BEGIN:VCALENDAR
VERSION:2.0
PRODID:-//Sabre//Sabre VObject 4.6.1//EN
CALSCALE:GREGORIAN
BEGIN:VTIMEZONE
TZID:Europe/Zurich
X-LIC-LOCATION:Europe/Zurich
TZURL:http://tzurl.org/zoneinfo/Europe/Zurich
BEGIN:DAYLIGHT
TZOFFSETFROM:+0100
TZOFFSETTO:+0200
TZNAME:CEST
DTSTART:19810329T020000
RRULE:FREQ=YEARLY;BYMONTH=3;BYDAY=-1SU
END:DAYLIGHT
BEGIN:STANDARD
TZOFFSETFROM:+0200
TZOFFSETTO:+0100
TZNAME:CET
DTSTART:19961027T030000
RRULE:FREQ=YEARLY;BYMONTH=10;BYDAY=-1SU
END:STANDARD
END:VTIMEZONE
BEGIN:VEVENT
UID:news2119@dmi.unibas.ch
DTSTAMP;TZID=Europe/Zurich:20261106T102702
DTSTART;TZID=Europe/Zurich:20261120T120000
SUMMARY:Junior BZ Seminar in Analysis: Massimo Sorella (Uni Basel)
DESCRIPTION:The two-dimensional incompressible Euler equations is a PDE des
 cribing the evolution of an ideal incompressible fluid. In 1963\, Yudovich
  proved global existence and uniqueness in the class of solutions with bou
 nded vorticity. Since then\, considerable effort has been devoted to under
 standing solutions with lower regularity. In this talk\, we present an ini
 tiative to understand an AI-generated proof of a breakthrough result: non-
 uniqueness of physically realizable solutions to the two-dimensional Euler
  equations with vorticity in L^p\, for any fixed finite p. Here\, physical
  realizability means that the solutions arise as vanishing-viscosity limit
 s of solutions to the two-dimensional Navier–Stokes equations.
X-ALT-DESC:<p>The two-dimensional incompressible Euler equations is a PDE d
 escribing the evolution of an ideal incompressible fluid. In 1963\, Yudovi
 ch proved global existence and uniqueness in the class of solutions with b
 ounded vorticity. Since then\, considerable effort has been devoted to und
 erstanding solutions with lower regularity. In this talk\, we present an i
 nitiative to understand an AI-generated proof of a breakthrough result: no
 n-uniqueness of physically realizable solutions to the two-dimensional Eul
 er equations with vorticity in L^p\, for any fixed finite p. Here\, physic
 al realizability means that the solutions arise as vanishing-viscosity lim
 its of solutions to the two-dimensional Navier–Stokes equations.</p>
DTEND;TZID=Europe/Zurich:20261120T122500
END:VEVENT
END:VCALENDAR