The existence of eigenvalue problems for the waveguide theory
© Maher and Karachevskii; licensee Springer 2012
Received: 5 April 2012
Accepted: 1 November 2012
Published: 13 November 2012
In this paper, the existence of the eigenvalue problem for the waveguide theory is investigated. We used the Fourier transformation method for the solution of this problem. Also, we applied this problem to a dielectric waveguide. In this study, four theorems and two lemmas are obtained.
MSC: 35A22, 35P10.
Keywordspartial differential equations eigenvalue problems Fourier transformation method
1 Basic preliminaries
in which for all and for all . If the boundary is sufficiently smooth, the condition of this junction may be put down in a natural form. Indeed, the contraction of is noninfinitely smooth in and , the functions which deteriorate their smoothness where the conditions themselves could be impossible to write. That is how the solution of this problem was progressing.
If the boundaries of domains are bad and there are several of them, it is not clear what the condition of the junction looks like. In this situation (connection), we need another approach to the solution of the set problem.
Since results of the junction must preserve the property of solution (being a generalized solution), we propose a new circuit system to solve the set problem. In general case, it is not solved.
It is obvious that if we prove the existence of the eigenvalue (3), we obtain the following solution of the problem (1) ; , , where they are found automatically joined by a required form.
2 Formulation of the problem
in which , if .
The problem (5) is self-adjoint. This can be easily seen if we use the Fourier transformation. However, it does not influence the eigenvalue existence. Some examples of the problem (5) are known (with concrete , N and ) both with and without eigenvalues.
for all u and .
From now on, if it is not specifically indicated, the notation is the norm in the space .
3 The existence of negative eigenvalues for the general case
for each sufficiently small and .
Theorem 1 The problem (6) has at least one negative eigenvalue if Ω is bounded.
It is necessary to introduce several lemmas before proving this theorem.
In each case, we consider . By virtue of (8), there is a function of the Fourier transformation which coincides with . Considering (7), the real and even function could be obtained.
Since outside Ω, then ; is the solution of the problem (11). If where in Ω we obtain for , by virtue of the latter equality . The necessity is proved.
Considering this inequality and (12), we obtain , i.e., is the solution of the problem (6). Thus, the lemma is proved. □
where Sup is determined for all the function , for which .
Hence, the first statement follows from (9).
δ will be chosen in a way such that for all and , . Since Ω is bounded, we may always obtain the latter.
Hence, by virtue of (10), the lemma is proved. □
When , we have the nonzero solution of the equation (11). It follows from Lemma 1 that is the eigenvalue of the problem (6).
are chosen in such a way that .
Considering the choice and the property , if , we can easily prove the boundedness of . Noting that when and for which , the operator is completely continuous. In this case, as we know, the set , contains the subsequence , which converges by norm where .
From (18) and (19) it follows that converges to by norm where . Then converges to by norm and satisfies the equality , i.e., when , the equation (11) has a nonzero solution. Hence, the theorem is proved. □
4 Application to the problem of a dielectric waveguide
It is clear that in the case of n arbitrary, these requirements are not satisfied. However, it takes place in the case important for the application. It can easily be proved when we use the spherical coordinates. Moreover, for the case when , (9) also takes place. Let us make sure that (10) is satisfied when .
when for all ; i.e., , outside , where at .
The theorem may be applied to the problem (21). As a consequence of this theorem, we get the following:
Theorem 2 If Ω is bounded, the problem (3) has an eigenvalue μ for which .
Now, we formulate the following theorem.
Theorem 3 The problem (3) does not have an eigenvalue μ for which .
If , , then by virtue of the condition , the latter is not impossible. □
By virtue of Theorems 2 and 3, we have
Theorem 4 Let be bounded. Then the problem (3) has an eigenvalue μ which satisfies the condition .
Remark If the condition that the bounded set is not valid, then the problem may not have eigenvalues.
This paper deals with the existence of eigenvalue problems for the waveguide theory. These problems are very important in the study of the mathematical analysis and mathematical physics. In this paper, we introduced four theorems and two lemmas.
We wish to thank the referees for their valuable comments which improved the original manuscript.
- Karchevskii EM: The research (investigation) of the numerical method of solving the spectral problem for the theory of dielectric waveguides. Izv. Vysš. Učebn. Zaved., Mat. 1999, 1: 10-17.MathSciNetGoogle Scholar
- Dautov RZ, Karchevskii EM: Existence and properties of solutions to the spectral problem of the dielectric waveguide theory. Comput. Math. Math. Phys. 2000, 40: 1200-1213.MathSciNetGoogle Scholar
- Karchevskii EM: The fundamental wave problem for cylindrical dielectric waveguides. Differ. Equ. 2000, 36: 998-999. 10.1007/BF02754500MathSciNetView ArticleGoogle Scholar
- Karchevskii EM, Solov’ev SI: Investigation of a spectral problem for Helmholtz operator on the plane. Differ. Equ. 2000, 36: 563-565.MathSciNetGoogle Scholar
- Pinasco JP: Asymptotic of eigenvalues and lattice points. Acta Math. Sin. Engl. Ser. 2000, 22(6):1645-1650.MathSciNetView ArticleGoogle Scholar
- Snyder A, Love D: Optical Waveguide Theory. Chapman & Hall, New York; 1987.Google Scholar
- Riss F, Sekefalvi-Nad B: Lectures on Functional Analysis. Mir, Moscow; 1979.Google Scholar