BEGIN:VCALENDAR
VERSION:2.0
PRODID:-//jEvents 2.0 for Joomla//EN
CALSCALE:GREGORIAN
METHOD:PUBLISH
BEGIN:VTIMEZONE
TZID:America/New_York
BEGIN:STANDARD
DTSTART:20211107T010000
RDATE:20220313T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20221106T010000
RDATE:20230312T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20231105T010000
RDATE:20240310T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20241103T010000
RDATE:20250309T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20251102T010000
RDATE:20260308T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20261101T010000
RDATE:20270314T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20271107T010000
RDATE:20280312T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:STANDARD
DTSTART:20281105T010000
RDATE:20290311T030000
TZOFFSETFROM:-0400
TZOFFSETTO:-0500
TZNAME:America/New_York EST
END:STANDARD
BEGIN:DAYLIGHT
DTSTART:20210331T121000
RDATE:20211107T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20220313T030000
RDATE:20221106T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20230312T030000
RDATE:20231105T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20240310T030000
RDATE:20241103T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20250309T030000
RDATE:20251102T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20260308T030000
RDATE:20261101T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20270314T030000
RDATE:20271107T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
BEGIN:DAYLIGHT
DTSTART:20280312T030000
RDATE:20281105T010000
TZOFFSETFROM:-0500
TZOFFSETTO:-0400
TZNAME:America/New_York EDT
END:DAYLIGHT
END:VTIMEZONE
BEGIN:VEVENT
UID:019a57c39f28908397fac6b411125714
CATEGORIES:Lie Group Quantum Mathematics Seminar
CREATED:20220323T093546
SUMMARY:General Relativity and Integrability
LOCATION:Zoom
DESCRIPTION:Abstract: A remarkable fact about general relativity is that it admits many
  exact solutions.  This fact can be explained (at least in many cases) by t
 he fact that the dimensional reduction of general relativity to two spaceti
 me dimensions is an integrable system.   The 2d theory has an infinite dime
 nsional hidden symmetry called the Geroch group that underlies its integrab
 ility.  I will review this story and then describe a new exact solution for
  gravitational pulse wave scattering.  The pulses maintain their shapes aft
 er scattering, as in ordinary soliton scattering.  In the last part of the 
 talk, I will describe evidence for a further symmetry enhancement in one di
 mension.   This enhanced symmetry is apparently a hyperbolic Kac-Moody alge
 bra, which is an interesting and mysterious mathematical object in its own 
 right.\n
X-ALT-DESC;FMTTYPE=text/html:<p>Abstract: A remarkable fact about general relativity is that it admits m
 any exact solutions.&nbsp; This fact can be explained (at least in many cas
 es) by the fact that the dimensional reduction of general relativity to two
  spacetime dimensions is an integrable system.&nbsp;&nbsp; The 2d theory ha
 s an infinite dimensional hidden symmetry called the Geroch group that unde
 rlies its integrability.&nbsp; I will review this story and then describe a
  new exact solution for gravitational pulse wave scattering.&nbsp; The puls
 es maintain their shapes after scattering, as in ordinary soliton scatterin
 g.&nbsp; In the last part of the talk, I will describe evidence for a furth
 er symmetry enhancement in one dimension.&nbsp;&nbsp; This enhanced symmetr
 y is apparently a hyperbolic Kac-Moody algebra, which is an interesting and
  mysterious mathematical object in its own right.</p>
CONTACT:Robert Penna, Institute for Advanced Study, School of Natural Sciences
X-EXTRAINFO:Zoom link https://rutgers.zoom.us/j/93921465287\nMeeting ID: 939 2146 5287\
 nPasscode: 196884, the dimension of the weight 2 homogeneous \nsubspace of 
 the moonshine module
DTSTAMP:20260828T210332
DTSTART;TZID=America/New_York:20220401T121000
DTEND;TZID=America/New_York:20220401T131000
SEQUENCE:0
TRANSP:OPAQUE
END:VEVENT
END:VCALENDAR