EDTThe characteristic gluing problem of general relativity11th Floor Lecture Hall
 Stefan Czimek, Brown University (ICERM)
Abstract
In this talk we introduce and solve the characteristic gluing problem for the Einstein vacuum equations. We show that obstructions to characteristic gluing come from an infinitedimensional space of conservation laws along null hypersurfaces for the linearized equations at Minkowski. We prove that this space splits into an infinitedimensional space of gaugedependent charges and a 10dimensional space of gaugeinvariant charges. We identify the 10 gaugeinvariant charges to be related to the energy, linear momentum, angular momentum and centerofmass of the spacetime. Based on this identification, we explain how to characteristically glue a given spacetime to a suitably chosen Kerr spacetime. As corollary we get an alternative proof of the CorvinoSchoen spacelike gluing to Kerr. Moreover, we apply our characteristic gluing method to localise characteristic initial data along null hypersurfaces. In particular, this yields a new proof of the CarlottoSchoen spacelike localization where our method yields no loss of decay, thus resolving an open problem. We also outline further applications. This is joint work with S. Aretakis (Toronto) and I. Rodnianski (Princeton).

11:30 am  12:30 pm EDTThe role of hyperbolicity in deciding uniqueness for minimizers of an energy with linear growth11th Floor Lecture Hall
 Gilles Francfort, Universite Paris 13

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, October 6, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am EDTProfessional Development: Ethics IProfessional Development  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, October 7, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm EDTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

2:00  4:00 pm EDTProbabilistic wellposedness for nonlinear Schrödinger equation (I)11th Floor Lecture Hall
 Haitian Yue, University of Southern California
Abstract
In this minicourse, we will introduce the probabilistic wellposedness theory in the background of the nonlinear Schrödinger equation and in particular will focus on local (in time) dynamics with the random initial data. The following topics will be covered: 1) the basic settings of random data Cauchy theory; 2) Bourgain's recentering method; 3) the random averaging operator method.

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, October 8, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

1:30  3:00 pm EDTProbabilistic wellposedness for nonlinear Schrödinger equation (I)11th Floor Lecture Hall
 Haitian Yue, University of Southern California
Abstract
In this minicourse, we will introduce the probabilistic wellposedness theory in the background of the nonlinear Schrödinger equation and in particular will focus on local (in time) dynamics with the random initial data. The following topics will be covered: 1) the basic settings of random data Cauchy theory; 2) Bourgain's recentering method; 3) the random averaging operator method.

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Tuesday, October 12, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am EDTSuperharmonic Instability of Stokes Waves11th Floor Lecture Hall
 Anastassiya Semenova, ICERM, Brown University
Abstract
We consider the classical problem of water waves on the surface of an ideal fluid in 2D. This work offers an investigation of dynamics and stability of nonlinear waves. We provide new insight into the stability of the Stokes waves by identifying previously inaccessible branches of instability in the equations of motion for fluid. The eigenvalues of the linearized problem that become unstable follow a selfsimilar law as they approach instability threshold, and a power law is suggested for unstable eigenvalues in the immediate vicinity of the limiting wave. Future direction of work is to study superharmonic instability of Stokes waves in finite depth.

11:30 am  12:30 pm EDTRevisit singularity formation for the inviscid primitive equation11th Floor Lecture Hall
 Slim IBRAHIM, University of Victoria
Abstract
The primitive equation is an important model for large scale fluid model including oceans and atmosphere. While solutions to the viscous model enjoy global regularity, inviscid solutions may develop singularities in finite time. In this talk, I will review the methods to show blowup, and share more recent progress on qualitative properties of the singularity formation.

2:00  4:30 pm EDTProbabilistic wellposedness for nonlinear Schrödinger equation (II)11th Floor Lecture Hall
 Yu Deng, University of Southern California

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, October 13, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am EDTProfessional Development: Ethics IIProfessional Development  11th Floor Lecture Hall

2:00  4:30 pm EDTProbabilistic wellposedness for nonlinear Schrödinger equation (II)11th Floor Lecture Hall
 Yu Deng, University of Southern California

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, October 14, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm EDTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, October 15, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, October 18, 2021

8:45  9:00 am EDTWelcome11th Floor Lecture Hall
 Brendan Hassett, ICERM/Brown University

9:00  9:50 am EDTMicrolocal analysis of singular measures11th Floor Lecture Hall
 Virtual Speaker
 Nicolas Burq, University ParisSud

10:00  10:30 am EDTCoffee Break11th Floor Collaborative Space

10:30  11:20 am EDTFull description of BenjaminFeir instability of Stokes waves in deep water11th Floor Lecture Hall
 Virtual Speaker
 Alberto Maspero, Scuola Internazionale Superiore di Studi Avanzati (SISSA)
Abstract
Smallamplitude, traveling, space periodic solutions  called Stokes waves  of the 2 dimensional gravity water waves equations in deep water are linearly unstable with respect to longwave perturbations, as predicted by Benjamin and Feir in 1967. We completely describe the behavior of the four eigenvalues close to zero of the linearized equations at the Stokes wave, as the Floquet exponent is turned on. We prove in particular the conjecture that a pair of nonpurely imaginary eigenvalues depicts a closed figure eight, parameterized by the Floquet exponent, in full agreement with numerical simulations. This is a joint work with M. Berti and P. Ventura.

11:30 am  1:00 pm EDTLunch/Free Time

1:00  1:50 pm EDTBreakdown of small amplitude breathers for the nonlinear KleinGordon equation11th Floor Lecture Hall
 Virtual Speaker
 Marcel Guardia, Universitat Politècnica de Catalunya
Abstract
Breathers are temporally periodic and spatially localized solutions of evolutionary PDEs. They are known to exist for integrable PDEs such as the sineGordon equation, but are believed to be rare for general nonlinear PDEs. When the spatial dimension is equal to one, exchanging the roles of time and space variables (in the socalled spatial dynamics framework), breathers can be interpreted as homoclinic solutions to steady solutions and thus arise from the intersections of the stable and unstable manifolds of the steady states. In this talk, we shall study the nonlinear KleinGordon equation and show that small amplitude breathers cannot exist (under certain conditions). We also construct generalized breathers, these are solutions which are periodic in time and in space are localized up to exponentially small (with respect to the amplitude) tails. This is a joint work with O. Gomide, T. Seara and C. Zeng.

2:00  2:50 pm EDTFluctuations of \deltamoments for the free Schrödinger Equation11th Floor Lecture Hall
 Luis Vega, Basque Center for Applied Mathematics (BCAM)
Abstract
I will present recent work done with S. Kumar and F.PonceVanegas.
We study the process of dispersion of lowregularity solutions to the free Schrödinger equation using fractional weights. We give another proof of the uncertainty principle for fractional weights and use it to get a lower bound for the concentration of mass. We consider also the evolution when the initial datum is the Dirac comb in R. In this case we find fluctuations that concentrate at rational times and that resemble a realization of a Lévy process. Furthermore, the evolution exhibits multifractality. 
3:00  4:30 pm EDTWelcome ReceptionReception  Hemenway's Patio
Tuesday, October 19, 2021

9:00  9:50 am EDTMathematical wave turbulence and propagation of chaos (I)11th Floor Lecture Hall
 Yu Deng, University of Southern California
Abstract
The theory of wave turbulence can be traced back to the 1920s and has played significant roles in many different areas of physics. However, for a long time the mathematical foundation of the theory has not been established. The central topics here are the wave kinetic equation, which describes the thermodynamic limit of interacting wave systems, and the propagation of chaos, which is a fundamental physical assumption in this field that lacks mathematical justification. In this first talk, I will present recent results with Zaher Hani (University of Michigan), where we provide the first rigorous derivation of the wave kinetic equation, and also justify the propagation of chaos assumption in the same setting. In part (II), we will discuss some important ideas in the proof.

10:00  10:30 am EDTCoffee Break11th Floor Collaborative Space

10:30  11:20 am EDTMathematical wave turbulence and propagation of chaos (II)11th Floor Lecture Hall
 Zaher Hani, University of Michigan
Abstract
The theory of wave turbulence can be traced back to the 1920s and has played significant roles in many different areas of physics. However, for a long time the mathematical foundation of the theory has not been established. The central topics here are the wave kinetic equation, which describes the thermodynamic limit of interacting wave systems, and the propagation of chaos, which is a fundamental physical assumption in this field that lacks mathematical justification. This talk is a continuation of that of Yu Deng (University of Southern California) who will present our recent joint results that provide the first rigorous derivation of the wave kinetic equation, and also justify the propagation of chaos assumption in the same setting. In this second part, we will discuss some important ideas in the proof.

11:30 am  1:00 pm EDTLunch/Free Time

1:00  1:50 pm EDTEnergy transfer for solutions to the nonlinear Schrodinger equation on irrational tori.11th Floor Lecture Hall
 Gigliola Staffilani, Massachusetts Institute of Technology
Abstract
We analyze the energy transfer for solutions to the defocusing cubic nonlinear Schr\"odinger (NLS) initial value problem on 2D irrational tori. Moreover we complement the analytic study with numerical experimentation. As a biproduct of our investigation we also prove that the quasiresonant part of the NLS initial value problem we consider, in both the focusing and defocusing case, is globally wellposed for initial data of finite mass.

2:00  2:50 pm EDTDeterminants, commuting flows, and recent progress on completely integrable systems11th Floor Lecture Hall
 Virtual Speaker
 Monica Visan, University of California, Los Angeles
Abstract
We will survey a number of recent developments in the theory of completely integrable nonlinear dispersive PDE. These include a priori bounds, the orbital stability of multisolitons, wellposedness at optimal regularity, and the existence of dynamics for Gibbs distributed initial data. I will describe the basic objects that tie together these disparate results, as well as the diverse ideas required for each problem.

3:10  4:00 pm EDTLightning Talks11th Floor Lecture Hall

4:00  4:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, October 20, 2021

9:00  9:50 am EDTOn the derivation of the Kinetic Wave Equation in the inhomogeneous setting11th Floor Lecture Hall
 Virtual Speaker
 Charles Collot, CergyParis Université
Abstract
The kinetic wave equation arises in weak wave turbulence theory. In this talk we are interested in its derivation as an effective equation from dispersive waves modelled with quadratic nonlinear Schrodinger equations. We focus on the spaceinhomogeneous case, which had not been treated earlier. More precisely, we will consider such a dispersive equations in a weakly nonlinear regime, and for highly oscillatory random Gaussian fields with localised enveloppes as initial data. A conjecture in statistical physics is that there exists a kinetic time scale on which, statistically, the Wigner transform of the solution (a space dependent local Fourier energy spectrum) evolve according to the kinetic wave equation.
I will present a joint work with Ioakeim Ampatzoglou and Pierre Germain (Courant Institute) in which we approach the problem of the validity of this kinetic wave equation through the convergence and stability of the corresponding Dyson series. We are able to identify certain nonlinearities, dispersion relations, and regimes, and for which the convergence indeed holds almost up to the kinetic time (arbitrarily small polynomial loss). 
10:00  10:30 am EDTCoffee Break11th Floor Collaborative Space

10:30  11:20 am EDT3 Problems in Wave Turbulence11th Floor Lecture Hall
 Jalal Shatah, New York University

11:30  11:40 am EDTGroup Photo (Immediately After Talk)11th Floor Lecture Hall

11:40 am  1:00 pm EDTLunch/Free Time

1:00  1:50 pm EDTConstructing global solutions for energy supercritical NLS equations11th Floor Lecture Hall
 Virtual Speaker
 Mouhamadou Sy, Imperial College London
Abstract
The last decades were very fruitful for the realm of dispersive PDEs. Besides several new deterministic developments in the study of the initial value problem and the behavior of solutions, probabilistic methods were introduced and made important progresses, particularly on bounded domain settings. Invariant measure are of considerable interest in these questions. However, in the context of energy supercritical equations, both the wellknown Gibbs measures based strategy and the standard fluctuationdissipation approach come across serious limitations. In this talk, we will present a new approach that combines the aforementioned ones to construct invariant measures, almost sure GWP, and strong controls on the time evolution of the solutions for the periodic NLS, with arbitrarily large power of nonlinearity and in any dimension. We will discuss the application to other contexts including nondispersive PDEs.

2:00  2:30 pm EDTCoffee Break11th Floor Collaborative Space

2:30  3:20 pm EDTInvariant Gibbs measures for NLS and Hartree equations11th Floor Lecture Hall
 Haitian Yue, University of Southern California
Abstract
In this talk, I'll present our results about invariant Gibbs measures for the periodic nonlinear Schrödinger equation (NLS) in 2D, for any (defocusing and renormalized) odd power nonlinearity and for the periodic Hartree equation in 3D. The results are achieved by introducing a new method (we call the random averaging operators method) which precisely captures the intrinsic randomness structure of the problematic highlow frequency interactions at the heart of this problem. This is work with Yu Deng (USC) and Andrea Nahmod (UMass Amherst).
Thursday, October 21, 2021

9:00  9:50 am EDTSingularities in the weak turbulence regime11th Floor Lecture Hall
 Virtual Speaker
 AnneSophie de Suzzoni, Ecole Polytechnique
Abstract
In this talk, we discuss the different regimes for the derivation of kinetic equations from the theory of weak turbulence for the quintic Schrödinger equation. In particular, we see that there exists a specific regime such that the correlations of the Fourier coefficients of the solution of the Schrödinger equation converge (in this regime) to a function that has an inifinite number of discontinuities.

10:00  10:30 am EDTCoffee Break11th Floor Collaborative Space

10:30  11:20 am EDTA New model for the stochasticly perturbed 2d navierstokes equations11th Floor Lecture Hall
 Jonathan Mattingly, Duke University
Abstract
I will introduce a new model of the stochastically forced navierstokes equation. The model will be targeted at studying the Equations forced by a large scale forcing. I give a number of properties of the model.

11:30 am  1:00 pm EDTLunch/Free Time

1:00  1:50 pm EDTGlobal wellposedness for the fractional NLS on the unit disk11th Floor Lecture Hall
 Xueying Yu, University of Washington
Abstract
In this talk, we discuss the cubic nonlinear Schr\"odinger equation with the fractional Laplacian on the unit disk. We show the global wellposedness for certain radial initial data below the energy space and establish a polynomial bound of the global solution. The result is proved by extending the Imethod in the fractional nonlinear Schr\"odinger equation setting.

2:00  2:30 pm EDTCoffee Break11th Floor Collaborative Space

2:30  3:20 pm EDTThe wave maps equation and Brownian paths11th Floor Lecture Hall
 Bjoern Bringmann, Institute for Advanced Study
Abstract
We discuss the $(1+1)$dimensional wave maps equation with values in a compact Riemannian manifold $\mathcal{M}$. Motivated by the Gibbs measure problem, we consider Brownian paths on the manifold $\mathcal{M}$ as initial data. Our main theorem is the probabilistic local wellposedness of the associated initial value problem. The analysis in this setting involves analytic, geometric, and probabilistic aspects. This is joint work with J. Lührmann and G. Staffilani.
Friday, October 22, 2021

9:00  9:50 am EDTPositive Lyapunov exponents for the GalerkinNavierStokes equations with stochastic forcing11th Floor Lecture Hall
 Jacob Bedrossian, University of Maryland
Abstract
In this talk we discuss our recently introduced methods for obtaining strictly positive lower bounds on the top Lyapunov exponent of highdimensional, stochastic differential equations such as the weaklydamped Lorenz96 (L96) model or Galerkin truncations of the 2d NavierStokes equations (joint with Alex Blumenthal and Sam PunshonSmith). This hallmark of chaos has long been observed in these models, however, no mathematical proof had previously been made for any type of deterministic or stochastic forcing. The method we proposed combines (A) a new identity connecting the Lyapunov exponents to a Fisher information of the stationary measure of the Markov process tracking tangent directions (the socalled "projective process"); and (B) an L1based hypoelliptic regularity estimate to show that this (degenerate) Fisher information is an upper bound on some fractional regularity. For L96 and GNSE, we then further reduce the lower bound of the top Lyapunov exponent to proving that the projective process satisfies Hörmander's condition. I will also discuss the recent work of Sam PunshonSmith and I on verifying this condition for the 2d GalerkinNavierStokes equations in a rectangular, periodic box of any aspect ratio using some special structure of matrix Lie algebras and ideas from computational algebraic geometry.

10:00  10:30 am EDTCoffee Break11th Floor Collaborative Space

10:30  11:20 am EDTA tale of two generalizations of Boltzmann equation11th Floor Lecture Hall
 Nataša Pavlovic, University of Texas at Austin
Abstract
In the first part of the talk we shall discuss dynamics of systems of particles that allow interactions beyond binary, and their behavior as the number of particles goes to infinity. This part of the talk is based on the joint work with Ampatzoglou on a derivation of a binaryternary Boltzmann equation describing the kinetic properties of a dense hard spheres gas, where particles undergo either binary or ternary instantaneous interactions, while preserving momentum and energy. An important challenge we overcome in deriving this equation is related to providing a mathematical framework that allows us to detect both binary and ternary interactions. In the second part of the talk we will discuss a rigorous derivation of a Boltzmann equation for mixtures of gases, which is a recent joint work with Ampatzoglou and Miller. We prove that the microscopic dynamics of two gases with different masses and diameters is well defined, and introduce the concept of a two parameter BBGKY hierarchy to handle the nonsymmetric interaction of these gases.

11:30 am  12:20 pm EDTSome Recent Results On Wave Turbulence: Derivation, Analysis, Numerics and Physical Application11th Floor Lecture Hall
 MinhBinh Tran, Southern Methodist University
Abstract
Wave turbulence describes the dynamics of both classical and nonclassical nonlinear waves out of thermal equilibrium. In this talk, we will discuss some of our recent results on some aspects of wave turbulence, concerning the derivation and analysis of wave kinetic equations, some numerical algorithms and physical applications in BoseEinstein Condensates.
Monday, October 25, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Tuesday, October 26, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am EDTWeak universality for the fractional \Phi_2^4 under the wave dynamics11th Floor Lecture Hall
 Chenmin Sun, CY CergyParis Université
Abstract
Parabolic \Phi^4 models, given by singular stochastic heat equation are believed to be the scaling limit for some physical relevant models. This motivated many recent results in the field of singular SPDE. In the context of dispersive equations, it is also of interest to investigate the limit of certain dispersive \Phi^4 models perturbed by higherorder potentials with correct scalings. In this talk, we consider the weak universality of the twodimensional fractional nonlinear wave equation. For a sequence of Hamiltonians of highdegree potentials scaling to the fractional \Phi_2^4, we first establish a sufficient and almost necessary criteria for the convergence of invariant measures to the fractional \Phi_2^4. Then we prove the convergence result for the sequence of associated wave dynamics to the (renormalized) cubic wave equation. The main difficulty is that we do not have a good local Cauchytheory for the highly supercritical nonlinearities. To prove the dynamical convergence, we rely on probabilistic ideas exploiting independence of different scales of frequencies. This is a joint work with Nikolay Tzvetkov and Weijun Xu.

11:30 am  12:30 pm EDTGlobal axisymmetric Euler flows with rotation11th Floor Lecture Hall
 Klaus Widmayer, EPFL, Switzerland
Abstract
We discuss the construction of a class of global, dynamical solutions to the 3d Euler equations near the stationary state given by uniform "rigid body" rotation. These solutions are axisymmetric, of Sobolev regularity and have nonvanishing swirl. At the heart of this result is the dispersive effect due to rotation, which is captured in our new "method of partial symmetries". This approach is adapted to maximally exploit the symmetries of this anisotropic problem, both for the linear and nonlinear analysis, and allows to globally propagate sharp decay estimates. This is joint work with Y. Guo and B. Pausader.

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, October 27, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am EDTProfessional Development: Job Applications in AcademiaProfessional Development  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, October 28, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm EDTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, October 29, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, November 1, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Tuesday, November 2, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am EDTGlobal solutions of aggregation equations and other flows with random diffusion11th Floor Lecture Hall
 Matthew Rosenzweig, Massachusetts Institute of Technology
Abstract
Aggregation equations, such as the parabolicelliptic PatlakKellerSegel model, are known to have an optimal threshold for global existence vs. finitetime blowup. In particular, if the diffusion is absent, then all smooth solutions with finite second moment can exist only locally in time. Nevertheless, one can ask whether global existence can be restored by adding a suitable noise to the equation, so that the dynamics are now stochastic. In this talk, we investigate whether random diffusion can restore global existence for a large class of active scalar equations in arbitrary dimension with possibly singular velocity fields. This class includes Hamiltonian flows, such as the SQG equation and its generalizations, and gradient flows, such as those arising in aggregation models. For this class, we show global existence of solutions in Gevreytype FourierLebesgue spaces with quantifiable high probability. This talk is based on joint work with Gigliola Staffilani.

11:15 am  12:15 pm EDTNumerical computations of invariant probability measures and their ergodicity11th Floor Lecture Hall
 Yao Li, University of Massachusetts Amherst
Abstract
Consider a stochastic process (such as a stochastic differential equation) that admits an invariant probability measure. We are interested in many things like the landscape, the sensitivity, and the speed of convergence of the invariant probability measure. Since it is difficult to obtain sharp estimates rigorously, some numerical computations are usually necessary. In this talk I will introduce a few novel datadriven computational methods, including both classical and deep learning approaches, to solve these problems for a class of stochastic processes. Generally those datadriven methods are less affected by the curseofdimensionality than classical gridbased methods. I will demonstrate a few high (up to 100) dimensional examples in my talk.

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Wednesday, November 3, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am EDTProfessional Development: Hiring ProcessProfessional Development  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Thursday, November 4, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm EDTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Friday, November 5, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm EDTCoffee Break11th Floor Collaborative Space
Monday, November 8, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Tuesday, November 9, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

10:00  11:00 am ESTLargetime dynamics of NLS in 3D with random data11th Floor Lecture Hall
 Nicolas Camps, Université Paris Saclay
Abstract
In this talk, we investigate the large time behavior of a probabilistic flow, solution to the defocusing cubic Schr ̈odinger equation in the Euclidean space of dimension 3. First, we consider the stability of small ground states which emerge from the presence of an external shortrange potential. By performing a “criticalweighted” strategy, we prove that these ground states are asymp totically stable below the energy space. At supercritical regularity, this result holds true almostsurely, when the data are randomized according to the Wiener decomposition. We then address the scattering issue, outside the small data regime. In order to do so, we propose a way to revisit in a probabilistic setting the Imethod with a Morawetz bootstrap.

11:15 am  12:15 pm ESTZerodispersion limit for the BenjaminOno equation on the torus11th Floor Lecture Hall
 Louise Gassot, Laboratoire de Mathématiques d'Orsay  Université ParisSaclay
Abstract
We discuss the zerodispersion limit for the BenjaminOno equation on the torus given a single well initial data. We prove that there exist approximate initial data converging to the initial data, such that the corresponding solutions admit a weak limit as the dispersion parameter tends to zero. The weak limit is expressed in terms of the multivalued solution of the inviscid Burgers equation obtained by the method of characteristics. We construct our approximation by using the Birkhoff coordinates of the initial data, introduced by Gérard, Kappeler and Topalov. In the case of the cosine initial data, we completely justify this approximation by proving an asymptotic expansion of the Birkhoff coordinates.

1:00  5:00 pm ESTReserved for Maintenance11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Wednesday, November 10, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am ESTProfessional Development: Papers and JournalsProfessional Development  11th Floor Lecture Hall

11:00 am  12:30 pm ESTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

12:30  12:45 pm ESTPostdoc/ Grad Student Group PhotoGroup Photo (Immediately After Talk)  11th Floor Lecture Hall

1:00  5:00 pm ESTReserved for Maintenance11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Thursday, November 11, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Friday, November 12, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Monday, November 15, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Tuesday, November 16, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:30  10:20 am ESTPersistence of Invariant Manifolds under Singular Perturbations11th Floor Lecture Hall
 Jiaqi Yang, ICERM
Abstract
We study persistence of the invariant manifolds of systems under delayrelated perturbations. The perturbations are very singular no matter how small they are. Our treatment bypasses the discussion of the phase space and evolution of the perturbed systems, which are known to be debatable. More precisely, we take advantage of the parameterization method, and solve equations of functions (invariance equations) with analysis. Our results are in aposteriori format. The constructive proofs rely on the fixed point approach. Therefore, our results provide algorithms and are suitable for computerassisted proofs.

10:30  11:20 am ESTHamiltonian Dysthe equation for 3d deepwater gravity waves.11th Floor Lecture Hall
 Virtual Speaker
 Adilbek Kairzhan, University of Toronto
Abstract
In this talk, we consider the water wave problem in a threedimensional domain of infinite depth and examine the modulational regime for weakly nonlinear wavetrains. Using the method of normal form transformations near the equilibrium state, we discuss how to derive the Hamiltonian Dysthe equation describing the slow evolution of the wave envelope. We also discuss how a precise calculation of the thirdorder normal form allows for a refined reconstruction of the free surface.
In conclusion, we show the comparison between our approximation, direct numerical simulations of the threedimensional Euler system and predictions from the classical Dysthe equation. 
11:30 am  12:20 pm ESTThermal convection in a penny shape cylinder: from idealized numerical models to tropical cyclones11th Floor Lecture Hall
 Ludivine Oruba, Sorbonne Universite
Abstract
We investigate atmospherical vortices using idealized mathematical models and direct numerical simulations. We establish connection both with geophysical observations and asymptotic developments.
We consider rotating convection in an elongated cylindrical domain, which intends to model the lower atmosphere. We examine the conditions under which the main vortex develops an eye at its core, which is reminiscent of that seen in a tropical cyclone ; that is, a region where the poloidal flow reverses and the angular momentum is low.
We first focus on the stationary flow and highlight the key role played by the viscous bottom boundary layer in the eye formation. We show that the eye results from a nonlinear instability.
In a mixed numerical / asymptotic approach, we then study the linear inertial wave activity which develops in the time dependent problem. These inertial waves are indeed reminiscent of oscillations which have been observed near the eye of actual tropical cyclones.
References:
L Oruba, P.A. Davidson and E. Dormy, J. Fluid Mech. (2017), 812, 890904.
L Oruba, A. M. Soward and E. Dormy, J. Fluid Mech. (2020), 888, A9.
L Oruba, A. M. Soward and E. Dormy, J. Fluid Mech. (2021), 915, A53. 
3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Wednesday, November 17, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:00  10:00 am ESTProfessional Development: Grant ProposalsProfessional Development  11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Thursday, November 18, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm ESTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Friday, November 19, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Monday, November 22, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Tuesday, November 23, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:30  10:20 am ESTEnergies and phase space for the 1d GrossPitaevskii equation11th Floor Lecture Hall
 Virtual Speaker
 Herbert Koch, University of Bonn
Abstract
The GrossPitaevskii equation is essentially the defocusing cubic nonlinear Schroedinger equation, but with energies which enforce that the absolute value of solutions tends to 1 as x tends to +/ infinity. Striking solutions are black and dark solitons. I will explain nonlinear phase spaces for solutions which contain the black and dark solitons, explain a new metric on it and its smooth and topological structure. I will conclude with the construction of a continuous family of conserved energies. This is joint work with Xian Liao

10:30  11:20 am ESTPhase transitions of the focusing Φ^p_1 measures11th Floor Lecture Hall
 Virtual Speaker
 Leonardo Tolomeo, Universität Bon
Abstract
We study the behaviour of the focusing Φ^p_1 measures on the onedimensional torus, initiated by Lebowitz, Rose, and Speer (1988). Because of the focusing nature of the measure, it is necessary to introduce a mass cutoff K, and restrict the measure to the set where the mass is smaller than K. We will show the following phase transitions:  When K is smaller than a certain threshold, the measure is well defined, while for K bigger than the threshold, the measure becomes nonnormalisable. We will also discuss what happens at the optimal threshold, and show that the measure is well defined in this case as well, solving a longstanding open problem. This is joint work with T. Oh (University of Edinburgh) and P. Sosoe (Cornell University).
 When the size L of the torus is going to infinity, in the weakly nonlinear regime, numeric simulations in the original paper by Lebowitz, Rose, and Speer (1988) suggest a phase transition depending on the temperature of the system. We show that this is indeed the case: if the temperature is high, the Φ^p_1 measure converges to a given gaussian measure. However, this convergence does not happen in the lowtemperature regime, and instead the measure progressively concentrates around a single soliton. This is joint work with H. Weber (University of Bath). 
11:30 am  12:20 pm ESTThe regularity of solutions to the Muskat equation with turnover points.11th Floor Lecture Hall
 Jia Shi, Princeton University
Abstract
The Muskat equation describes the interface of two liquids in porous media. When the heavier liquid lies under the lighter one, the equation behaves like a parabolic equation. When the heavier one is above the lighter one, it looks like a backward parabolic equation. However, the behavior has been proved to be local in time. There exist solutions that start from a graph and develop a turnover point as the time is going. I will discuss the regularity of the solutions to the Muskat problems with turnover points and show that they are analytic except at the turnover points, given that the solutions are smooth enough.

12:20  12:30 pm ESTSemester Program Group PhotoGroup Photo (Immediately After Talk)  11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Monday, November 29, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

11:00 am  12:30 pm ESTPost Doc/Graduate Student SeminarPost Doc/Graduate Student Seminar  11th Floor Lecture Hall

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Tuesday, November 30, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

9:30  10:20 am ESTAsymptotic stability of the sineGordon kink under odd perturbations.11th Floor Lecture Hall
 Jonas Luhrmann, Texas A&M University
Abstract
The sineGordon model is a classical nonlinear scalar field theory that was discovered in the 1860s in the context of the study of surfaces with constant negative curvature. Its equation of motion features soliton solutions called kinks and breathers, which play an important role for the longtime dynamics. I will begin the talk with an introduction to classical 1D scalar field theories and the asymptotic stability problem for kinks. After surveying recent progress on the problem, I will present a joint work with W. Schlag on the asymptotic stability of the sineGordon kink under odd perturbations. Our proof is perturbative and does not rely on the complete integrability of the sineGordon model. Key aspects are a supersymmetric factorization property of the linearized operator and a remarkable nonresonance property of a variable coefficient quadratic nonlinearity.

10:30  11:20 am ESTGagliardoNirenbergSobolev inequality in Dirichlet spaces.11th Floor Lecture Hall
 Patricia Alonso Ruiz, Texas A&M University
Abstract
The GagliardoNirenbergSobolev inequality in R^n is a classical Sobolev embedding with many applications in the theory of PDEs and calculus of variations. In this talk, I will present the full scale of GagliardoNirenbergSobolev inequalities in the more general framework of Dirichlet spaces with (sub)Gaussian heat kernel estimates. In particular, we will discover that the optimal exponent in the embedding not only depends on the Hausdorff dimension of the underlying space, but also on other invariants. To this end, I will use a recent approach to (1,p)Sobolev spaces via heat semigroups inspired by ideas going back to work of de Giorgi and Ledoux. If time permits, I will outline some results and conjectures concerning further Sobolev embeddings in this setting. The talk is based on joint work with F. Baudoin.

11:30 am  12:20 pm ESTBirkhoff normal forms for Hamiltonian PDEs in their energy space11th Floor Lecture Hall
 Benoît Grébert, University of Nantes
Abstract
We study the long time behavior of small solutions of semilinear dispersive Hamiltonian partial differential equations on confined domains. Provided that the system enjoys a new nonresonance condition and a strong enough energy estimate, we prove that its low superactions are almost preserved for very long times. Roughly speaking, it means that, only modes with the same linear frequency will be able to exchange energy in a reasonable time. Contrary to the previous existing results, we do not require the solutions to be especially smooth. They only have to live in the energy space. We apply our result to nonlinear KleinGordon equations in dimension $d=1$ and nonlinear Schrödinger equations in dimension $d\leq 2$.

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Wednesday, December 1, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Thursday, December 2, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Friday, December 3, 2021
Hamiltonian Methods in Dispersive and Wave Evolution Equations

3:00  3:30 pm ESTCoffee Break11th Floor Collaborative Space
Monday, December 6, 2021

8:55  9:00 am ESTWelcome11th Floor Lecture Hall
 Brendan Hassett, ICERM/Brown University

9:00  10:00 am ESTAsymptotic stability of the SineGordon kink under odd perturbations via supersymmetry11th Floor Lecture Hall
 Wilhelm Schlag, Yale University
Abstract
We will describe the recent asymptotic analysis with Jonas Luehrmann of the SineGordon evolution of odd data near the kink. We do not rely on the complete integrability of the problem in a direct way, in particular we do not use the inverse scattering transform.

10:00  10:30 am ESTCoffee Break11th Floor Collaborative Space

10:30  11:15 am ESTTimedependent BogoliubovdeGennes and GinzburgLandau equations11th Floor Lecture Hall
 Virtual Speaker
 Rupert Frank, LMU Munich
Abstract
We study the timedependent BogoliubovdeGennes equations for generic translationinvariant fermionic manybody systems. For initial states that are close to thermal equilibrium states at temperatures near the critical temperature, we show that the magnitude of the order parameter stays approximately constant in time and, in particular, does not follow a timedependent GinzburgLandau equation, which is often employed as a phenomenological description and predicts a decay of the order parameter in time.

11:30 am  12:15 pm ESTOn the wellposedness of the derivative nonlinear Schr\"odinger equation11th Floor Lecture Hall
 Maria Ntekoume, Rice University
Abstract
We consider the derivative nonlinear Schr\"odinger equation in one space dimension, posed both on the line and on the circle. This model is known to be completely integrable and $L^2$critical with respect to scaling. However, not much is known regarding the wellposendess of the equation below $H^{\frac 12}$. In this talk, we prove that this problem is globally wellposed for initial data in the Sobolev spaces $H^s$ for $\frac 1 6\leq s<\frac 12$. The key ingredient in our argument is proving that ensembles of orbits with $L^2$equicontinuous initial data remain equicontinuous under evolution. This is joint work with Rowan Killip and Monica Visan.

12:30  2:30 pm ESTLunch/Free Time

2:30  3:30 pm ESTQuantitative derivation and scattering of the 3D cubic NLS in the energy space11th Floor Lecture Hall
 Justin Holmer, Brown University
Abstract
We consider the derivation of the {defocusing cubic nonlinear Schr\"{o}dinger equation (NLS) on $\mathbb{R}^{3}$ from quantum $N$body dynamics. We reformat the hierarchy approach with KlainermanMachedon theory and prove a biscattering theorem for the NLS to obtain convergence rate estimates under $H^{1}$ regularity. The $H^{1}$ convergence rate estimate we obtain is almost optimal for $H^{1}$ datum, and immediately improves if we have any extra regularity on the limiting initial oneparticle state. This is joint work with Xuwen Chen (University of Rochester).

3:30  4:30 pm ESTLocal smoothing estimate for the cone in R^311th Floor Lecture Hall
 Virtual Speaker
 Hong Wang, Institute for Advanced Study (IAS)
Abstract
If u is a solution to the wave equation on R^n, a local smoothing inequality bounds $\u\_{L^p(\mathbb{R}^n\times [1,2])}$ in terms of the Sobolev norms of the initial data. We prove Sogge's local smoothing conjecture in 2+1 dimensions.
In the proof, we introduced an approximation of the $L^4$norm that works better for induction. Another key ingredient is an incidence estimate for points and tubes.
This is joint work with Larry Guth and Ruixiang Zhang. 
4:30  6:00 pm ESTWelcome ReceptionReception  11th Floor Collaborative Space
Tuesday, December 7, 2021

9:00  9:45 am ESTHighOrder Rogue Waves and Solitons, and Solutions Interpolating Between Them11th Floor Lecture Hall
 Virtual Speaker
 Peter Miller, University of Michigan
Abstract
A family of exact solutions to the focusing nonlinear Schrödinger equation is presented that contains fundamental rogue waves and multiplepole solitons of all orders. The family is indexed with a continuous parameter representing the "order" that allows one to continuously tune between rogue waves and solitons of different integer orders. In this scheme, solitons and rogue waves of increasing integer orders alternate as the continuous order parameter increases. For example, the Peregrine solution can be viewed as a soliton of order threehalves. We show that solutions in this family exhibit certain universal features in the limit of high (continuous) order. This is joint work with Deniz Bilman (Cincinnati).

10:00  10:30 am ESTCoffee Break11th Floor Collaborative Space

10:30  11:15 am ESTLandau law and stability of 3D shocks11th Floor Lecture Hall
 Virtual Speaker
 Igor Rodnianski, Princeton University
Abstract
We will discuss stability and long term behavior of 3 dimensional compressible irrotational shocks arising in the compressible Euler equations.
In 1945, Landau argued that spherically symmetric solutions which form weak shocks will settle to a profile with 2 shocks decaying at the rate proportionate to 1/{t\sqrt{\log t}}. We address this conjecture by first identifying the asymptotic profile which exhibit 2 shocks, as a selfsimilar solution of a related Burgers equation, and then proving its stability and the conjectured rate of decay for general (nonspherically symmetric) perturbations. This is joint work with D. Ginsberg. 
11:30 am  12:15 pm ESTGround state in the energy supercritical GrossPitaevskii equation with a harmonic potential11th Floor Lecture Hall
 Virtual Speaker
 Dmitry Pelinovsky, McMaster University
Abstract
In order to prove the existence of a ground state (a positive, radially symmetric solution in the energy space), we develop the shooting method and deal with a oneparameter family of classical solutions to an initialvalue problem for the stationary equation. We prove that the solution curve (the graph of the eigenvalue parameter versus the supremum norm) is oscillatory below a threshold and monotone above a threshold. Compared to the existing literature, rigorous asymptotics are derived by constructing families of solutions to the stationary equation with functionalanalytic rather than geometric methods. The same analytical technique allows us to characterize the Morse index of the ground state.

12:30  2:00 pm ESTLunch/Free Time

2:00  2:45 pm ESTRigidity for solutions to the quintic NLS equation at the ground state level11th Floor Lecture Hall
 Benjamin Dodson, John Hopkins University
Abstract
In this talk, we will prove rigidity for solutions to the quintic nonlinear Schrodinger equation in one dimension, at the level of the ground state. Specifically, we show that the only solutions that fail to scatter are the solitons and the pseudoconformal transformation of the solitons.

3:00  4:30 pm ESTLightning Talks followed by Coffee Break and discussionsLightning Talks  11th Floor Lecture Hall
Wednesday, December 8, 2021

9:00  9:45 am ESTA Rigorous Derivation of the Hamiltonian Structure for the Nonlinear Schrodinger Equation11th Floor Lecture Hall
 Virtual Speaker
 Nataša Pavlovic, University of Texas at Austin
Abstract
Many mathematical works have focused on understanding the manner in which the dynamics of the nonlinear Schrodinger equation (NLS) arises as an effective equation. By effective equation, we mean that solutions of the NLS equation approximate solutions to an underlying physical equation in some topology in a particular asymptotic regime. For example, the cubic NLS is an effective equation for a system of N bosons interacting pairwise via a delta or approximate delta potential. In this talk, we will advance a new perspective on deriving an effective equation, which focuses on structure. In particular, we will show how the Hamiltonian structure for the cubic NLS in any dimension arises from corresponding structure at the Nparticle level. Also we will discuss what we have learned so far about understanding origins of integrability of the 1D cubic NLS. The talk is based on joint works with Dana Mendelson, Andrea Nahmod, Matthew Rosenzweig and Gigliola Staffilani.

10:00  10:30 am ESTCoffee Break11th Floor Collaborative Space

10:30  11:15 am ESTGibbs measures, canonical stochastic quantization, and singular stochastic wave equations11th Floor Lecture Hall
 Virtual Speaker
 Tadahiro Oh, The University of Edinburgh
Abstract
In this talk, I will discuss the (non)construction of the focusing Gibbs measures and the associated dynamical problems. This study was initiated by Lebowitz, Rose, and Speer (1988) and continued by Bourgain (1994), BrydgesSlade (1996), and CarlenFröhlichLebowitz (2016). In the onedimensional setting, we consider the masscritical case, where a critical mass threshold is given by the mass of the ground state on the real line. In this case, I will show that the Gibbs measure is indeed normalizable at the optimal mass threshold, thus answering an open question posed by Lebowitz, Rose, and Speer (1988).
In the three dimensionalsetting, I will first discuss the construction of the $\Phi^3_3$measure with a cubic interaction potential. This problem turns out to be critical, exhibiting a phase transition: normalizability in the weakly nonlinear regime and nonnormalizability in the strongly nonlinear regime. Then, I will discuss the dynamical problem for the canonical stochastic quantization of the $\Phi^3_3$measure, namely, the threedimensional stochastic damped nonlinear wave equation with a quadratic nonlinearity forced by an additive spacetime white noise (= the hyperbolic $\Phi^3_3$model). As for the local theory, I will describe the paracontrolled approach to study stochastic nonlinear wave equations, introduced in my work with Gubinelli and Koch (2018). In the globalization part, I introduce a new, conceptually simple and straightforward approach, where we directly work with the (truncated) Gibbs measure, using the variational formula and ideas from theory of optimal transport.
The first part of the talk is based on a joint work with Philippe Sosoe (Cornell) and Leonardo Tolomeo (Bonn), while the second part is based on a joint work with Mamoru Okamoto (Osaka) and Leonardo Tolomeo (Bonn). 
11:30 am  12:15 pm ESTMathematical Construction for Gravitational Collapse11th Floor Lecture Hall
 Yan Guo, Brown University
Abstract
We will discuss recent constructions of blowup solutions for describing gravitational collapse for EulerPoisson system.

12:30  12:40 pm ESTGroup Photo (Immediately After Talk)11th Floor Lecture Hall

12:40  2:30 pm ESTLunch/Free Time

2:30  3:15 pm ESTInternal Modes and Radiation Damping for 3d KleinGordon equations11th Floor Lecture Hall
 Virtual Speaker
 Fabio Pusateri, University of Toronto
Abstract
We consider quadratic KleinGordon equations with an external potential $V$ in $3+1$ spacetime dimensions. We assume that $V$ is generic and decaying, and that the operator $\Delta + V + m^2$ has an eigenvalue $\lambda^2 < m^2$. This is a socalled ‘internal mode’ and gives rise to timeperiodic localized solutions of the linear flow. We address the question of whether such solutions persist under the full nonlinear flow. Our main result shows that small nonlinear solutions slowly decay as the energy is transferred from the internal mode to the continuous spectrum, provided a natural Fermi golden rule holds. Moreover, we obtain very precise asymptotic information including sharp rates of decay and the growth of weighted norms. These results extend the seminal work of SofferWeinstein for cubic nonlinearities to the case of any generic perturbation. This is joint work with Tristan Léger (Princeton University).

3:30  4:00 pm ESTCoffee Break11th Floor Collaborative Space

4:00  4:45 pm ESTSolutions to the KdV and Related Equations With Almost Periodic Initial Data11th Floor Lecture Hall
 David Damanik, Rice University
Abstract
We discuss recent work concerning the existence, uniqueness, and structure of solutions to the KdV equation, as well as related ones, with almost periodic initial data. The talk is based on several joint works with a variety of coauthors, including Ilia Binder, Michael Goldstein, Yong Li, Milivoje Lukic, Alexander Volberg, Fei Xu, and Peter Yuditskii.
Thursday, December 9, 2021

9:00  9:45 am ESTThe Quartic Integrability and Long Time Existence of Steep Water Waves in 2D11th Floor Lecture Hall
 Virtual Speaker
 Sijue Wu, University of Michigan
Abstract
Abstract. It is known since the work of Dyachenko & Zakharov in 1994 that for the weakly nonlinear 2d infinite depth water waves, there are no 3wave interactions and all of the 4wave interaction coefficients vanish on the non trivial resonant manifold. In this talk, I will present a recent result that proves this partial integrability from a different angle. We construct a sequence of energy functionals Ej (t), directly in the physical space, which are explicit in the Riemann mapping variable and involve material derivatives of order j of the solutions for the 2d water wave equation, so that ddtEj (t) is quintic or higher order. We show that if some scaling invariant norm, and a norm involving one spacial derivative above the scaling of the initial data are of size no more than ε, then the lifespan of the solution for the 2d water wave equation is at least of order O(ε−3), and the solution remains as regular as the initial data during this time. If only the scaling invariant norm of the data is of size ε, then the lifespan of the solution is at least of order O(ε−5/2). Our long time existence results do not impose size restrictions on the slope of the initial interface and the magnitude of the initial velocity, they allow the interface to have arbitrary large steepnesses and initial velocities to have arbitrary large magnitudes.

10:00  10:30 am ESTCoffee Break11th Floor Collaborative Space

10:30  11:15 am ESTGlobal wellposedness of the Zakharov System below the ground state11th Floor Lecture Hall
 Virtual Speaker
 Sebastian Herr, Bielefeld University
Abstract
We consider the Cauchy problem for the Zakharov system with a focus on the energycritical dimension d = 4 and prove that global wellposedness holds in the full (nonradial) energy space for any initial data with energy and wave mass below the ground state threshold. The result is based on a uniform Strichartz estimate for the Schr ̈odinger equation with potentials solving the wave equation. This is joint work with Timothy Candy and Kenji Nakanishi.

11:30 am  12:15 pm ESTStability of solitary waves in the generalized BenjaminOno equation and its 2d extensions11th Floor Lecture Hall
 Svetlana Roudenko, Florida International University
Abstract
We discuss solitary wave solutions in the generalized BenjaminOno equation, including the critical and supercritical cases. We then look at its higherdimensional generalization in 2d, the Shrira equation, and its fractional generalization, the HBO (Higherdimensional BenjaminOno) equation and examine the behavior of solutions in various cases as well as the stability of solitary waves.

12:30  2:30 pm ESTLunch/Free Time

2:30  3:15 pm ESTLow regularity solutions for nonlinear waves11th Floor Lecture Hall
 Daniel Tataru, University of California, Berkeley
Abstract
The sharp local wellposedness result for generic nonlinear wave equations was proved in my work with Smith about 20 years ago. Around the same time, it was conjectured that, for problems satisfying a suitable nonlinear null condition, the local wellposedness threshold can be improved. In this talk, I will describe the first result establishing this conjecture for a good model. This is joint work with Albert Ai and Mihaela Ifrim.

3:30  4:00 pm ESTCoffee Break11th Floor Collaborative Space

4:00  4:45 pm ESTSimple motion of stretchlimited elastic strings11th Floor Lecture Hall
 Virtual Speaker
 Casey Rodriguez, University of North Carolina
Abstract
Perfectly flexible strings are among the simplest onedimensional continuum bodies and have a rich mechanical and mathematical theory dating back to the derivation of their equations of motion by Euler and Lagrange. In classical treatments, the string is either completely extensible (force produces stretching) or completely inextensible (every segment has a fixed length, regardless of the motion). However, common experience is that a string can be stretched (is extensible), and after a certain amount of force is applied the stretch of the string is maximized (becoming inextensible). In this talk, we discuss a simple model for these stretchlimited elastic strings, in what way they model ``elastic" behavior, the wellposedness and asymptotic stability of certain simple motions, and (many) open questions.
Friday, December 10, 2021

9:00  9:45 am ESTKink stability in nonlinear KleinGordon equations11th Floor Lecture Hall
 Pierre Germain, NYU  Courant Institute
Abstract
Nonlinear KleinGordon equations whose potential have a double well admit kink solutions (most famous examples: Phi4, SineGordon). I will present joint work with Fabio Pusateri which establishes the stability of this kink under some spectral conditions on the linearized problem. The key idea of the proof is to view the problem through the distorted Fourier transform associated with the linearized problem.

10:00  10:30 am ESTCoffee Break11th Floor Collaborative Space

10:30  11:15 am ESTNontrivial selfsimilar blowup in energy supercritical wave equations11th Floor Lecture Hall
 Birgit Schoerkhuber, University of Innsbruck, Austria
Abstract
Selfsimilar solutions play an important role in the dynamics of nonlinear wave equations as they provide explicit examples for finitetime blowup. This talk will be concerned with the focusing cubic and the quadratic wave equation, respectively, in dimensions where the models are energy supercritical. For both equations, we present new selfsimilar solutions with nontrivial profiles, which are completely explicit in all supercritical dimensions. Furthermore, we analyse their stability locally in backward light cones without symmetry assumptions. This involves a delicate spectral problem that we are able to solve rigorously only in particular space dimensions. In these cases, we prove that the solutions are codimension one stable modulo translations in a backward light cone of the blowup point. This is joint work with Irfan Glogić (Vienna) and Elek Csobo (Innsbruck).

11:30 am  12:15 pm ESTThe stability of charged black holes11th Floor Lecture Hall
 Virtual Speaker
 Elena Giorgi, Columbia University
Abstract
Black hole solutions in General Relativity are parametrized by their mass, spin and charge. In this talk, I will motivate why the charge of black holes adds interesting dynamics to solutions of the Einstein equation thanks to the interaction between gravitational and electromagnetic radiation. Such radiations are solutions of a system of coupled wave equations with a symmetric structure which allows to define a combined energymomentum tensor for the system. Finally, I will show how this physicalspace approach is resolutive in the most general case of KerrNewman black hole, where the interaction between the radiations prevents the separability in modes.

12:30  2:00 pm ESTLunch/Free Time

2:00  2:45 pm ESTInvariance of the Gibbs measures for the periodic generalized KdV equations11th Floor Lecture Hall
 Virtual Speaker
 Andreia Chapouto, UCLA
Abstract
In this talk, we consider the periodic generalized Kortewegde Vries equations (gKdV). In particular, we study gKdV with the Gibbs measure initial data. The main difficulty lies in constructing localintime dynamics in the support of the measure. Since gKdV is analytically illposed in the L2based Sobolev support, we instead prove deterministic local wellposedness in some FourierLebesgue spaces containing the support of the Gibbs measure. New key ingredients are bilinear and trilinear Strichartz estimates adapted to the FourierLebesgue setting. Once we construct localintime dynamics, we apply Bourgain's invariant measure argument to prove almost sure global wellposedness of the defocusing gKdV and invariance of the Gibbs measure. Our result completes the program initiated by Bourgain (1994) on the invariance of the Gibbs measures for periodic gKdV equations. This talk is based on joint work with Nobu Kishimoto (RIMS, University of Kyoto).

3:00  3:45 pm ESTGlobal in x Stability of Prandtl's Boundary Layer for 2D, Stationary NavierStokes Flows11th Floor Lecture Hall
 Virtual Speaker
 Sameer Iyer, UC Davis
Abstract
In this talk, I will discuss a recent work which proves stability of Prandtl's boundary layer in the vanishing viscosity limit. The result is an asymptotic stability result of the background profile in two senses: asymptotic as the viscosity tends to zero and asymptotic as x (which acts a time variable) goes to infinity. In particular, this confirms the lack of the "boundary layer separation" in certain regimes which have been predicted to be stable. This is joint work w. Nader Masmoudi (Courant Institute, NYU).

4:00  4:30 pm ESTCoffee Break11th Floor Collaborative Space
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Publications
 Yu Deng, Zaher Hani, Derivation of the wave kinetic equation: full range of scaling laws, arXiv preprint arXiv:2301.07063 (2023).
 Joseph K Miller, Andrea R Nahmod, Nata{\v{s}}a Pavlovi{\'c}, Matthew Rosenzweig, Gigliola Staffilani, A rigorous derivation of the Hamiltonian structure for the Vlasov equation, arXiv preprint arXiv:2206.07589 (2022).
 Yongji Wang, ChingYao Lai, Javier GómezSerrano, Tristan Buckmaster, Asymptotic selfsimilar blow up profile for 3D Euler via physicsinformed neural networks, arXiv:2201.06780, 2022.
 Yu Deng, Zaher Hani, Propagation of chaos and the higher order statistics in the wave kinetic theory, arXiv preprint arXiv:2110.04565 (2021).
 Louise Gassot, Zerodispersion limit for the BenjaminOno equation on the torus with single well initial data, arXiv preprint arXiv:2111.06800 (2021).
 Nicolas Camps, Louise Gassot, Pathological set of initial data for scalingsupercritical nonlinear Schr$\backslash$" odinger equations, arXiv preprint arXiv:2203.04840 (2022).