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