Popowicz Z. Generalized Peakon's equations, talk at The Workshop on Geometry of PDEs and Integrability, 14-18 October 2013, Teplice nad Becvou, Czech Republic (abstract): Difference between revisions
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{{MeetingTalk | {{MeetingTalk | ||
| speaker = Ziemowit Popowicz | | speaker = Ziemowit Popowicz | ||
| title = Generalized | | title = Generalized peakon equations | ||
| abstract = New Lax representation which generates the four component system of equations will be discussed. The Bi-Hamiltonian structure and conserved quantities of this system will be discussed. Under the special reduction our system is reduced to the twocomponent Qiao or Novikow equation which later could be reduced to the Comassa-Holm or Degasperis-Procesi equations. | | abstract = New Lax representation which generates the four component system of equations will be discussed. The Bi-Hamiltonian structure and conserved quantities of this system will be discussed. Under the special reduction our system is reduced to the twocomponent Qiao or Novikow equation which later could be reduced to the Comassa-Holm or Degasperis-Procesi equations. | ||
| slides = [[Media:Popowicz Z. Generalized Peakon's equations (presentation at The Workshop on Geometry of PDEs and Integrability, 14-18 October 2013, Teplice nad Becvou, Czech Republic).pdf|Popowicz Z. Generalized Peakon's equations (presentation at The Workshop on Geometry of PDEs and Integrability, 14-18 October 2013, Teplice nad Becvou, Czech Republic).pdf]] | | slides = [[Media:Popowicz Z. Generalized Peakon's equations (presentation at The Workshop on Geometry of PDEs and Integrability, 14-18 October 2013, Teplice nad Becvou, Czech Republic).pdf|Popowicz Z. Generalized Peakon's equations (presentation at The Workshop on Geometry of PDEs and Integrability, 14-18 October 2013, Teplice nad Becvou, Czech Republic).pdf]] | ||
Latest revision as of 05:21, 1 September 2015
Speaker: Ziemowit Popowicz
Title: Generalized peakon equations
Abstract:
New Lax representation which generates the four component system of equations will be discussed. The Bi-Hamiltonian structure and conserved quantities of this system will be discussed. Under the special reduction our system is reduced to the twocomponent Qiao or Novikow equation which later could be reduced to the Comassa-Holm or Degasperis-Procesi equations.