DOI: 10.68381/jca09009 ISSN: 0944-6532

Lagrangian Manifolds, Viscosity Solutions and Maslov Index

David McCaffrey, S. P. Banks

Let

M M
be a Lagrangian manifold, let the 1-form
pdx p d x
be globally exact on
M M
and let
S(x,p) S ( x , p )
be defined by
dS=pdx d S = p d x
on
M. M .
Let
H(x,p) H ( x , p )
be convex in
p p
for all
x x
and vanish on
M M
. Let
V(x)=\inf \{S(x,p):p V ( x ) = inf ⁡ { S ( x , p ) : p
such that
(x,p)\in M\} ( x , p ) ∈ M }
. Recent work in the literature has shown that (i)
V V
is a viscosity solution of
H(x,\partial V/\partial x)=0 H ( x , ∂ V / ∂ x ) = 0
provided
V V
is locally Lipschitz, and (ii)
V V
is locally Lipschitz outside the set of caustic points for
M M
. It is well known that this construction gives a viscosity solution for finite time variational problems – the Lipschitz continuity of
V V
follows from that of the initial condition for the variational problem. However, this construction also applies to infinite time variational problems and stationary Hamilton-Jacobi-Bellman equations where the regularity of
V V
is not obvious. We show that for dim
\,M\leq   M ≤
5, the local Lipschitz property follows from some geometrical assumptions on
M M
– in particular that the Maslov index vanishes on closed curves on
M. M .
We obtain a local Lipschitz constant for
V V
which is some uniform power of a local bound on
M M
, the power being determined by dim
M. M .
This analysis uses Arnold's classification of Lagrangian singularities