On the energy transfer to high frequencies in the damped/driven nonlinear Schrödinger equation
We consider a damped/driven nonlinear Schrödinger equation in R n , where n is arbitrary, E u t - ν Δ u + i | u | 2 u = ν η ( t , x ) , ν > 0 , under odd periodic boundary conditions. Here η ( t , x ) is a random force which is white in time and smooth in space. It is known that the Sobolev norms...
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Published in | Stochastic partial differential equations : analysis and computations Vol. 9; no. 4; pp. 867 - 891 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
New York
Springer US
01.12.2021
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | We consider a damped/driven nonlinear Schrödinger equation in
R
n
, where
n
is arbitrary,
E
u
t
-
ν
Δ
u
+
i
|
u
|
2
u
=
ν
η
(
t
,
x
)
,
ν
>
0
,
under odd periodic boundary conditions. Here
η
(
t
,
x
)
is a random force which is white in time and smooth in space. It is known that the Sobolev norms of solutions satisfy
‖
u
(
t
)
‖
m
2
≤
C
ν
-
m
,
uniformly in
t
≥
0
and
ν
>
0
. In this work we prove that for small
ν
>
0
and any initial data, with large probability the Sobolev norms
‖
u
(
t
,
·
)
‖
m
with
m
>
2
become large at least to the order of
ν
-
κ
n
,
m
with
κ
n
,
m
>
0
, on time intervals of order
O
(
1
ν
)
. It proves that solutions of the equation develop short space-scale of order
ν
to a positive degree, and rigorously establishes the (direct) cascade of energy for the equation. |
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ISSN: | 2194-0401 2194-041X |
DOI: | 10.1007/s40072-020-00187-2 |