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SUMMARY:Konstantin Druzhkov
DTSTART:20240501T162000Z
DTEND:20240501T180000Z
DTSTAMP:20260423T022917Z
UID:GDEq/111
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/GDEq/111/">I
 nternal Lagrangians and gauge systems</a>\nby Konstantin Druzhkov as part 
 of Geometry of differential equations seminar\n\n\nAbstract\nIn classical 
 mechanics\, the Hamiltonian formalism is given in terms of instantaneous p
 hase spaces of mechanical systems. This explains why it can be interpreted
  as an encapsulation of the Lagrangian formalism into the intrinsic geomet
 ry of equations of motion. This observation can be generalized to the case
  of arbitrary variational equations. To do this\, we describe instantaneou
 s phase spaces using the intrinsic geometry of PDEs. The description is gi
 ven by the lifts of involutive codim-1 distributions from the base of a di
 fferential equation viewed as a bundle with a flat connection (Cartan dist
 ribution). Such lifts can be considered differential equations\, which one
  can regard as gauge systems. They encode instantaneous phase spaces. In a
 ddition\, each Lagrangian of a variational system generates a unique eleme
 nt of a certain cohomology of the system. We call such elements internal L
 agrangians. Internal Lagrangians can be varied within classes of paths in 
 the instantaneous phase spaces. This fact yields a direct (non-covariant) 
 reformulation of the Hamiltonian formalism in terms of the intrinsic geome
 try of PDEs. Finally\, the non-covariant internal variational principle gi
 ves rise to its covariant child.\n
LOCATION:https://researchseminars.org/talk/GDEq/111/
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