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Discreteness of the spectrum of vectorial Schrödinger operators with δ-interactions
Boundary Value Problems volume 2016, Article number: 24 (2016)
Abstract
This paper deals with the vectorial Schrödinger operators with δ-interactions generated by \(L_{X,A,Q}:=-\frac{d^{2}}{dx^{2}} +Q(x)+\sum_{k=1}^{\infty}A_{k}\delta(x-x_{k})\), \(x\in[ 0,+\infty)\). First, we obtain an embedding inequality. Then using standard form methods, we prove that the operator \(\mathbf{H}_{X,A,Q}\) given in this paper is self-adjoint. Finally, a sufficient condition and a necessary condition are given for the spectrum of the operator \(\mathbf {H}_{X,A,Q}\) to be discrete. By giving additional restrictions on the symmetric potential matrix \(Q(x)\) and \(A_{k}\), we also give a necessary and sufficient condition for a special case. The conditions are analogous to Molchanov’s discreteness criteria.
1 Introduction
The present paper deals with the vectorial (matrix) Schrödinger operators with δ-interactions generated by the formal differential expression
where \(Q(x)=(q_{ij}(x))_{i,j=1}^{m}\in L_{\mathrm{loc}}^{1}(\mathbb {R}_{+},\mathbb{C} ^{m\times m})\) and \(A_{k}=(a_{i,j}^{k})_{i,j=1}^{m}\in\mathbb {R}^{m\times m} \) are real valued and symmetric \(m\times m\) matrices. Denote \(A:=\{A_{k}\}_{k=1}^{\infty}\subset\mathbb{R}^{m\times m}\), and let \(X:=\{x_{k}\}_{k=1}^{\infty}\subset\mathbb{R}_{+}\) be a strictly increasing sequence such that \(x_{k}\rightarrow+\infty\). The minimal operator \(\mathbf{H}_{X,A,Q}\) can be defined as follows:
Here θ is the m-dimensional zero vector. It is clear that \(\mathbf{ H}_{X,A,Q}^{0}\) is a symmetric operator, and the minimal operator \(\mathbf{H} _{X,A,Q}\) is the closure of \(\mathbf{H}_{X,A,Q}^{0}\) in \(L^{2}(\mathbb{R} _{+},\mathbb{C}^{m})\), that is, \(\mathbf{H}_{X,A,Q}:=\overline{\mathbf{H} _{X,A,Q}^{0}}\). \(L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\) is the Hilbert space of vector-valued functions with the scalar product
where \(u=(u_{1},u_{2},\ldots,u_{m})^{T}\), \(v=(v_{1},v_{2},\ldots,v_{m})^{T}\), \((u,v)_{m}:=\overline{v}^{T}u=\sum_{i=1}^{m}\overline{v_{i}}u_{i}\), \(u_{i},v_{i}\in L^{2}(\mathbb{R}_{+})\).
Schrödinger operators with δ-interactions can be used as solvable models in many situations. The operators \(\mathbf{H}_{X,A,Q}\) in the scalar case describes δ-interactions of strength at the points \(x_{k}\). Numerous results can be found in [1–5]. Also, there are some papers about a vectorial operator with δ-interactions. For example, a detailed spectral theoretic treatment of Schrödinger operators with distributional matrix-valued potentials is developed in [6]. Some results about the defect index of the matrix case \(\mathbf{H}_{X,A,Q}\) when Q is missing are obtained in [7]. However, there are a few results about the spectral properties of such operators.
The main objective of the present paper is to give conditions for the spectra of the vectorial Schrödinger operators \(\mathbf{H}_{X,A,Q}\) to be discrete. First, we prove that the operator \(\mathbf{H}_{X,A,Q}\) given in this paper is self-adjoint. If the singular part in (1.1) is missing, then \(\mathbf{H}_{Q}=\mathbf{H}_{X,0,Q}\) is just a classical vectorial Sturm-Liouville expression. Liu and Wang [8] gave some criterions that guarantee the operator \(\mathbf{H}_{Q}\) to have a purely discrete spectrum. This result was proved by direct sum decomposition methods of operators and estimation of the corresponding quadratic forms. Clark and Gesztesy [9] derived Povzner-Wienholtz-type self-adjointness results for the classical matrix Sturm-Liouville operators. A generalization of this result to the case of scalar (\(m=1\)) operators with point interactions was obtained by Albeverio et al. [1]. Second, after we derive an embedding inequality of vector-valued functions, we obtain some criterions that guarantee the operator \(\mathbf{H}_{X,A,Q}\) to have a purely discrete spectrum. The condition is an analog of the classical discreteness criterion due to Molchanov [10]. Our result reads as follows:
However, condition (1.3) is no longer necessary in the case of matrix Hamiltonians \(\mathbf{H}_{X,A,Q}\) (see Theorem 1). This results coincides with the corresponding result obtained by Albeverio et al. [1] in the scalar case (\(m=1\)), whereas in this case it is also necessary. Subsequently, giving additional restrictions on the symmetric potential matrix \(Q(x)\) and \(A_{k}\), we obtain a sufficient and necessary condition for a special case (see Theorem 3).
This paper is organized as follows. In Section 2, we introduce some basic definitions and lemmas and a generalized embedding theorem. Section 3 contains some lemmas and quadratic forms associated with the operator \(\mathbf{H}_{X,A,Q}\) for our main results. Some criterions based on the Molchanov’s theorem, which guarantee that the operator has a purely discrete spectrum, are given in Section 4.
2 Preliminaries
Let \(\mathfrak{H}\) be a Hilbert space with inner product \((\cdot,\cdot)\), and let t be a densely defined quadratic form in \(\mathfrak{H}\) with lower bound −c, that is, \(\mathbf{t}[u]\geqslant-c\| u\|_{ \mathfrak{H}}^{2}\), \(c\in\mathbb{R}\). Let \(\mathbf{t}[\cdot,\cdot]\) be the sesquilinear form associated with t. Then the equality
defines a scalar product on \(\operatorname{Dom}(\mathbf{t})\) such that \(\| u\|_{ \mathbf{t}}\geqslant\| u\|_{\mathfrak{H}}\) for all \(u\in \operatorname{Dom}( \mathbf{t})\), where
The form t is called closable if the norm \(\|\cdot\|_{ \mathbf{t}}\) is compatible with \(\|\cdot\|_{\mathfrak{H}}\), that is, for every \(\|\cdot\|_{\mathbf{t}}\)-Cauchy sequence \(\{u_{n}\}_{n=1}^{\infty}\) in \(\operatorname{Dom}(\mathbf{t})\), \(\| u_{n}\|_{ \mathfrak{H}}\rightarrow0\) implies \(\| u_{n}\|_{\mathbf{t} }\rightarrow0\). Let \(\mathfrak{H}_{\mathbf{t}}\) be the \(\|\cdot \|_{ \mathbf{t}}\)-completion of \(\operatorname{Dom}(\mathbf{t})\). In this case, the completion \(\mathfrak{H}_{\mathbf{t}}\) can be considered as a subset of \(\mathfrak{H}\). The form t is closed if the sets \(\mathfrak{H}_{\mathbf{t}}\) and \(\operatorname{Dom}(\mathbf{t})\) are equal. Let A be a self-adjoint lower semibounded operator in \(\mathfrak{H}\), that is, \((Au,u)\geqslant-c(u,u)\) for all \(u\in \operatorname{Dom}(A)\) and some \(c\in\mathbb{R}\). Denote by \(\mathbf{t}_{A}^{\prime }\) the densely defined quadratic form given by
Clearly, this form is closable and lower semibounded, \(\mathbf{t} _{A}^{\prime}\geqslant-c\), and its closure \(\mathbf{t}_{A}\) satisfies \(\mathbf{t}_{A}\geqslant-c\). We set \(\mathfrak{H}_{A}:=\mathfrak {H}_{\mathbf{t}_{A}}\). By the first representation theorem [11], Theorem 6.2.1, for any closed lower semibounded quadratic form \(\mathbf{t}\geqslant -c\) in \(\mathfrak{H}\), there corresponds a unique self-adjoint operator \(A=A^{\ast}\) in \(\mathfrak{H}\) satisfying \((Au,u)\geqslant-c(u,u)\) for all \(u\in \operatorname{Dom} (A)\) such that t is the closure of \(\mathbf{t}_{A}^{\prime}\). The form t is uniquely determined by the conditions \(\operatorname{Dom}(A)\subset \operatorname{Dom}(\mathbf{t})\) and
Lemma 1
Let \(A=A^{\ast}\) be a lower semibounded operator in \(\mathfrak{H}\), and let \(\mathbf{t}_{A}\) be the corresponding form. The spectrum \(\sigma(A)\) of the operator A is discrete if and only if the embedding \(i_{A}: \mathfrak{H}_{A}\hookrightarrow \mathfrak{H}\) is compact.
Proof
See [11]. □
Definition 1
Let the operator A be self-adjoint and positive on \(\mathfrak{H}\), and let \(\mathbf{t}_{A}\) be the corresponding form. The form t is called relatively form bounded with respect to \(\mathbf{t}_{A}\) (\(\mathbf{t}_{A}\)-bounded) if \(\operatorname{Dom}(\mathbf {t}_{A})\subset \operatorname{Dom}(\mathbf{t})\) and there are positive constants a, b such that
The infimum of all possible a is called the form bound of t with respect to \(\mathbf{t}_{A}\). If a can be chosen arbitrary small, then t is called infinitesimally form bounded with respect to \(\mathbf{t}_{A}\).
Lemma 2
Let \(\mathbf{t}_{A}\) be the form corresponding to the operator \(A=A^{\ast}>0\) in \(\mathfrak{H}\). If the form t is \(\mathbf{t}_{A}\)-bounded with relative bound \(a<1\), then the form
is closed and lower semibounded in \(\mathfrak{H}\) and hence gives rise to a self-adjoint semibounded operator. Moreover, the norms \(\|\cdot \| _{A} \) and \(\|\cdot\|_{\mathbf{t}_{1}}\) are equivalent.
Proof
See [12]. □
We also need a generalized embedding inequality of vector-valued functions, which we state here. In [13], p.232, Theorem A.2, Muller-Pfeiffer gave an embedding theorem for scalar functions. We extend the theorem to vectorial functions. For an interval I, let \(u(x)=(u_{1}(x),u_{2}(x),\ldots,u_{m}(x))^{T}\), where \(u_{j}\in W^{l,p}(I)\), \(j=1,2,\ldots,m\), and we denote by \(W^{l,p}(I,\mathbb{C}^{m})\) the space of all such vectorial functions. The norm is \(\Vert u\Vert _{W^{l,p}(I,\mathbb{C}^{m})}^{2}=\sum_{i=1}^{m}\Vert u_{i}\Vert _{W^{l,p}(I)}^{2}\), \(\Vert u_{i}\Vert _{W^{l,p}(I)}= ( \sum_{k=0}^{l}\int_{I}|u_{i}^{(k)}(x)|^{p}\,dx ) ^{1/p}\). If \(u_{j}\in C^{k}(I)\), \(j=1,2,\ldots,m\), then we denote by \(C^{k}(I,\mathbb {C}^{m})\) the space of all such vectorial functions. The norm is \(\Vert u\Vert _{C^{k}(I,\mathbb{C}^{m})}^{2}=\sum_{i=1}^{m}\Vert u_{i}\Vert _{C^{k}(I)}^{2}\), \(\Vert u_{i}\Vert _{C^{k}(I)}=\sum_{l=0}^{k}\sup_{x\in I}|u_{i}^{(l)}(x)|\). If \(u_{j}\in L^{k}(I)\), \(j=1,2,\ldots,m\), then we denote by \(L^{k}(I,\mathbb {C}^{m})\) the space of all such vectorial functions. The norm is \(\Vert u\Vert _{L^{k}(I,\mathbb{C}^{m})}^{2}=\sum_{i=1}^{m}\Vert u_{i}\Vert _{L^{k}(I)}^{2}\), \(\Vert u_{i}\Vert _{L^{k}(I)}= ( \int_{I}|u_{i}(x)|^{k} ) ^{1/k}\). We get the following embedding inequality for vectorial functions.
Lemma 3
If \(l>k\geq0\) and \(1< p<\infty\), \(W^{l,p}((x_{1},x_{2}),\mathbb{C}^{m})\) is continuously embedded into the space \(C^{k}((x_{1},x_{2}),\mathbb{C}^{m})\), and, for any \(\varepsilon>0\), there exists a constant \(C_{\varepsilon}\) such that
for all \(u\in W^{l,p}((x_{1},x_{2}),\mathbb{C}^{m})\).
Proof
Using the embedding theorem in [13], for any \(\varepsilon >0\) and every component function \(u_{i}\), \(i=1,2,\ldots,m\), there are constants \(C_{i,\varepsilon}>0\) such that
Then
where \(C_{\varepsilon}=\max_{1\leq i\leq m}\{C_{i,\varepsilon}\}\). For integer \(l>0\) and \(1< p<\infty\),
hence, we get (2.1). □
3 Quadratic forms associated with the operator
We begin this section with the operators \(\mathbf{H}_{X,A,Q}\) and their corresponding quadratic forms in the Hilbert space \(L^{2}(\mathbb{R}_{+}, \mathbb{C}^{m})\). First, we recall some notation for the convenience of the readers. The inequality \(Q(x)\geq(>)0\) means that for any \(Y(x)= (y_{1}(x),y_{2}(x), \ldots,y_{m}(x))^{T}\), \((Q(x)Y(x),Y(x))_{m}\geq(>)0\), and \(Q(x)\) is called bounded from below if \((Q(x)Y(x),Y(x))_{m}\geq-c(Y(x),Y(x))_{m}\), where c is a constant. Then we consider the quadratic forms
We denote by \(\mu_{\min}(Q(x))\) and \(\mu_{\max}(Q(x))\) respectively the minimal and maximal eigenvalues of \(Q(x)\), and by \(\mu_{\min}(A_{k})\) and \(\mu_{\max}(A_{k})\) respectively the minimal and maximal eigenvalues of \(A_{k}\). The quadratic form \(\mathfrak{q}[Y]\) is called semibounded from below (above) if and only if so is \(\mu_{\min}(Q(x))(\mu_{\max}(Q(x)))\). We denote by \(\mathbf{t}_{0}[Y]\) the following quadratic form:
Together with the form \(\mathfrak{q}\), we consider the form
\(\operatorname{Dom}(\mathbf{t}_{0}[Y])\) is the set of all \(Y\in L^{2}(\mathbb{R}_{+}, \mathbb{C}^{m})\) such that \(Y(x)\) is absolutely continuous, \(Y^{\prime }\in L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\), and \(Y(0)=\theta\). The form \(\mathbf{t}_{0}[Y]\) is symmetric and closed. \(\operatorname{Dom}(\mathfrak{q})\) is the set of all \(Y\in L^{2}( \mathbb{R}_{+},\mathbb{C}^{m})\) such that \(\int_{0}^{\infty }(Q(x)Y(x),Y(x))_{m}\,dx<+\infty\). The form \(\mathfrak{q}\) is also symmetric and closed. Thus, \(\mathbf{t}_{Q}[Y]=\mathbf{t}_{0}[Y]+\mathfrak{q}[Y]\) is symmetric and closed (see [11], Chapter VI, Theorem 1.31). If the potential \(Q(x)\) is lower semibounded with bound −c, that is, \((Q(x)Y,Y)\geq -c(Y,Y)\), \(\forall Y\in\mathbb{C}^{m}\), then \(\operatorname{Dom}(\mathbf{t}_{Q})\) equipped with the norm \(\| Y\|_{\mathfrak{H}_{Q}}^{2}:=\| Y\| _{W^{1,2}}^{2}+\mathbf{t}_{Q}[Y]+(1+c)\| Y\|_{\mathfrak{H}}^{2}\) is the Hilbert space \(\mathfrak{H}_{Q}:=\mathfrak{H}_{\mathbf{t} _{Q}}:=W_{0}^{1,2}(\mathbb{R}_{+},\mathbb{C}^{m};Q)\). Let
be defined on the domain
Denote by \(\mathbf{t}_{R}^{\pm}[Y]\) the sum of k positive (negative) parts of \((A_{k}Y(x_{k}),Y(x_{k}))_{m}\), that is,
Similarly,
Then we define the form
which is naturally associated with the differential expression, and the form is as follows:
Notation
If the form \(\mathbf{t}_{X,A,Q}\) is nonnegative, then \(\mathfrak{H}_{X,A,Q}:=\mathfrak{H}_{\mathbf{t}_{X,A,Q}}\) denotes the domain \(\operatorname{Dom}(\mathbf{t}_{X,A,Q})\) equipped with the norm
where \(\mu_{\max}^{\pm}(Q(x)):=(\mu_{\max}(Q(x))\pm|\mu_{\max }(Q(x))|)/2\), \(\mu(A)^{\pm}:=\{\mu(A_{k})^{\pm}\}_{1}^{\infty}\), and \(\mu_{\max}^{\pm}(A_{k}):=(\mu_{\max}(A_{k}) \pm|\mu_{\max }(A_{k})|)/2\).
Lemma 4
If the minimal operator \(\mathbf{H}_{\min}=\mathbf{H} _{X,A,Q}\) is lower semibounded, then the operator \(\mathbf{H}_{X,A,Q}\) is self-adjoint, \(\mathbf{H}_{X,A,Q}=(\mathbf{H}_{X,A,Q})^{\ast}\).
Proof
Without loss of generality, we assume that \(\mathbf{H}_{X,A,Q}\geqslant I\). It is sufficient to show that \(\ker((\mathbf{H}_{X,A,Q})^{\ast})=\{ \theta \}\), that is, the equation
has only a trivial solution (the derivative is understood in a distribution sense).
Assume the converse, that is, let \(Y(x)=(y_{1}(x),y_{2}(x),\ldots,y_{m}(x))^{T}\) be a solution of equation (3.8). Let \(\chi_{i}\in C_{0}^{\infty}(\mathbb{R}_{+},\mathbb{C} ^{m})\) (\(i=1,2,\ldots,m\)) be such that \(0 \leq \Vert \chi _{i}\Vert \leq1\) and
where \(\Vert \cdot \Vert \) is the Euclidean norm. Let the matrix \(X(x)\) be the combination of \(\chi_{i}(x)\), \(i=1,2,\ldots,m\), that is, \(X(x)=[\chi_{1}(x),\chi_{2}(x),\ldots,\chi_{m}(x)]\). Define
Obviously, \(\sup pY_{n}\subset[0,n]\). Since \(Y_{n}(x_{k}-)=Y_{n}(x_{k}+)\) and \(\chi_{i}\in C_{0}^{\infty}(\mathbb{R} _{+},\mathbb{C}^{m})\) (\(i=1,2,\ldots,m\)), we get
and hence \(Y_{n}\in \operatorname{Dom}(\mathbf{H}_{\min})\). Furthermore,
By \(\mathbf{H}_{X,A,Q}\geqslant I\),
On the other hand, transforming the first part of (3.9), integrating by parts, and noting that \(X_{n}(x)\) has a compact support, we get
where \(\chi_{i,i}(x/n)\) denotes the ith component function of \(\chi _{i}(x/n)\), which is the ith column of the matrix \(X_{n}(x)\) (\(i=1,2,\ldots,m\)). The second part of (3.9) is as follows:
By (3.9), (3.11), and (3.12) we get
Therefore, by (3.10) and (3.13) we obtain
where \(C:=\sup_{x\in[0,1]}|X^{\prime}(x)|\). Noting that \(Y\in L^{2}( \mathbb{R}_{+},\mathbb{C}^{m})\), inequality (3.14) yields \(Y=\theta\). This contradiction completes the proof. □
Before proceeding further, we need the following fact.
Lemma 5
If
then the forms \(\mathfrak{q}\) and \(\mathbf{t}_{R}:=\mathbf{t}_{R}^{+}+ \mathbf{t}_{R}^{-}\) are infinitesimally \(\mathbf{t}_{0}\)-bounded, and hence the form \(\mathbf{t}_{X,A,Q}\) is closed and lower semibounded, and \(\operatorname{Dom}(\mathbf{t}_{X,A,Q})= W^{1,2}(\mathbb{R}_{+},\mathbb{C}^{m})\) algebraically and topologically.
Proof
By Lemma 3, for any \(\varepsilon>0\), we have the following inequality:
where \(x\in[ n,n+1]\), and the constant \(C_{\varepsilon}>0\) does not depend on Y and \(n\in\mathbb{N}\). Combining (3.15) and (3.16) with (3.17), we obtain, for \(Y\in\operatorname{Dom} (\mathbf{t}_{0})=W_{0}^{1,2}(\mathbb{R} _{+},\mathbb{C}^{m})\),
Since \(\varepsilon>0\) is arbitrary, the forms \(\mathfrak{q}\) and \(\mathbf{t} _{R}\) are infinitesimally form bounded with respect to \(\mathbf {t}_{0}\). It remains to apply Lemma 2. □
We refer to \(A:=\{A_{k}\}_{k=1}^{\infty}\subset\mathbb{R}^{m\times m}\) again. We denote by \(l_{m}^{2}(\|A\|)\) the weighted space of m-dimensional vector sequences \(f=\{f_{k}\}_{k=1}^{\infty}\subset\mathbb{C}^{m}\), where \(\|A\|\) is any norm of a matrix A, and every element \(f_{k}\) of the sequence is an m-dimensional column vector. Let \(f_{k}=(f_{k,1},f_{k,2}, \ldots,f_{k,m})^{T}\); then \(\{f_{k,i}\}_{k=1}^{\infty}\in l^{2}\), \(i=1,2,\ldots,m\), and hence \(\|f_{k,i}\|^{2}=\sum_{k=1}^{\infty }|f_{k,i}|^{2}<\infty\) and \(\|f\|^{2}=\sum_{i=1}^{m}\|f_{k,i}\|^{2}\). The space \(l_{m}^{2}(\|A\|)\) equipped with the weighted norm \(\|f\|_{l_{m}^{2}(\|A\|)}=(\sum_{i=1}^{m}\sum_{k=1}^{ \infty}\|A_{k}\||f_{k,i}|^{2})^{\frac{1}{2}}\) is a Banach space.
Lemma 6
Assume that \(Q(x)\geq0\) and \(A_{k}\geq0\) for \(k=1,2,\ldots \) . Then the form \(\mathbf{t}_{X,A,Q}\) is nonnegative and closed.
Proof
It is obvious that the form \(\mathbf{t}_{X,A,Q}\) is nonegative if \(Q(x)\geq0\) and \(A_{k}\geq0\). Now we prove the closeness of the form \(\mathbf{t}_{X,A,Q}\). Let us equip \(\mathfrak{H}_{X,A,Q}= \operatorname{Dom}(\mathbf{t} _{X,A,Q})\) with the norm
Let \(\{Y_{n}\}_{n=1}^{\infty}\) be a Cauchy sequence in \(\mathfrak{H} _{X,A,Q} \). Since \(W_{0}^{1,2}(\mathbb{R}_{+},\mathbb{C}^{m})\) and \(l_{m}^{2}(\|A\|)\) are Hilbert spaces, there exist \(Y\in W_{0}^{1,2}(\mathbb{ R}_{+},\mathbb{C}^{m})\) and
such that
and
where \(\xi_{i}\) and \(Y_{n}\) are m-dimensional vectors. Since the space \(W_{0}^{1,2}(\mathbb{R}_{+},\mathbb{C}^{m})\) is continuously embedded into \(C( \mathbb{R}_{+},\mathbb{C}^{m})\), the Banach space of bounded continuous functions on \(\mathbb{R}_{+}\). Therefore,
and then \(Y\in\mathfrak{H}_{X,A,Q}\) and
In addition, since \(Q(x)\geq0\) and \(\{A_{k}\}_{k=1}^{\infty}\geq0\), \(\mathfrak{H}_{X,A,Q}\) is a Hilbert space with the inner product
where E is the identity matrix. Then the form \(\mathbf{t}_{X,A,Q}\) is closed. □
Lemma 7
If the form \(\mathbf{t}_{X,A,Q}\) is lower semibounded, then the set \(\operatorname{Dom}(H_{X,A,Q}^{0})\) is a core of the form \(\mathbf{t}_{X,A,Q}\).
Proof
We need to show that \(\operatorname{Dom}(H_{X,A,Q}^{0})\) is dense in \(\operatorname{Dom}(\mathbf{t} _{X,A,Q})\) with respect to the norm \(\| Y\|_{\mathfrak{H} _{X,A,Q}}^{2}=\mathbf{t}_{Q}[Y]+\mathbf{t}_{R}[Y]+\| Y\|_{L^{2}( \mathbb{R}_{+},\mathbb{C}^{m})}^{2}\). Let \(D_{\min}^{\prime}\) be the linear span of \(C^{\infty}\) functions with compact support in a single interval \((x_{i-1},x_{i})\), \(i\in\mathbb{N}\). Each function \(f_{i}\in C_{0}^{\infty}((x_{i-1},x_{i}),\mathbb{C}^{m})\) can be extended to \([0,\infty)\), and the extended function
belongs to \(D_{\min}^{\prime}\subset \operatorname{Dom}(H_{X,A,Q}^{0})\).
We need to prove that for \(u\in \operatorname{Dom}(\mathbf{t}_{X,A,Q})\) and for all \(f\in \operatorname{Dom}(H_{X,A,Q}^{0})\),
implies that \(u=0\). Equation (3.18) holds for all \(f\in \operatorname{Dom} (H _{X,A,Q}^{0})\), and thus, for each interval \((x_{i-1},x_{i})\), the equation
holds for all \(f_{i}\in C_{0}^{\infty}((x_{i-1},x_{i}),\mathbb{C}^{m})\). Then \(u^{\prime\prime}=(Q+E)u\) on each interval \((x_{i-1},x_{i})\) in the sense of distributions.
Since equation (3.18) holds for all \(f\in \operatorname{Dom}(H _{X,A,Q}^{0}) \), integrating by parts, we get \(u\in \operatorname{Dom}((H _{X,A,Q}^{0})^{\ast})\). Then by a similar method as in Lemma 4, the only function \(u\in \operatorname{Dom}(\mathbf{t}_{X,A,Q})\) satisfying equation (3.18) is \(u=0\). So we obtain that the set \(\operatorname{Dom} (H_{X,A,Q}^{0})\) is a core of the form \(\mathbf{t}_{X,A,Q}\). □
Lemma 8
If the form \(\mathbf{t}_{X,A,Q}\) is closed and \(\mathbf{H}_{X,A,Q}\) is self-adjoint, then the operator associated with the form \(\mathbf{t} _{X,A,Q}\) coincides with \(\mathbf{H}_{X,A,Q}=(\mathbf{H}_{X,A,Q})^{\ast}\).
Proof
Integrating by parts, we can get from (1.2) that \(\operatorname{Dom}(\mathbf{H} _{X,A,Q}^{0})\subset \operatorname{Dom}(\mathbf{t}_{X,A,Q})\). For \(u,v\in \operatorname{Dom}(\mathbf{H} _{X,A,Q}^{0})\),
Assume that T is the self-adjoint operator associated with \(\mathbf {t}_{X,A,Q}\). Since \(\operatorname{Dom}(H_{X,A,Q}^{0})\) is a core of the form \(\mathbf{t} _{X,A,Q}\) by Lemma 7, by the first representation theorem we have \(u\in \operatorname{Dom}(T)\) and \(Tu=\mathbf{H}_{X,A,Q}^{0}u\), and hence \(T=\mathbf{H} _{X,A,Q}\). □
Lemma 9
Assume that \(Q(x)\geq0\), \(x\in\mathbb{R}_{+}\). Let the forms \(\mathbf{t}_{Q}\) and \(\mathbf{t}_{R}^{+}\) be defined by (3.3) and (3.5). Then the form \(\mathbf{t}_{X,A^{+},Q}=\mathbf{t}_{Q}+\mathbf{t}_{R}^{+}\) is nonnegative and closed.
Proof
The proof is similar to that of Lemma 6. □
Lemma 10
Let \(q_{ij}\in L_{\mathrm{loc}}^{1}( \mathbb{R} _{+})\), and let the forms \(\mathbf{t}_{Q}\) and \(\mathbf{t}_{R}^{\pm}\) be given by (3.3) and (3.4).
-
(i)
If \(\mu_{\max}^{-}(Q(x))\) and \(\mu_{\max}^{-}(A_{k})\) satisfy (3.7), then the form \(\mathbf{t}_{X,A,Q}\) is closed and lower semibounded. Moreover, \(\operatorname{Dom}(\mathbf{t}_{X,A,Q})=\operatorname{Dom} (\mathbf{t}_{X,A^{+},Q^{+}})\), and the operator associated with \(\mathbf{t}_{X,A,Q}\) coincides with \(\mathbf{H} _{X,A,Q}\).
-
(ii)
If \(\mu_{\max}(Q(x))=\mu_{\max}^{-}(Q(x))\) and \(\mu _{\max }(A_{k})=\mu_{\max}^{-}(A_{k})\), then conditions (3.7) are necessary and sufficient for the form \(\mathbf{t}_{X,A,Q}\) to be lower semibounded.
Proof
(i) By the Lemma 9 the form \(\mathbf{t}_{X,A^{+},Q }\)is closed. Moreover, by Lemma 5, \(\mathbf{t}_{Q}^{-}\) and \(\mathbf{t} _{R}^{-} \) are infinitesimally \(\mathbf{t}_{Q}^{+}\)-bounded and hence infinitesimally \(\mathbf{t}_{X,A^{+},Q^{+}}\)-bounded. Using Lemma 2, we complete the proof.
(ii) Sufficiency is implied by (i). Let us prove necessity. Assume the converse, that is, the second condition in (3.7) does not hold. Then there exists \(\{n_{j}\}_{1}^{\infty}\subset\mathbb{N}\) such that
Define \(\varphi_{j}(x):=\varphi(x-n_{j})\), \(j\in\mathbb{N}\), where \(\varphi\in C_{0}^{\infty}(\mathbb{ \mathbb{R}}_{+},\mathbb{C}^{m})\) is such that \(\sup p\varphi\in(-\frac{1}{2},\frac{3}{2})\), \(0\leq \|\varphi \|\leq1\), and \(\varphi(x)=e_{1}\), \(x\in[0,1]\), where \(e_{1}\) denotes the m-dimensional column unit vector whose first component is 1. By (3.19) and the form (3.6) we obtain \(\mathbf{t} _{X,A,Q}[\varphi_{j}]\leq-n_{j}+\|\varphi\|_{W^{1,2}(\mathbb{R}_{+}, \mathbb{C}^{m})}^{2}\), and we note that when \(n_{j}\rightarrow\infty \), \(\mathbf{t}_{X,A,Q}\) is not lower semibounded. Hence, the contradiction finishes the proof. □
Corollary 1
If
then the form \(\mathbf{t}_{X,A}=\mathbf{t}_{X,A,0}\) is closed, and lower semibounded, and \(\operatorname{Dom}(\mathbf{t}_{X,A})=W_{0}^{1,2}(\mathbb {R}_{+},\mathbb{C} ^{m})\). Moreover, the operator associated with the form \(\mathbf{t}_{X,A}\) coincides with \(\mathbf{H}_{X,A}\).
Proof
Clearly, (3.20) yields (3.15) and (3.16). Lemma 10 completes the proof. □
4 Discrete spectrum
4.1 Sufficient conditions and necessary conditions
In this section we find conditions under which the vectorial Schrödinger operator \(\mathbf{H}_{X,A,Q}\) has a purely discrete spectrum. The discrete spectrum of a self-adjoint operator T, \(\sigma_{d}(T)\), is the set of all isolated eigenvalues of T with finite multiplicity, and the essential spectrum of T is the complement in \(\sigma(T)\) of \(\sigma_{d}(T)\) (see [14, 15]).
Theorem 1
Assume that \(q_{ij}\in L_{\mathrm{loc}}^{1}(\mathbb{R}_{+})\) and (3.7) is satisfied. Then the operator \(\mathbf{H}_{X,A,Q}\) is lower semibounded and self-adjoint, and its spectrum \(\sigma(\mathbf {H}_{X,A,Q})\) is discrete if, for every \(\varepsilon>0\),
If the spectrum \(\sigma(\mathbf{H}_{X,A,Q})\) is discrete, then
Remark 1
Before giving the proof, we note the following facts about matrices.
-
(i)
If a matrix-valued function \(Q(x)\geq0\), then its eigenvalues are all positive.
-
(ii)
If \(Q(x)\in L_{\mathrm{loc}}^{1}(\mathbb{R}_{+},\mathbb {C}^{m\times m})\), then the eigenvalue functions are also integrable.
Proof
We divide the proof into two steps.
(i) First, assume that the potential \(Q(x)\) is lower semibounded. Let \(Y(x)=(y_{1}(x),y_{2}(x), \ldots,y_{m}(x))^{T}\).
Sufficiency. Without loss of generality we assume that \((Q(x)Y(x),Y(x))_{m} \geq(Y(x),Y(x))_{m}\). By Lemma 6 the form \(\mathbf{t}_{X,A,Q}\) is closed in \(\mathfrak{H}=L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\). Let \(\mathfrak{H}_{X,A,Q}\) be the Hilbert space generated by \(\mathbf{t}_{X,A,Q}\). Let us show that the unit ball in \(\mathfrak{H}_{X,A,Q}\),
is compact in \(L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\). Since the embedding \(W^{1,2}([0,a],\mathbb{C}^{m})\hookrightarrow L^{2}([0,a],\mathbb {C}^{m})\) is compact for any \(a>0\), it suffices to show that the tails \(\int _{N}^{\infty }(Y(x),Y(x))_{m}\,dx\) uniformly tend to zero in \(\mathbb{U}_{X,A,Q}\).
Let us divide the semiaxis \(\mathbb{R}_{+}\) into intervals \(\Omega _{n}:=\Omega_{n}(2\varepsilon)\) of length 2ε, \(\Omega _{k}\cap\Omega_{j}=\varnothing\). Clearly, for any \(Y\in W^{1,2}(\mathbb{R} _{+},\mathbb{C}^{m})\) and any \(x,z\in\Omega_{n}\), we have
Since Y is continuous on \(\mathbb{R}_{+}\), there exists \(t_{n}\in \Omega _{n}\) such that
Integrating (4.3) over \(\Omega_{n}\) and taking (4.4) into account, we obtain
According to condition (4.1), there exists \(N\in\mathbb{N}\) such that
Combining (4.5) and (4.6), we get
Hence, \(\int_{N}^{\infty}(Y(x),Y(x))_{m}\,dx\) uniformly tends to zero in \(\mathbb{U}_{X,A,Q}\). By Lemma 1 the spectrum \(\sigma(\mathbf{H} _{X,A,Q})\) is discrete.
Necessity. Assume that condition (4.2) is violated. Then there exist \(\varepsilon>0\) and a sequence \(x_{k}\rightarrow\infty\) such that the inequality
holds with some \(C_{1}>0\). Let \(\varphi\in W^{1,2}(\mathbb{R}_{+})\) with \(\Vert \varphi \Vert _{W^{1,2}}=1\) and \(\sup p\varphi\subset (0,\varepsilon)\). Let
Clearly, \(\Vert \varphi_{n}\Vert _{W^{1,2}}=\Vert \varphi \Vert _{W^{1,2}}=1\). Since \(\sup_{x\in\mathbb{R}_{+}}|\varphi (x)|=C_{2}<\infty\), we get
Thus, the sequence \(\{\varphi_{n}\}_{1}^{\infty}\) is bounded in \(\mathfrak{ H}_{X,A,Q}\) but is not compact in \(L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\). By Lemma 1 the spectrum \(\sigma(\mathbf{H}_{X,A,Q})\) is not discrete.
(ii) Assume now that \(Q(x)\) satisfies condition (3.7). Then by Lemma 10(i) the operator \(\mathbf{H}_{X,A,Q}\) is self-adjoint and lower semibounded if \(A_{k}\) (\(k=1,2,\ldots\)) satisfy (3.7). Furthermore, by (3.7), \(\mu_{\max}(Q(x))\) and \(\mu_{\max}^{+}(Q(x))\) satisfy (4.1) simultaneously. By the above considerations, the spectrum of the operator \(\mathbf{H}_{X,A,Q^{+}}\) is discrete if \(\mu _{\max }^{+}(Q(x))\) satisfies (4.1). Note that \(\mathfrak{q}^{-}\) is infinitesimally \(\mathbf{t}_{Q^{+}}\)-bounded if \(Q(x)\) satisfies condition (3.7). This yields
and the proof of Lemma 1 is finished. □
Remark 2
This result coincides with the corresponding result obtained in [1] in the scalar case (\(m=1\)), and in this case it is also necessary. But in the vectorial case, condition (4.1) is no longer necessary. In the next subsection, by giving additional restrictions on symmetric potential matrix \(Q(x)\) and \(A_{k}\) we obtain a sufficient and necessary condition.
Corollary 2
Let \(Q(x)\) and \(A_{k}\) satisfy (3.7). Then the spectrum \(\sigma( \mathbf{H}_{X,A,Q})\) is discrete whenever
for every \(\varepsilon>0\). If, in addition,
for some \(\varepsilon>0\), then
is necessary for \(\sigma(\mathbf{H}_{X,A,Q})\) to be discrete.
Proof
The proof is immediate from Theorem 1. □
Corollary 3
Let the symmetric potential function \(Q(x)\) and the matrix sequence \(\{A_{k}\}\) satisfy (3.7). Assume also that \(d_{\ast}=\inf_{k\in \mathbb{N}}d_{k}>0\). Then the spectrum \(\sigma(\mathbf{H}_{X,A,Q})\) is discrete if, for every \(\varepsilon>0\),
Proof
Sufficiency is immediate from Theorem 1. □
4.2 Sufficient and necessary conditions for a special case
In this subsection, we give some restrictions on \(Q(x)\) and \(A_{k}\) to get a sufficient and necessary condition for the spectrum \(\sigma(\mathbf{H} _{X,A,Q})\) to be discrete:
-
(1)
\(\sum_{i\neq j}q_{ij}(x)\leq aq_{jj}(x)\), \(j=1,2,\ldots, m\), \(0\leq a<1\);
-
(2)
\(\sum_{i\neq j}a_{ij}^{k}\leq ba_{jj}^{k}\), \(j=1,2,\ldots ,m\), \(k=1,2,\ldots\) , \(0\leq b<1\).
Let \(Q(x)=Q_{1}(x)+Q_{2}(x)\) and \(A_{k}=A_{k1}+A_{k2}\), where \(Q_{1}(x)=(q_{ij}(x)\delta_{ij})_{i,j=1}^{m}\) and \(A_{k1}=(a_{ij}^{k}\delta _{ij})_{i,j=1}^{m}\). By (3.1) and (3.4) we denote the following forms:
Theorem 2
Under conditions (1)-(2), \(\mathfrak{q}_{2}[Y]\) is \(\mathfrak{q}_{1}[Y]\) relatively form bounded with bound \(a<1\), and \(\mathbf{t} _{R_{2}}[Y]\) is \(\mathbf{t}_{R_{1}}[Y]\) relatively form bounded with bound \(b<1\).
Proof
Similarly, \(\mathbf{t}_{R_{2}}[Y]\leq b\mathbf{t}_{R_{1}}[Y]+c\|Y\|^{2}\), where c is a positive constant. Then by Definition 1 the theorem is proved. □
We denote the operator corresponding to the differential expression
by H. Obviously, H equals the direct sum of scalar operators \(\mathbf{H} _{i}\) on \(L^{2}(\mathbb{R}_{+})\) that are defined by the expressions
Then \(\sigma(\mathbf{H})\) =\(\cup_{i=1}^{m}\sigma(\mathbf{H}_{i})\), which is obtained by the direct sum decomposition method of operators (see [16]). Denote \(\mathbf{t}_{\mathbf{H}}=\mathfrak{q}_{1}[Y]+\mathbf{t} _{R_{1}}[Y]+\mathbf{t}_{0}[Y]\). Note that \(\mathbf{t}_{X,A,Q}=\mathbf{t}_{ \mathbf{H}}+\mathfrak{q}_{2}[Y]+\mathbf{t}_{R_{2}}[Y]\), \(\mathfrak{q}_{2}[Y]+ \mathbf{t}_{R_{2}}[Y]\) is \(\mathbf{t}_{\mathbf{H}}\) relatively form bounded, and \(\mathbf{t}_{\mathbf{H}}\) is associated with the operator H. By Lemma 2 the norms \(\|\cdot\|_{\mathbf{t}_{X,A,Q}}\) and \(\|\cdot\|_{\mathbf{H}}\) are equivalent. If \(i_{\mathbf{H}}:\mathfrak{H}_{\mathbf{H} }\hookrightarrow L^{2}(\mathbb{R}_{+},\mathbb{C}^{m})\) is compact, then \(i_{\mathbf{H}}:\mathfrak{H}_{\mathbf{H}_{X,A,Q}}\hookrightarrow L^{2}( \mathbb{R}_{+},\mathbb{C}^{m})\) is also compact. Thus, if \(\sigma (\mathbf{H})\) is discrete, then \(\sigma(\mathbf{H}_{X,A,Q})\) is also discrete.
It is evident that H has a purely discrete spectrum if and only if the operator \(\mathbf{H}_{i}\) has such a spectrum for all \(i=1,2,\ldots ,m\). But the operator \(\mathbf{H}_{i}\) is the ordinary ‘scalar’ Schrödinger operator with positive potential and δ-interactions, and the theorem of discrete criterion in [1] holds. Hence. we get the following theorem.
Theorem 3
Let \(Q(x)\) and \(A_{k}\) satisfy conditions (1)-(2). Then the spectrum \(\sigma(\mathbf{H}_{X,A,Q})\) is discrete if and only if, for each \(i=1,2,\ldots,m\) and for every \(\varepsilon>0\),
Example 1
Let \(m=2\), \(Y(x)=(y_{1}(x),y_{2}(x))^{T}\), \(Q(x)=\bigl ( {\scriptsize\begin{matrix}{} x^{2}-2 & 0 \cr 0 & x-4\end{matrix}} \bigr ) \), \(A_{k}=\bigl ( {\scriptsize\begin{matrix}{} k+1 & 1 \cr 1 & 2^{k}\end{matrix}} \bigr ) \), and \(x_{k}=\sqrt{k}\). Then by Theorem 3 we have that the spectrum of such an operator is discrete.
References
Albeverio, S, Kostenko, A, Malamud, M: Spectral theory of semibounded Sturm-Liouville operators with local interactions on a discrete set. J. Math. Phys. 51, 102102 (2010)
Kostenko, A, Malamud, M: 1-dimensional Schrödinger operators with local point interactions on a discrete set. J. Differ. Equ. 249(2), 253-304 (2010)
Yan, J, Shi, G: Spectra properties of Sturm-Liouville operators with local interactions on a discrete set. J. Differ. Equ. 257, 3423-3447 (2014)
Shubin, C, Christ Stolz, G: Spectral theory of one-dimensional Schrödinger operators with point interactions. J. Math. Anal. Appl. 184, 491-516 (1994)
Albeverio, S, Gesztesy, F, Hoegh-Krohn, R, Holden, H: Solvable Models in Quantum Mechanics, 2nd edn. Chelsea, New York (2005)
Eckhardt, J, Gesztesy, F, et al.: Supersymmetry and Schrödinger-type operators with distributional matrix-valued potentials. J. Spectr. Theory 4, 715-768 (2014)
Mirzoev, KA, Safonova, TA: Singular Sturm-Liouville operators with distribution potential on spaces of vector functions. Dokl. Akad. Nauk SSSR 441(2), 165-168 (2011)
Liu, X, Wang, Z: Conditions for the discreteness of spectra of two-item self-adjoint vector differential operators. J. Inn. Mong. Norm. Univ. 2, 153-156 (2009)
Clark, S, Gesztesy, F: On Povzner-Wienholtz-type self-adjointness results for matrix-valued Sturm-Liouville operators. Proc. R. Soc. Edinb. A 133, 747-758 (2003)
Molčanov, AM: On conditions for the spectrum of a second order self-adjoint differential equation to be discrete. Trans. Mosc. Math. Soc. 2, 169-200 (1953)
Kato, T: Perturbation Theory for Linear Operators. Springer, Berlin (1966)
Reed, M, Simon, B: Methods of Modern Mathematical Physics. II. Fourier Analysis, Self-Adjointness. Academic Press, New York (1975)
Muller-Pfeiffer, E: Spectral Theory of Ordinary Differential Operators. Ellis Horwood, Chichester (1981)
Glazman, IM: Direct Methods of Qualitative Spectral Analysis of Singular Differential Operators. Israel Program for Scientific Translations, Jerusalem (1965)
Weidmann, J: Linear Operators in Hilbert Spaces. Springer, Berlin (1980)
Muller-Pferiffer, E, Sun, J: On the discrete spectrum of ordinary differential operators in weighted function spaces. Z. Anal. Anwend. 14(5), 637-646 (1995)
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Liu, X., Zhao, X. & Shi, G. Discreteness of the spectrum of vectorial Schrödinger operators with δ-interactions. Bound Value Probl 2016, 24 (2016). https://doi.org/10.1186/s13661-016-0536-4
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DOI: https://doi.org/10.1186/s13661-016-0536-4