Abstract
Abstract
We are concerned with the existence of multibump solutions to the nonlinear Schrödinger equation
−
Δ
u
+
λ
a
(
x
)
u
+
μ
u
=
|
u
|
2
σ
u
in
R
N
with an L
2-constraint
‖
u
‖
L
2
(
R
N
)
2
=
ρ
in the L
2-subcritical case σ ∈ (0, 2/N) and the L
2-supercritical case σ ∈ (2/N, 2*/N), where the usual critical Sobolev exponent is 2* = +∞ if N = 1, 2 and 2* = 2N/(N − 2) if N ⩾ 3. Here
μ
∈
R
will arise as a Lagrange multiplier, and
0
⩽
a
∈
L
loc
∞
(
R
N
)
has a bottom int a
−1(0) composed of ℓ
0 (ℓ
0 ⩾ 1) connected components
{
Ω
i
}
i
=
1
ℓ
0
, where int a
−1(0) is the interior of the zero set
a
−
1
(
0
)
=
{
x
∈
R
N
|
a
(
x
)
=
0
}
of a. When ρ is fixed either large in the L
2-subcritical case or small in the L
2-supercritical case, we construct a ℓ-bump (1 ⩽ ℓ ⩽ ℓ
0) positive normalized solution which is localised at ℓ prescribed components
{
Ω
i
}
i
=
1
ℓ
for large λ. The asymptotic profile of the solution is also analysed through taking the limit as λ → +∞, and subsequently as ρ → +∞ in the L
2-subcritical case or ρ → 0+ in the L
2-supercritical case. In particular, we find ℓ-bump normalized solutions to the related Dirichlet problem
0\quad \text{for}\ i=1,\dots ,\ell .\hfill \end{aligned}\right.\end{equation*}?>
−
Δ
v
+
μ
v
=
|
v
|
2
σ
v
,
v
∈
H
0
1
(
∪
i
=
1
ℓ
Ω
i
)
,
∑
i
=
1
ℓ
∫
Ω
i
v
2
=
ρ
,
v
|
Ω
i
>
0
for
i
=
1
,
…
,
ℓ
.
Funder
China Postdoctoral Science Foundation
National Natural Science Foundation of China
Subject
Applied Mathematics,General Physics and Astronomy,Mathematical Physics,Statistical and Nonlinear Physics
Cited by
8 articles.
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