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Reverse Agmon Estimates in Forbidden Regions
Let ( M , g ) be a compact, Riemannian manifold and V ∈ C ∞ ( M ; R ) . Given a regular energy level E > min V , we consider L 2 -normalized eigenfunctions, u h , of the Schrödinger operator P ( h ) = - h 2 Δ g + V - E ( h ) with P ( h ) u h = 0 and E ( h ) = E + o ( 1 ) as h → 0 + . The well-kn...
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Published in: | Annales Henri Poincaré 2020, Vol.21 (1), p.303-325 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | Let (
M
,
g
) be a compact, Riemannian manifold and
V
∈
C
∞
(
M
;
R
)
. Given a regular energy level
E
>
min
V
, we consider
L
2
-normalized eigenfunctions,
u
h
,
of the Schrödinger operator
P
(
h
)
=
-
h
2
Δ
g
+
V
-
E
(
h
)
with
P
(
h
)
u
h
=
0
and
E
(
h
)
=
E
+
o
(
1
)
as
h
→
0
+
.
The well-known Agmon–Lithner estimates [
5
] are exponential decay estimates (i.e. upper bounds) for eigenfunctions in the forbidden region
{
V
>
E
}
.
The decay rate is given in terms of the Agmon distance function
d
E
associated with the degenerate Agmon metric
(
V
-
E
)
+
g
with support in the forbidden region. The point of this note is to prove a reverse Agmon estimate (i.e. exponential
lower
bound for the eigenfunctions) in terms of Agmon distance in the forbidden region under a control assumption on eigenfunction mass in the allowed region
{
V
<
E
}
arbitrarily close to the caustic
{
V
=
E
}
.
We then give some applications to hypersurface restriction bounds for eigenfunctions in the forbidden region along with corresponding nodal intersection estimates. |
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ISSN: | 1424-0637 1424-0661 |
DOI: | 10.1007/s00023-019-00867-3 |