Abstract
In this paper, we consider a discontinuous Dirac operator with eigenparameter dependent both boundary and two transmission conditions. We introduce a suitable Hilbert space formulation and get some properties of eigenvalues and eigenfunctions. Then we investigate the Green’s function, the resolvent operator, and some uniqueness theorems by using the Weyl function and some spectral data.
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1 Introduction
Inverse problems of spectral analysis recover operators by their spectral data. Fundamental and vast studies about the classical Sturm-Liouville, Dirac operators, Schrödinger equation, and hyperbolic equations are well studied (see [1–9] and references therein).
Studies of eigenvalue dependence appearing not only in the differential equation but also in the boundary conditions have increased in recent years (see [10–18] and corresponding bibliography). Moreover, boundary conditions which depend linearly and nonlinearly on the spectral parameter are considered in [10, 18–23] and [24–30], respectively. Furthermore, boundary value problems with transmission conditions are also increasingly studied. These types of studies introduce qualitative changes in the exploration. Direct and inverse problems for Sturm-Liouville and Dirac operators with transmission conditions are investigated in some papers (see [7, 31–34] and the corresponding bibliography). Then differential equations with the spectral parameter and transmission conditions arise in heat, mechanics, mass transfer problems, in diffraction problems, and in various physical transfer problems (see [20, 31, 35–42] and corresponding bibliography).
More recently, some boundary value problems with eigenparameter in boundary and transmission conditions were extended to the case of two, more than two or a finite number of transmissions in [43–47] and the references therein.
The present paper deals with the discontinuous Dirac operator with eigenparameter dependent boundary and two transmission conditions. The aim of the present paper is to obtain the asymptotic formulas of the eigenvalues and eigenfunctions, to construct the Green’s function and the resolvent operator, and to prove some uniqueness theorems. Especially, some parameters of the considered problem can be determined by the Weyl function and some spectral data.
We consider a discontinuous boundary value problem L with function \(\rho (x)\);
where
and \(\rho_{1}\), \(\rho_{2}\), and \(\rho_{3}\) are given positive real numbers;
\(\lambda\in \mathbb{C} \) is a complex spectral parameter; we have boundary conditions at the endpoints,
with transmission conditions at the two points \(x=\xi_{1}\), \(x=\xi_{2}\),
where \(\alpha_{i}\), and \(\alpha_{j}^{\prime}\), \(\gamma_{j}^{\prime}\) (\(i=\overline{1,6}\), \(j=1,2\)) are real numbers; \(\alpha_{3}>0\), \(\alpha_{5}>0\), and
2 Operator formulation and properties of spectrum
In this section, we present the inner product in the Hilbert space \(H:=L_{2}(\Lambda)\oplus L_{2}(\Lambda)\oplus \mathbb{C} ^{4}\) and the operator T defined on H such that (1)-(7) can be regarded as the eigenvalue problem of operator T. We define an inner product in H by
for
Consider the operator T defined in the domain
such that
for
Thus, we can rewrite the considered problem (1)-(7) in the operator form as \(TF=\lambda F\), i.e., the problem (1)-(7) can be considered as an eigenvalue problem of the operator T.
We define the solutions
and
of equation (1) satisfying the initial conditions
and similarly
respectively.
These solutions are entire functions of λ for each fixed \(x\in[ a,b ] \) and satisfy the relation \(\psi(x,\lambda_{n})=\kappa_{n}\varphi(x,\lambda_{n})\) for each eigenvalue \(\lambda_{n}\), where
Lemma 1
T is a self-adjoint operator. Therefore, all eigenvalues and eigenfunctions of the problem (1)-(7) are real and the two eigenfunctions \(\varphi(x,\lambda _{1})= ( \varphi_{1}(x,\lambda_{1}),\varphi_{2}(x,\lambda_{1}) ) ^{T}\) and \(\varphi(x,\lambda_{2})= ( \varphi_{1}(x,\lambda_{2}),\varphi_{2}(x,\lambda_{2}) ) ^{T}\) corresponding to different eigenvalues \(\lambda_{1}\) and \(\lambda_{2}\) are orthogonal in the sense of
By the method of variation of parameters, integral equations in Lemmas 2, 3 can be obtained and with the help of these integral equations, we also have their asymptotic behaviors.
Lemma 2
The following integral equations and asymptotic behaviors hold:
Lemma 3
The following integral equations and asymptotic behaviors hold:
Denote
which are independent of \(x\in\Lambda_{i}\) and are entire functions such that \(\Lambda_{1}= [ a,\xi_{1} ) \), \(\Lambda_{2}= ( \xi_{1},\xi_{2} ) \), \(\Lambda_{3}= ( \xi _{2},b ] \).
Let
and
The function \(\Delta(\lambda)\) is called the characteristic function and numbers \(\{ \mu_{n} \} _{n\in \mathbb{Z} }\) are called the normalizing constants of the problem (1)-(7).
Lemma 4
The following equality holds for each eigenvalue \(\lambda_{n}\):
Proof
Since
and
we obtain
After adding and subtracting \(\Delta(\lambda)\) on the left-hand side of the last equality and by using the conditions (2)-(7) one can obtain
or
For \(\lambda\rightarrow\lambda_{n}\), \(-\dot{\Delta}(\lambda_{n})=\kappa_{n}\mu_{n}\) is obtained by using the equality \(\psi(x,\lambda_{n})=\kappa_{n}\varphi(x,\lambda _{n})\) and (12). □
From Lemma 4, we see that \(\dot{\Delta}(\lambda_{n})\neq0\). Thus, the eigenvalues of problem L are simple.
Lemma 5
(cf. [48])
Let \(\{ \alpha_{i} \} _{i=1}^{p}\) be the set of real numbers satisfying the inequalities \(\alpha_{0}>\cdots >\alpha_{p-1}>0\) and \(\{ a_{i} \} _{i=1}^{p}\) be the set of complex numbers. If \(a_{p}\neq0\) then the roots of the equation \(e^{\alpha_{0}\lambda}+a_{1}e^{\alpha_{1}\lambda}+\cdots +a_{p-1}e^{\alpha _{p-1}\lambda}+a_{p}=0\) have the form
where \(\Psi(n)\) is a bounded sequence.
Now, from Lemma 2 and (11), we can note that
where
On the other hand, we can see non-zero roots, namely the \(\lambda _{n}^{0}\) of the equation \(\Delta_{0}(\lambda)=0\) are real and simple.
Furthermore, it can be proved by using Lemma 5 that
Theorem 1
The eigenvalues \(\{ \lambda_{n} \} \) which are located on the positive side of the real axis satisfy the following asymptotic behavior:
Proof
Denote
where δ is a sufficiently small number. The relations
and
are valid for \(\lambda\in\partial G_{n}\). Then, by Rouche’s theorem, we see that the number of zeros of \(\Delta_{0}(\lambda)\) coincides with the number of zeros of \(\Delta (\lambda)\) in \(G_{n}\), namely \(n+4\) zeros, \(\lambda_{0},\lambda_{1},\lambda_{2},\ldots,\lambda_{n+3}\). In the annulus between \(G_{n}\) and \(G_{n+1}\), \(\Delta(\lambda)\) has accurately one zero, namely \(k_{n}:k_{n}=\lambda_{n}^{0}+\delta_{n}\), for \(n\geq1\). So, it follows that \(\lambda_{n+4}=k_{n}\). Applying Rouche’s theorem in \(\eta_{\varepsilon }= \{ \lambda:\vert \lambda-\lambda_{n}^{0}\vert \leq\varepsilon\} \) for sufficiently small ε and sufficiently large n, we get \(\delta_{n}=o(1)\). Finally, we obtain the asymptotic formula \(\lambda_{n}=\lambda_{n-4}^{0}+o(1)\). □
3 Construction of Green’s function
In this section, we get the resolvent of the boundary value problem (1)-(7) for λ, not an eigenvalue. Hence, we find the solution of the non-homogeneous differential equation
which satisfies the conditions (2)-(7).
We can find the general solution of homogeneous differential equation
in the form
where \(c_{i}\), \(i=\overline{1,6}\) are arbitrary constants. By using the method of variation of parameters, we shall investigate the general solution of the non-homogeneous linear differential equation (15) in the form
where the functions \(c_{i} ( x,\lambda) \) (\(i=\overline{1\text{-}6}\)) satisfy the following linear system of equations:
Since λ is not an eigenvalue, each of the linear system of equations has a unique solution. Thus,
and
It is obvious that
where \(c_{i}\), \(i=\overline{1,6}\) are arbitrary constants. Substituting these above expressions in (16), then we obtain the general solution of non-homogeneous linear differential equation (15) in the form
Therefore, we easily see that \(l_{1} ( U_{1} ) =-c_{2}\Delta_{1} ( \lambda) \), \(l_{2} ( U_{3} ) =c_{5}\Delta_{3} ( \lambda) \). Since \(\Delta_{1} ( \lambda) \neq0\), \(\Delta_{2} ( \lambda) \neq0\), and from the boundary conditions (2)-(3), \(c_{2}=0\), and \(c_{5}=0\).
On the other hand, considering these results and transmission conditions (4)-(7), the following linear equation system according to the variables \(c_{1}\), \(c_{3}\), \(c_{4}\), and \(c_{6}\) is acquired:
Recalling the definitions of the solutions \(\varphi_{ij} ( x,\lambda) \) and \(\chi_{ij} ( x,\lambda)\) (\(i=2,3\), \(j=1,2\)), the following relation is gotten for the determinant of this linear equation system:
Since the above determinant is different from zero, the solution of (18) is unique. When we solve system (18), we obtain the following equality for the coefficients \(c_{1}\), \(c_{3}\), \(c_{4}\), and \(c_{6}\):
As a result, if we substitute the coefficients \(c_{i}\) (\(i=1,3,4,6\)) in (17), then we get the resolvent \(U ( x,\lambda) \) as follows:
such that
We can easily find the Green’s function from the resolvent (19) as follows:
We can rewrite equation (19) in the following form:
Now, we define the resolvent operator
It is easy to see that the operator equation \(( T-\lambda I ) Y=F\), \(F\in H_{1}\) is equivalent to the boundary value problem (15), (2)-(7) where λ is not an eigenvalue,
4 Inverse problems
In this section, we study the inverse problems for the reconstruction of boundary value problem (1)-(7) by the Weyl function and spectral data.
We consider the boundary value problem L̃ which has the same form as L but with different coefficients \(\tilde{\Omega}(x)\), \(\tilde {\alpha }_{j}\), \(\tilde{\gamma}_{j}\), \(\tilde{\alpha}_{j}^{\prime}\), \(\tilde{\gamma}_{j}^{\prime}\), \(j=1,2\), such that
If a certain symbol σ denotes an object related to L, then the symbol σ̃ denotes the corresponding object related to L̃.
Let \(\Phi(x,\lambda)\) be a solution of equation (1) which satisfies the condition \(( \lambda\alpha_{2}^{\prime}-\alpha _{2} ) \Phi_{2}(a,\lambda)- ( \lambda\alpha_{1}^{\prime}-\alpha _{1} ) \Phi_{1}(a,\lambda)=1\) and the transmissions (4)-(7).
Assume that the function \(\phi(x,\lambda)= ( \phi_{1}(x,\lambda),\phi _{2}(x,\lambda) ) ^{T}\) is the solution of equation (1) that satisfies the conditions \(\phi_{1}(a,\lambda)=d_{1}^{-1}\alpha _{2}^{\prime}\), \(\phi_{2}(a,\lambda)=d_{1}^{-1}\alpha_{1}^{\prime}\) and the transmission conditions (4)-(7).
Since \(W [ \varphi,\phi] =1\), the functions ϕ and φ are linearly independent. Therefore, the function \(\psi(x,\lambda)\) can be represented by
or
which is called the Weyl solution, and
is called the Weyl function.
Lemma 6
The following representation is true:
Proof
The Weyl function \(M(\lambda)\) is a meromorphic function with respect to λ, which has simple poles at \(\lambda_{n}\). Therefore, we calculate
Since
and \(\dot{\Delta}(\lambda_{n})=-\kappa _{n}\mu_{n}\),
Let \(\Gamma_{n}= \{ \lambda:\vert \lambda\vert \leq\vert \lambda_{n}^{o}\vert +\varepsilon\} \), where ε is a sufficiently small number. Consider the contour integral \(I_{n} ( \lambda) =\frac{1}{2\pi i}{ \int_{\Gamma_{n}}} \frac{M ( \mu) }{\mu-\lambda}\,d\mu\), \(\lambda\in \operatorname{int}\Gamma_{n}\).
Since \(\Delta( \lambda) \geq C_{\delta}\lambda ^{4}e^{\vert \operatorname{Im}\lambda\vert ( ( \xi _{1}-a ) \rho_{1}+ ( \xi_{2}-\xi_{1} ) \rho_{2}+ ( b-\xi_{2} ) \rho_{3} ) }\) and \(M(\lambda)=\frac{\alpha _{1}^{\prime}\psi_{1}(a,\lambda)-\alpha_{2}^{\prime}\psi_{2}(a,\lambda)}{d_{1}\Delta(\lambda)}\), \(\vert M ( \lambda) \vert \leq\frac{C_{\delta}}{\vert \lambda\vert }\) for \(\lambda\in F_{\delta}= \{ \lambda:\vert \lambda-\lambda_{n}\vert \geq\delta, n=0,\pm1,\ldots\} \), where δ is a sufficiently small number. Thus, \(\lim_{n\rightarrow\infty}I_{n} ( \lambda) =0\). Then the residue theorem yields
□
Theorem 2
If \(M(\lambda)=\tilde{M}(\lambda)\), then \(L=\tilde{L}\), i.e., \(\Omega (x)=\tilde{\Omega}(x)\), a.e. and \(\alpha_{j}=\tilde{\alpha}_{j}\), \(\gamma _{j}=\tilde{\gamma}_{j}\), \(\alpha_{j}^{\prime}=\tilde{\alpha }_{j}^{\prime}\), \(\gamma_{j}^{\prime}=\tilde{\gamma}_{j}^{\prime}\), \(j=1,2\).
Proof
We introduce a matrix \(P(x,\lambda)= [ P_{kj}(x,\lambda) ] _{k,j=1,2}\) by the formula
or
where \(\Phi(x,\lambda)=\frac{\psi(x,\lambda)}{\Delta(\lambda)}\) and \(W ( \tilde{\Phi},\tilde{\varphi} ) =1\). Thus, we find
On the other hand, from (20), we get
Thus, if \(M(\lambda)\equiv\tilde{M}(\lambda)\) then the functions \(P_{ij}(x,\lambda)\) (\(i,j=1,2\)) are entire in λ for each fixed x. Moreover, since asymptotic behaviors of \(\varphi_{i}(x,\lambda)\), \(\tilde{\varphi}_{i}(x,\lambda)\), \(\psi _{i}(x,\lambda)\), \(\tilde{\psi}_{i}(x,\lambda)\), and \(\vert \Delta (\lambda)\vert \geq C_{\delta}\vert \lambda\vert ^{4}e^{\vert \operatorname{Im}\lambda\vert ((\xi_{1}-a)\rho _{1}+(\xi_{2}-\xi_{1})\rho_{2}+(b-\xi_{2})\rho_{3})}\) in \(F_{\delta}\cap \tilde{F}_{\delta}\), we can easily see that the functions \(P_{ij}(x,\lambda)\) are bounded with respect to λ. As a result, these functions do not depend on λ. Here, we denote \(\tilde{F}_{\delta}= \{ \lambda:\vert \lambda-\tilde{\lambda}_{n}\vert \geq\delta, n=0,\pm1,\pm2,\ldots\} \) where n is sufficiently small number, \(\tilde{\lambda}_{n}\) are eigenvalues of the problem L̃.
From (25), we get
It follows from the representations of the solutions \(\varphi(x,\lambda )\) and \(\psi(x,\lambda)\), that
for all x in Λ. Thus, \(\lim_{\lambda \rightarrow\infty} ( P_{11}(x,\lambda)-1 ) =0\) is valid uniformly with respect to x. So we have \(P_{11}(x,\lambda )\equiv1\) and similarly \(P_{12}(x,\lambda)\equiv0\), \(P_{21}(x,\lambda )\equiv 0\), \(P_{22}(x,\lambda)\equiv1\).
From (23), we obtain \(\varphi_{1}(x,\lambda)\equiv\tilde{\varphi }_{1}(x,\lambda)\), \(\Phi_{1}\equiv\tilde{\Phi}_{1}\), \(\varphi_{2}(x,\lambda)\equiv\tilde{\varphi}_{2}(x,\lambda)\), and \(\Phi_{2}\equiv \tilde{\Phi}_{2}\) for all x and λ. Moreover, from \(\Phi (x,\lambda)=\frac{\psi(x,\lambda)}{\Delta(\lambda)}\), we get \(\frac{\psi_{2} ( x,\lambda) }{\psi_{1} ( x,\lambda) }=\frac{\tilde{\psi}_{2} ( x,\lambda) }{\tilde{\psi}_{1} ( x,\lambda) }\). Hence, \(\Omega(x)=\tilde{\Omega}(x)\), i.e., \(p ( x ) =\tilde{p} ( x ) \), \(r ( x ) =\tilde{r} ( x ) \) almost everywhere. On the other hand, since
we easily see that \(\alpha_{2}^{\prime}=\tilde{\alpha}_{2}^{\prime}\), \(\alpha_{2}=\tilde{\alpha}_{2}\), \(\alpha_{1}^{\prime}=\tilde{\alpha}_{1}^{\prime}\), \(\alpha_{1}=\tilde{\alpha}_{1}\), and \(\gamma _{2}^{\prime}=\tilde{\gamma}_{2}^{\prime}\), \(\gamma_{2}=\tilde{\gamma}_{2}\), \(\gamma_{1}^{\prime}=\tilde{\gamma}_{1}^{\prime}\), \(\gamma_{1}=\tilde {\gamma }_{1}\). Therefore, \(L\equiv\tilde{L}\). □
Theorem 3
If \(\lambda_{n}=\tilde{\lambda}_{n}\) and \(\mu_{n}=\tilde{\mu}_{n}\) for all n, then \(L\equiv\tilde{L}\), i.e., \(\Omega(x)=\tilde{\Omega }(x)\), a.e., \(\alpha_{j}=\tilde{\alpha}_{j}\), \(\gamma_{i}=\tilde{\gamma}_{i}\), \(\alpha _{j}^{\prime}=\tilde{\alpha}_{j}^{\prime}\), \(\gamma_{j}^{\prime}=\tilde {\gamma}_{j}^{\prime}\), \(j=1,2\). Hence, the problem (1)-(7) is uniquely determined by the spectral data \(\{ \lambda_{n},\mu_{n} \} \).
Proof
If \(\lambda_{n}=\tilde{\lambda}_{n}\) and \(\mu_{n}=\tilde{\mu}_{n}\) for all n, then \(M(\lambda)=\tilde{M}(\lambda)\) by Lemma 6. Therefore, we get \(L=\tilde{L}\) by Theorem 2. □
Let us consider the boundary value problem \(L_{1}\) with the condition \(\alpha_{1}^{\prime}y_{1}(a,\lambda)-\alpha_{2}^{\prime}y_{2}(a,\lambda)=0\) instead of the condition (2) in L. Let \(\{ \tau_{n} \} _{n\in \mathbb{Z} }\) be the eigenvalues of the problem \(L_{1}\). It is clear that the \(\tau _{n}\) are zeros of \(\Delta_{1}(\tau):=\alpha_{1}^{\prime}\psi_{1}(a,\tau )-\alpha_{2}^{\prime}\psi_{2}(a,\tau)\), which is the characteristic function of \(L_{1}\).
Theorem 4
If \(\lambda_{n}=\tilde{\lambda}_{n}\) and \(\tau_{n}=\tilde{\tau}_{n}\) for all n, then \(L(\Omega,\gamma_{i},\gamma_{j}^{\prime})=L(\tilde{\Omega},\tilde{\gamma}_{i},\tilde{\gamma}_{j}^{\prime})\), \(j=1,2\).
Hence, the problem L is uniquely determined by the sequences \(\{ \lambda_{n} \} \) and \(\{ \tau_{n} \} \) except coefficients \(\alpha_{j}\) and \(\alpha_{j}^{\prime}\).
Proof
Since the characteristic functions \(\Delta(\lambda)\) and \(\Delta _{1}(\tau)\) are entire of order 1, the functions \(\Delta(\lambda)\) and \(\Delta _{1}(\tau)\) are uniquely determined up to a multiplicative constant with their zeros by Hadamard’s factorization theorem [49],
where C and \(C_{1}\) are constants depending on \(\{ \lambda_{n} \} \) and \(\{ \tau _{n} \} \), respectively. When \(\lambda_{n}=\tilde{\lambda}_{n}\) and \(\tau_{n}=\tilde{\tau}_{n}\) for all n, \(\Delta(\lambda)\equiv\tilde{\Delta}(\lambda)\) and \(\Delta_{1}(\tau )\equiv\tilde{\Delta}_{1}(\tau)\). Hence, \(\alpha_{1}^{\prime}\psi_{1}(a,\tau)-\alpha_{2}^{\prime}\psi_{2}(a,\tau)=\tilde{\alpha}_{1}^{\prime}\tilde{\psi}_{1}(a,\tau)-\tilde{\alpha}_{2}^{\prime}\tilde {\psi }_{2}(a,\tau)\). As a result, we get \(M(\lambda)=\tilde{M}(\lambda)\) by (21). So, the proof is completed by Theorem 2. □
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Güldü, Y. On discontinuous Dirac operator with eigenparameter dependent boundary and two transmission conditions. Bound Value Probl 2016, 135 (2016). https://doi.org/10.1186/s13661-016-0639-y
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DOI: https://doi.org/10.1186/s13661-016-0639-y