Vitolo R. Hamiltonian formalism for general PDEs, talk at Conf. Nonlinear Physics. Theory and Experiment. VI (Gallipoli, Italy), 23 June - 3 July, 2010 (abstract): Difference between revisions
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| title = Hamiltonian formalism for general PDEs | | title = Hamiltonian formalism for general PDEs | ||
| abstract = We will discuss the following question: What happens to a Hamiltonian operator of an evolution system if we change coordinates so that the system becomes non-evolution? As an answer to this question we will develop a geometric theory of Hamiltonian operators, and illustrate it through examples. | | abstract = We will discuss the following question: What happens to a Hamiltonian operator of an evolution system if we change coordinates so that the system becomes non-evolution? As an answer to this question we will develop a geometric theory of Hamiltonian operators, and illustrate it through examples. | ||
| slides = [[Media:Kersten_P.%2C_Krasil%27shchik_J.%2C_Verbovetsky_A.%2C_Vitolo_R._Hamiltonian_structures_for_general_PDEs_%28presentation_at_Conf._Nonlinear_Physics._Theory_and_Experiment._VI%2C_23_June_-_3_July%2C_2010%2C_Gallipoli%2C_Italy%29.pdf]] | | slides = [[Media:Kersten_P.%2C_Krasil%27shchik_J.%2C_Verbovetsky_A.%2C_Vitolo_R._Hamiltonian_structures_for_general_PDEs_%28presentation_at_Conf._Nonlinear_Physics._Theory_and_Experiment._VI%2C_23_June_-_3_July%2C_2010%2C_Gallipoli%2C_Italy%29.pdf|Kersten P., Krasil'shchik J., Verbovetsky A., Vitolo R. Hamiltonian structures for general PDEs (presentation at Conf. Nonlinear Physics. Theory and Experiment. VI, 23 June - 3 July, 2010, Gallipoli, Italy).pdf ]] | ||
| references = | | references = | ||
| 79YY-MM-DD = 7989-93-75 | | 79YY-MM-DD = 7989-93-75 | ||
}} | }} | ||
Revision as of 13:20, 3 July 2010
Speaker: Raffaele Vitolo
Title: Hamiltonian formalism for general PDEs
Abstract:
We will discuss the following question: What happens to a Hamiltonian operator of an evolution system if we change coordinates so that the system becomes non-evolution? As an answer to this question we will develop a geometric theory of Hamiltonian operators, and illustrate it through examples.