Seminar talk, 13 February 2014: Difference between revisions
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We restrict our consideration on simplest case associated with <math>2\times 2</math> zero curvature representation. | We restrict our consideration on simplest case associated with <math>2\times 2</math> zero curvature representation. | ||
| slides = | | slides = [[Media:Pavlov_M._Integrable_dispersive_chains_(presentation,_2014).pdf|Pavlov M. Integrable dispersive chains (presentation, 2014).pdf]] | ||
| references = Pavlov M.V. Integrable Dispersive Chains and Energy Dependent Schrodinger Operator, {{arXiv|1402.3836}} | | references = Pavlov M.V. Integrable Dispersive Chains and Energy Dependent Schrodinger Operator, {{arXiv|1402.3836}} | ||
| 79YY-MM-DD = 7985-97-86 | | 79YY-MM-DD = 7985-97-86 | ||
}} | }} | ||
Latest revision as of 18:12, 21 February 2014
Speaker: Maxim Pavlov
Title: Integrable dispersive chains
Abstract:
We construct a new object in the theory of integrable systems - integrable dispersive chains, which contain infinitely many multi-component integrable systems.
We restrict our consideration on simplest case associated with zero curvature representation.
Slides: Pavlov M. Integrable dispersive chains (presentation, 2014).pdf
References:
Pavlov M.V. Integrable Dispersive Chains and Energy Dependent Schrodinger Operator, arXiv:1402.3836
