Abstract
In this paper, we consider the locations of spikes of ground states for the following nonlinear Schrödinger system with three wave interaction
as \(\varepsilon \rightarrow +0\). In addition, we study the asymptotic behavior of a quantity \(\inf _{x \in {\mathbb {R}}^N} {\tilde{c}}({{\textbf{V}}}(x);\gamma )\) as \(\gamma \rightarrow \infty \) which determines locations of spikes. In particular, we give the sharp asymptotic behavior of a ground states of (\({{\mathcal {P}}}_\varepsilon \)) for \(\gamma \) sufficiently large and small, respectively. Furthermore, we consider when all the ground states of (\({{\mathcal {P}}}_\varepsilon \)) are scalar or vector.
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Acknowledgements
This work was supported by JSPS KAKENHI Grant Number JP23KJ0293. The author would like to thank Professor Kazuhiro Kurata for his useful advices on the structure of this paper. He also would like to thank Professor Yohei Sato for his helpful comments. He also would like to thank the referees for carefully reading his manuscript and for giving many useful comments.
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Appendix
Appendix
In this Appendix, we consider the radial symmetry and monotonicity of classical solutions of elliptic system of the following type:
where \(k \ge 1\).
Busca-Sirakov [5] studied the radial symmetry and monotonicity of classical solutions of elliptic systems for \(N \ge 2\). Moreover, Ikoma [16] considered the symmetry and monotonicity of the solutions in the case \(N=1\) and \(k=2\).
Here, we show the symmetry result for \(N=1\) after slight modification.
Let us note \({{\textbf{u}}} = (u_1,\dots ,u_k) \in (0,\infty )^k\) and
We suppose that \(f_i \in C^1({\mathbb {R}} \times (0,\infty )^k,{\mathbb {R}})\) for all \(i=1,\dots ,k\) and (A0)–(A4):
-
(A0)
\(f_i(-x,{{\textbf{u}}}) = f_i(x,{{\textbf{u}}})\) for all \(x \in {\mathbb {R}}\), \({{\textbf{u}}} \in (0,\infty )^k\) and \(i=1,\dots ,k\).
-
(A1)
\((\partial f_i/\partial x)(x,{{\textbf{u}}}) \le 0\) for all \(x \ge 0\), \({{\textbf{u}}} \in (0,\infty )^k\) and \(i=1,\dots ,k\).
-
(A2)
\((\partial f_i / \partial u_j)(x,{{\textbf{u}}}) \ge 0\) for all \(x \in {\mathbb {R}}\), \({{\textbf{u}}} \in (0,\infty )^k\) and \(i,j \in \{1,\dots ,k\},\ i \ne j\).
-
(A3)
there exist constants \(\varepsilon > 0\) and \(R_1 > 0\) such that for any \(I,J \subset \{1,\dots ,k\}\), \(I \cap J = \emptyset \), \(I \cup J = \{1,\dots ,k\}\), there exist \(i_0 \in I\) and \(j_0 \in J\) such that \((\partial f_{i_0} / \partial u_{j_0})(x,{{\textbf{u}}}) > 0\) for all \((x,{{\textbf{u}}}) \in {{\mathcal {O}}}\), where
$$\begin{aligned} {{\mathcal {O}}} = \{(x,{{\textbf{u}}}) \in {\mathbb {R}} \times (0,\infty )^k \mid \left|x\right| > R_1,\ \left|{{\textbf{u}}}\right| < \varepsilon \}. \end{aligned}$$ -
(A4)
all k-principal minors of \(-A(x,u_1,\dots ,u_k)\) have positive determinants, for all \((x,{{\textbf{u}}}) \in {{\mathcal {O}}}\), \(1 \le i \le k\). We recall that the k-principal minors of a matrix \((m_{ij})_{1 \le i,j \le k}\) are the submatrices \((m_{ij})_{1 \le i,j \le k'}\) with \(1 \le k' \le k\).
Theorem 5.1
Suppose \(f_1,\dots ,f_k\) satisfy (A0)–(A4), and \({{\textbf{u}}} = (u_1,\dots ,u_k)\) is a classical solution of (5.1). Then there exists a point \(y_0 \in {\mathbb {R}}\) such that the functions \(u_i\) are radially symmetric with respect to the origin \(y_0\), that is \(u_i(x) = u_i(\left|x - y_0\right|)\), \(i=1,\dots ,k\). Moreover,
For \(\lambda \in {\mathbb {R}}\), set \(\Sigma _\lambda := (\lambda ,\infty )\) and for \(x \in \Sigma _\lambda \), we define
Outline of the proof of Theorem 5.1
We define
Since \(u_i(x) \rightarrow 0\) as \(\left|x\right| \rightarrow \infty \), there exists \(R_0 \ge R_1\) such that \(u_i(x) < \varepsilon /\sqrt{k}\) if \(\left|x\right| \ge R_0\) for all \(i=1,\dots ,k\). We take \(\lambda ^* > R_0\), for which
for all \(\lambda > \lambda ^*\). Hence \(U_i^\lambda > 0\) in \([2 \lambda - R_0, 2 \lambda + R_0] \subset \Sigma _\lambda \) for all \(\lambda > \lambda ^*\). We notice that the functions \(U_i^\lambda \) satisfy the following system
where \(\mathbf {\eta } = \mathbf {\eta }(x,\lambda ) \in (0,\infty )^{k+1}\) and
Since \(\left|x^\lambda \right| < x\) for \(x \in \Sigma _\lambda \), we obtain from (A1) the following systems of inequality for \(U_i^\lambda \)
We want to show that \(U_i^\lambda \ge 0\) in \(\Sigma _\lambda \), for all \(\lambda > \lambda ^*\). We argue by contradiction. Suppose there exist \(\lambda > \lambda ^*\) and \(i_0 \in \{1,\dots ,k\}\) such that \(\inf _{\Sigma _\lambda } U_{i_0}^\lambda < 0\). We set \(J = \{j \mid U_j^\lambda \ge 0\ \text { in }\ \Sigma _\lambda \}\), and \(I = \{1,\dots ,k\} {\setminus } J\) (note that \(i_0 \in I\)).
Since all k-principal minors of \(- A(x,{{\textbf{u}}})\) have positive determinants, for all \((x,{{\textbf{u}}}) \in {{\mathcal {O}}}\), we do not need to introduce a function g as in [5]. Note the following lemma stated as Lemma 2.2 in [13].
Lemma 5.2
Let \(M = (m_{ij})_{1 \le i,j \le k}\) be a matrix such that \(m_{ij} \le 0\) for \(i \ne j\). Assume all k-principal minors of M have positive determinants. Then
-
(i)
all minors of M obtained by dropping lines and columns of the same order have positive determinants.
-
(ii)
if \(M_{ij}\) is the minor of M obtained by dropping the i th line and j th column we have \((-1)^{i+j} \det M_{ij} \ge 0\).
Hence we may assume \(I = \{1,\dots ,p\}\). Since \(U_j^\lambda \ge 0\) in \(\Sigma _\lambda \) for \(j \in J\), from (A2) and (5.2), we have
Since \(\inf _{\Sigma _\lambda } U_i^\lambda < 0\) for all \(i=1,\dots ,p\), \(U_i^\lambda > 0\) in \([2 \lambda - R_0, 2 \lambda + R_0]\), \(U_i^\lambda (\lambda ) = 0\) and \(U_i^\lambda (x) \rightarrow 0\) as \(\left|x\right| \rightarrow \infty \), there exist \(x_1,\dots ,x_p \in \Sigma _\lambda {\setminus } [2 \lambda - R_0, 2 \lambda + R_0]\) such that \(U_i^\lambda (x_i) = \min _{\Sigma _\lambda } U_i^\lambda < 0\). Then \((U_i^\lambda )''(x_i) \ge 0\) and \((U_i^\lambda )'(x_i) = 0\). Substituting \(x=x_i\) at i-th equation and using the fact that \(U_j^\lambda (x_j) \le U_j^\lambda (x_i)\), we have
(5.3) can be written as
where
Since \(x_i \not \in [2 \lambda - R_0, 2 \lambda + R_0]\), then \(x_i^\lambda \not \in [-R_0, R_0]\), that is, \(\left|x_i^\lambda \right| > R_0\). Noting that \(x_i > R_0\), we have \(u_j(x_i),u_j(x_i^\lambda ) < \varepsilon /\sqrt{k}\). Thus we have \(\xi _{i1}(x_i,\lambda )^2 + \dots + \xi _{ik}(x_i,\lambda )^2 < \varepsilon ^2\). From (A2) and (A4), we have \(m_{ij} \le 0\) for \(i \ne j\), and all p-principal minors of M have positive determinants. Since \(\det M > 0\), it follows that \({{\textbf{U}}} = M^{-1} Y\). From Lemma 5.2, \(U_i^\lambda (x_i) \ge 0\) for all \(i=1,\dots ,p\). This contradicts the fact that \(U_i(x_i) < 0\). Hence \(\Lambda < \infty \).
The rest of the proof of Theorem 5.1 can be showed by the same argument as in [5]. \(\square \)
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Osada, Y. A singular perturbation problem for a nonlinear Schrödinger system with three wave interaction. Nonlinear Differ. Equ. Appl. 31, 7 (2024). https://doi.org/10.1007/s00030-023-00901-8
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DOI: https://doi.org/10.1007/s00030-023-00901-8
Keywords
- Singular perturbation
- Nonlinear Schrödinger system
- Three wave interaction
- Asymptotic behavior
- Concentration of ground states