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SUMMARY:Mark Fels
DTSTART:20230510T162000Z
DTEND:20230510T180000Z
DTSTAMP:20260423T023042Z
UID:GDEq/88
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/GDEq/88/">Va
 riational/Symplectic and Hamiltonian Operators</a>\nby Mark Fels as part o
 f Geometry of differential equations seminar\n\n\nAbstract\nGiven a differ
 ential equation (or system) $\\Delta$ = 0 the inverse problem in the calcu
 lus of variations asks if there is a multiplier function $Q$ such that\n\\
 [Q\\Delta=E(L)\,\\]\nwhere $E(L)=0$ is the Euler-Lagrange equation for a L
 agrangian $L$. A solution to this problem can be found in principle and ex
 pressed in terms of invariants of the equation $\\Delta$. The variational 
 operator problem asks the same question but $Q$ can now be a differential 
 operator as the following simple example demonstrates for the evolution eq
 uation $u_t - u_{xxx} = 0$\,\n\\[D_x(u_t - u_{xxx}) = u_{tx}-u_{xxxx}=E(-\
 \frac12(u_tu_x+u_{xx}^2)).\\]\nHere $D_x$ is a variational operator for $u
 _t - u_{xxx} = 0$.\n\nThis talk will discuss how the variational operator 
 problem can be solved in the case of scalar evolution equations and how va
 riational operators are related to symplectic and Hamiltonian operators.\n
LOCATION:https://researchseminars.org/talk/GDEq/88/
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