On the global well-posedness of focusing energy-critical inhomogeneous NLS
We consider the focusing energy-critical inhomogeneous nonlinear Schrödinger equation: i u t + Δ u + g | u | p - 1 u = 0 , u ( 0 ) = φ ∈ H ˙ 1 , where 0 ≤ g i ≤ | x | b g ≤ g s , 0 < b < 4 3 , and p = 5 - 2 b . On the road map of Kenig and Merle (Invent Math 166:645–675, 2006), we show the glo...
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Published in: | Journal of evolution equations Vol. 20; no. 4; pp. 1349 - 1380 |
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Main Authors: | , , |
Format: | Journal Article |
Language: | English |
Published: |
Cham
Springer International Publishing
01-12-2020
|
Subjects: | |
Online Access: | Get full text |
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Summary: | We consider the focusing energy-critical inhomogeneous nonlinear Schrödinger equation:
i
u
t
+
Δ
u
+
g
|
u
|
p
-
1
u
=
0
,
u
(
0
)
=
φ
∈
H
˙
1
,
where
0
≤
g
i
≤
|
x
|
b
g
≤
g
s
,
0
<
b
<
4
3
, and
p
=
5
-
2
b
. On the road map of Kenig and Merle (Invent Math 166:645–675, 2006), we show the global well-posedness and scattering of radial solutions under energy condition
E
g
(
φ
)
<
E
g
(
Q
b
)
,
and
g
s
1
p
0
‖
φ
‖
H
˙
1
2
<
‖
Q
b
‖
H
˙
1
2
,
where
Q
b
is the solution of
Δ
Q
b
+
|
x
|
-
b
Q
b
p
=
0
, together with scaling condition
|
x
|
|
∇
g
(
x
)
|
≲
|
x
|
-
b
, variational condition
g
s
2
p
-
1
(
p
+
1
2
-
g
i
)
≤
p
-
1
2
, and rigidity condition
-
b
g
(
x
)
≤
x
·
∇
g
(
x
)
. We also provide sharp finite time blow-up results for non-radial and radial solutions. For this, we utilize the localized virial identity. |
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ISSN: | 1424-3199 1424-3202 |
DOI: | 10.1007/s00028-020-00558-1 |