Spectrum of the quadratic eigenparameter dependent discrete Dirac equations
© Koprubasi; licensee Springer. 2014
Received: 26 February 2014
Accepted: 5 May 2014
Published: 16 May 2014
Let us consider the Boundary Value Problem (BVP) for the discrete Dirac equations , , , , where , , and , are complex sequences, , , and λ is an eigenparameter. Discussing the eigenvalues and the spectral singularities, we prove that this BVP has a finite number of eigenvalues and spectral singularities with a finite number of multiplicities, if , holds, for some and .
MSC:34L40, 47A10, 47A75.
In the last decade, discrete boundary value problems have been intensively studied. The spectral analysis of the difference equations have been treated by various authors in connection with the classical moment problem (see the monographs of Agarwal , Agarwal-Wong  and Kelley-Peterson  and the papers of Agarwal et al. [4, 5] and the references therein). Moreover, the modeling of certain linear and nonlinear problems in economies, optimal control theory, and other areas of study have led to the rapid development of the theory of difference equations. The spectral theory of the difference equations has also been applied to the solution of classes of nonlinear discrete Korteweg-de Vries equations and Toda lattices [6, 7].
where and are complex sequences, and λ is a spectral parameter. The spectral analysis of the BVP (1.1), (1.2) with continuous and point spectrum has been studied in . In this article, the authors proved that the spectrum of the BVP (1.1), (1.2) consists of a continuous spectrum, eigenvalues and a spectral singularities. The spectral singularities are poles of the resolvent and are also imbedded in the continuous spectrum, but they are not eigenvalues. The effect of the spectral singularities in the spectral expansion of the BVP (1.1), (1.2) in terms of the principal vectors has been investigated in . In [10, 11], the dependence of the structure of the spectral singularities of the BVP (1.1), (1.2) on the behavior of the sequences and was considered. Some problems related to the spectral analysis of difference equations with spectral singularities have been discussed in [12–15]. The spectral analysis of an eigenparameter dependent non-selfadjoint BVP for the system of difference equations of first order has been studied in [16, 17].
(see , Chapter 2). Therefore the system (1.5) (also (1.3)) is called a discrete Dirac system. The specific feature of this paper is the presence of the spectral parameter not only in the difference equation and also in the boundary condition, which is quadratic.
holds, for some and .
2 Jost solution of (1.3)
holds, where is a constant and is the integer part of . Therefore is a vector-valued analytic function with respect to z in and continuous in . The solution is called the Jost solution of (1.3).
3 Eigenvalues and spectral singularities of (1.3)-(1.4)
Definition 3.1 The multiplicity of a zero of F in T is called the multiplicity of the corresponding eigenvalue or spectral singularity of the BVP (1.3), (1.4).
It follows from (3.2) and (3.3) that, in order to investigate the quantitative properties of the eigenvalues and the spectral singularities of the BVP (1.3), (1.4), we need to discuss the quantitative properties of the zeros of F in T.
We also denote the set of all limit points of by and the set of all zeros of F with infinite multiplicity by .
The set is bounded and countable.
The set is compact and , where μ denotes the Lebesgue measure in the real axis.
, ; .
Equation (3.11) shows that is bounded. Since F is analytic in and is a 4π periodic function, we find that has at most a countable number of elements. This proves (i).
From the uniqueness theorems of analytic functions we obtain (ii)-(iv) .
Using the continuity of all derivatives of F on we get (v). □
From (3.10) and Theorem 3.1, we have the following.
The set of eigenvalues of the BVP (1.3), (1.4) is bounded and countable and its limit points can lie only in .
, and .
Theorem 3.3 Under the condition (3.12) the BVP (1.3), (1.4) has a finite number of eigenvalues and spectral singularities and each of them is of finite multiplicity.
where is a constant. From (3.6) and (3.13) we observe that the function F has an analytic continuation to the half-plane . Since F is a 4π periodic function, the limit points its zeros in T cannot lie in . Using Theorem 3.1 we have the bounded sets and having a finite number of elements. From analyticity of F in , we find that all zeros of F in T have a finite multiplicity. Therefore using (3.10), we obtain the finiteness of the eigenvalues and spectral singularities of the BVP (1.3), (1.4). □
It is seen that the condition (3.12) guarantees the analytic continuation of F from the real axis to lower half-plane. So the finiteness of eigenvalues and spectral singularities of the BVP (1.3), (1.4) are obtained as a result of this analytic continuation.
which is weaker than (3.12). It is evident that under the condition (3.14) the function F is analytic in and infinitely differentiable on the real axis. But F does not have an analytic continuation from the real axis to lower half-plane. Therefore under the condition (3.14) the finiteness of eigenvalues and spectral singularities of the BVP (1.3), (1.4) cannot be shown in a way similar to Theorem 3.3.
Under the condition (3.14), to prove that the eigenvalues and the spectral singularities of the BVP (1.3), (1.4) are of finite number we will use the following.
Theorem 3.4 ()
where and is the Lebesgue measure of s-neighborhood of G and is an arbitrary constant, then in .
where D and d are constants depending on C, ε, and δ.
Theorem 3.5 If (3.14) holds, then .
Since , (3.19) holds for arbitrary s if and only if or . □
Theorem 3.6 Under the condition (3.14) the BVP (1.3), (1.4) has a finite number of eigenvalues and spectral singularities and each of them is of finite multiplicity.
Proof To be able to prove the theorem we have to show that the function F has a finite number of zeros with finite multiplicities in T.
From Theorem 3.1 and Theorem 3.5 we see that . So the bounded sets and have no limit points, i.e., the function F has only a finite number of zeros in T. Since , these zeros are of finite multiplicity. □
- Agarwal RP: Difference Equation and Inequalities: Theory, Methods and Applications. Dekker, New York; 2000.MATHGoogle Scholar
- Agarwal RP, Wong PJY: Advanced Topics in Difference Equations. Kluwer Academic, Dordrecht; 1997.View ArticleMATHGoogle Scholar
- Kelley WG, Peterson AC: Difference Equations: An Introduction with Applications. Academic Press, San Diego; 2001.MATHGoogle Scholar
- Agarwal RP, Perera K, O’Regan D: Multiple positive solutions of singular and nonsingular discrete problems via variational methods. Nonlinear Anal. 2004, 58: 69–73. 10.1016/j.na.2003.11.012MathSciNetView ArticleMATHGoogle Scholar
- Agarwal RP, Perera K, O’Regan D: Multiple positive solutions of singular discrete p -Laplacian problems via variational methods. Adv. Differ. Equ. 2005, 2005(2):93–99.MathSciNetView ArticleMATHGoogle Scholar
- Berezanski YM: Integration of nonlinear difference equations by the inverse spectral problem method. Sov. Math. Dokl. 1985, 31: 264–267.Google Scholar
- Toda M: Theory of Nonlinear Lattices. Springer, Berlin; 1981.View ArticleMATHGoogle Scholar
- Bairamov E, Cakar O, Krall AM: Non-selfadjoint difference operators and Jacobi matrices with spectral singularities. Math. Nachr. 2001, 229: 5–14. 10.1002/1522-2616(200109)229:1<5::AID-MANA5>3.0.CO;2-CMathSciNetView ArticleMATHGoogle Scholar
- Krall AM, Bairamov E, Cakar O: Spectral analysis of non-selfadjoint discrete Schrödinger operator with spectral singularities. Math. Nachr. 2001, 231: 89–104. 10.1002/1522-2616(200111)231:1<89::AID-MANA89>3.0.CO;2-YMathSciNetView ArticleMATHGoogle Scholar
- Adivar M, Bairamov E: Spectral properties of non-selfadjoint difference operators. J. Math. Anal. Appl. 2001, 261: 461–478. 10.1006/jmaa.2001.7532MathSciNetView ArticleMATHGoogle Scholar
- Adivar M, Bairamov E: Difference equations of second order with spectral singularities. J. Math. Anal. Appl. 2003, 277: 714–721. 10.1016/S0022-247X(02)00655-8MathSciNetView ArticleMATHGoogle Scholar
- Adivar M, Bohner M: Spectral analysis of q -difference equations with spectral singularities. Math. Comput. Model. 2006, 43(7–9):695–703.MathSciNetView ArticleMATHGoogle Scholar
- Adivar M, Bohner M: Spectrum and principal vectors of second order q -difference equations. Indian J. Math. 2006, 48(1):17–33.MathSciNetMATHGoogle Scholar
- Bairamov E, Celebi AO: Spectrum and spectral expansion for the non-selfadjoint discrete Dirac operators. Q. J. Math. 1999, 50(2):371–384.MathSciNetView ArticleMATHGoogle Scholar
- Bairamov E, Coskun C: Jost solutions and the spectrum of the system of difference equations. Appl. Math. Lett. 2004, 17: 1039–1045. 10.1016/j.aml.2004.07.006MathSciNetView ArticleMATHGoogle Scholar
- Bairamov E, Koprubasi T: Eigenparameter dependent discrete Dirac equations with spectral singularities. Appl. Math. Comput. 2010, 215: 4216–4220. 10.1016/j.amc.2009.12.043MathSciNetView ArticleMATHGoogle Scholar
- Aygar Y, Olgun M, Koprubasi T: Principal functions of nonselfadjoint discrete Dirac equations with spectral parameter in boundary conditions. Abstr. Appl. Anal. 2012., 2012: Article ID 924628Google Scholar
- Levitan BM, Sargsjan IS Translations of Mathematical Monographs 39. Introduction to Spectral Theory 1975.Google Scholar
- Dolzhenko EP: Boundary value uniqueness theorems for analytic functions. Math. Notes 1979, 26(6):437–442.MathSciNetView ArticleMATHGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.