Asymptotic properties of nodes of solutions to Schrödinger equations. (English) Zbl 0699.35214
Partial differential equations, Proc. Symp., Holzhau/GDR 1988, Teubner- Texte Math. 112, 157-162 (1989).
[For the entire collection see Zbl 0665.00006.]
Real valued solutions \(\psi\) of Schrödinger equations \((-\Delta+V- E)\psi=0\) in a domain \(\Omega\subset\mathbb{R}^ n\), \(n\geq2\), are considered. Nodal properties of such solutions are studied under suitable assumptions on \(V\) and \(E\). Some theorems are proved, concerning the nodal set of \(\psi\) and the asymptotic behaviour of nodal lines.
Theorem 1 investigates various asymptotic properties of \(u=\psi/v\) (\(v\) is the solution of a radial comparison problem). Theorem 3 gives, under some assumptions, the asymptotic behaviour of the nodal lines.
Theorem 6: Let \(\psi\) satisfy: \(\Omega\subset\mathbb{R}^ n\) (\(n\geq2\)) a domain with \(x_0 \in \Omega\), \(V \in C^\infty (\Omega)\) and \(\psi\not\equiv0\), \(\psi \in C^\infty (\Omega)\) in \(\Omega\) and \(\psi(x_0)=0\), \(x_0=\mathcal O\), \(\displaystyle\lim_{r\to0-} r^{-M} \psi(ry) = Y_ M (y)\) \(\forall y\in S^{n-1}\), where \(Y_ M\) is a surface harmonic (\(M\geq1\)), \(y = x/r \in S^{n-1}\) (\(S^{n-1}\) the unit sphere in \(R^ n\)). Let \(D_{\varepsilon_0}\) denote a nodal domain of \(\psi\) with \(\mathcal O \in D_{\varepsilon_ 0}\), \(S(r) = \{y\in S^{n-1}\;| \;r_ y\in D_{\varepsilon_0}\}\), and denote \(\psi_0 = \left(\int_{S(r)} \psi^2 d\sigma\right)^{\frac{1}{2}}\) then \(\psi_0 r^{-M}\) and \(| S(r)|\) have for \(r\to0\) nonzero finite limits.
Real valued solutions \(\psi\) of Schrödinger equations \((-\Delta+V- E)\psi=0\) in a domain \(\Omega\subset\mathbb{R}^ n\), \(n\geq2\), are considered. Nodal properties of such solutions are studied under suitable assumptions on \(V\) and \(E\). Some theorems are proved, concerning the nodal set of \(\psi\) and the asymptotic behaviour of nodal lines.
Theorem 1 investigates various asymptotic properties of \(u=\psi/v\) (\(v\) is the solution of a radial comparison problem). Theorem 3 gives, under some assumptions, the asymptotic behaviour of the nodal lines.
Theorem 6: Let \(\psi\) satisfy: \(\Omega\subset\mathbb{R}^ n\) (\(n\geq2\)) a domain with \(x_0 \in \Omega\), \(V \in C^\infty (\Omega)\) and \(\psi\not\equiv0\), \(\psi \in C^\infty (\Omega)\) in \(\Omega\) and \(\psi(x_0)=0\), \(x_0=\mathcal O\), \(\displaystyle\lim_{r\to0-} r^{-M} \psi(ry) = Y_ M (y)\) \(\forall y\in S^{n-1}\), where \(Y_ M\) is a surface harmonic (\(M\geq1\)), \(y = x/r \in S^{n-1}\) (\(S^{n-1}\) the unit sphere in \(R^ n\)). Let \(D_{\varepsilon_0}\) denote a nodal domain of \(\psi\) with \(\mathcal O \in D_{\varepsilon_ 0}\), \(S(r) = \{y\in S^{n-1}\;| \;r_ y\in D_{\varepsilon_0}\}\), and denote \(\psi_0 = \left(\int_{S(r)} \psi^2 d\sigma\right)^{\frac{1}{2}}\) then \(\psi_0 r^{-M}\) and \(| S(r)|\) have for \(r\to0\) nonzero finite limits.
Reviewer: A.B.Borisov
MSC:
35Q99 | Partial differential equations of mathematical physics and other areas of application |
35B40 | Asymptotic behavior of solutions to PDEs |
81Q05 | Closed and approximate solutions to the Schrödinger, Dirac, Klein-Gordon and other equations of quantum mechanics |