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計(jì)算機(jī)科學(xué)學(xué)院學(xué)術(shù)講座--Integrablepeakon and cuspon equations

發(fā)布時(shí)間:2015-06-08 瀏覽:

講座題目:計(jì)算機(jī)科學(xué)學(xué)院學(xué)術(shù)講座--Integrablepeakon and cuspon equations

講座人:喬志軍 教授

講座時(shí)間:09:00

講座日期:2015-6-6

地點(diǎn):長安校區(qū) 文津樓三段612室

主辦單位:計(jì)算機(jī)科學(xué)學(xué)院

講座內(nèi)容:In my talk, I will introduce integrablepeakon and cuspon equations and present a basic approach how to get peakon solutions. Those equations include the well-known Camassa-Holm (CH), the Degasperis-Procesi (DP), and other new peakon equations with M/W-shape soutions. I take the CH case as a typical example to explain the details. My presentation is based on my previous work (Communications in Mathematical Physics 239, 309-341). I will show that the Camassa-Holm (CH) spectral problem yields two different integrable hierarchies of nonlinear evolution equations (NLEEs), one is of negative order CH hierachy while the other one is of positive order CH hierarchy. The two CH hierarchies possess the zero curvature representations through solving a key matrix equation. We see that the well-known CH equation is included in the negative order CH hierarchy while the Dym type equation is included in the positive order CH hierarchy. In particular, the CH equation, constrained to a symplecticsubmanifold in R^2N, has the parametric solutions. Moreover, solving the parametric representation of the solution on the symplecticsubmanifold gives a class of a new algebro-geometric solution of the CH equation. In the end of my talk, some open problems are also addressed for discussion.

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