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Symmetry breaking for ground states of biharmonic NLS via Fourier extension estimates
We consider ground state solutions u ∈ H 2 (ℝ N ) of biharmonic (fourth-order) nonlinear Schrödinger equations of the form Δ 2 u + 2 a Δ u + b u − ∣ u ∣ p − 2 u = 0 in ℝ N with positive constants a, b > 0 and exponents 2 < p < 2*, where 2 ∗ = 2 N N − 4 if N > 4 and 2* = ∞ if N ≤ 4. By ex...
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Published in: | Journal d'analyse mathématique (Jerusalem) 2024, Vol.152 (2), p.777-800 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We consider ground state solutions
u
∈
H
2
(ℝ
N
) of biharmonic (fourth-order) nonlinear Schrödinger equations of the form
Δ
2
u
+
2
a
Δ
u
+
b
u
−
∣
u
∣
p
−
2
u
=
0
in
ℝ
N
with positive constants
a, b
> 0 and exponents 2 <
p
< 2*, where
2
∗
=
2
N
N
−
4
if
N
> 4 and 2* = ∞ if
N
≤ 4. By exploiting a connection to the adjoint Stein–Tomas inequality on the unit sphere and by using trial functions due to Knapp, we prove a general symmetry breaking result by showing that all ground states
u
∈
H
2
(ℝ
N
) in dimension
N
≥ 2 fail to be radially symmetric for all exponents
2
<
p
<
2
N
+
2
N
−
1
in a suitable regime of
a, b
> 0.
As applications of our main result, we also prove symmetry breaking for a minimization problem with constrained
L
2
-mass and for a related problem on the unit ball in ℝ
N
subject to Dirichlet boundary conditions. |
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ISSN: | 0021-7670 1565-8538 |
DOI: | 10.1007/s11854-023-0311-2 |