Spectral theory of operator-valued functions (OFVs) envelops different solution techniques for operator eigenvalue problems with nonlinear dependence on the spectral parameter. This theory offers a universal approach to the solution of linear and nonlinear partial differential equations (PDEs), integral equations (IEs), and boundary value problems (BVP)s, and often when traditional methods fail, e.g. when nonselfadjoint BVPs are considered in unbounded domains and the spectral parameter enters the conditions at infinity in a nonlinear manner. Ideas and methods of the spectral theory of OFVs are now used in quite different areas: from qualitatively new approaches to the existence and uniqueness theorems for linear and nonlinear PDEs to new numerical methods and mathematical models (nature of resonance scattering, interaction phenomena, and others). The first studies date back to the works of Hilbert [1] and Giraud [2] published in the 1920s and 1930s. They considered in particular integral operators (and infinite determinants) with kernels depending on a complex parameter. Many important results were obtained by Keldysh [3] and other mathematicians in the 1950s who studied abstract operator pencils. A breakthrough was made by Gohberg [4] in the 1950s; he introduced main definitions and constructed foundations of the modern spectral theory of OFVs and proved on this basis the so-called analytical Fredholm theorem, according to which a Fredholm OVF A(z) acting in a Hilbert space and analytical with respect to the complex spectral parameter z may have not more than a finite set of characteristic numbers (CNs) in every bounded subdomain. This result was then generalized to the case of analytical Fredholm OVFs acting on a pair of Banach spaces. It was shown [5] that many statements of the theory of functions of one complex variable remain valid in the 'operator' case, in particular, the Rouchet's theorem [6]. Another significant contribution was made by Vainikko and coauthors in the 1970s [7] who performed a fine analysis of the spectrum of operator eigenvalue problems and justified in particular the approximate determination of CNs. Spectral theory of nonselfadjoint operators [8, 9] has been successfully applied to the solution of nonselfadjoint BVPs since the early 1950s. Beginning from the second half of the 1970s the methods of spectral theory of OFVs, which was a rapidly developing branch of the general nonselfadjoint spectral theory, found broad application as a powerful solution technique. Nonselfadjoint BVPs arise naturally in many branches of mathematical physics, first of all in the mathematical theory of wave propagation and diffraction (electromagnetis), and also in mechanics, elasticity, fluid dynamics [10—13]. BVPs for the Maxwell and Helmholtz equations in unbounded domains occupy a specific place: first, they are nonselfadjoint, and, second, the spectral parameter enters the boundary conditions in a nonlinear manner. Already correct statements of BVPs, especially eigenvalue problems meet substantial difficulties. The proof of unique solvability and determination of the spectrum require alternative techniques. Therefore specific methods are needed to investigate these problems. Some of them are reviewed in [14, 15]. In this respect, the spectral theory of OVFs clearly demonstrated advantages during the last two decades. Perturbation theory. The analysis of the dependence of eigenvalues of differential operators on parameters is a specific part of the perturbation theory [16] which also can be studied using the methods of the spectral theory of OVFs. This dependence can be described [16, 17] by functions of several complex variables that have critical points of various nature. Degeneration of eigenvalues as well as many important physical phenomena (e.g., resonance scattering and interaction of oscillations and waves) are shown to be connected with such points. The knowledge of critical points enables one to solve inverse problems because it gives a specific alternative description of the object (a characterization of the domain where the eigenvalue problem is considered and the equation parameters). The determination of critical points with respect to the different problem parameters and the analysis of the interaction phenomena are reviewed in [14] and recently, in [15]. Nonlinear equations. Development of the methods of solution to singular BVPs for the linear and nonlinear Helmholtz and Schrödinger equations with complex-valued coefficients is another field of application of the spectral theory of OVFs [18—20]. These problems can be reduced to nonlinear Volterra and Fredholm integral equations and their CNs are determined using contraction. Application to mathematical methods in electromagnetics. In the 1980s, the specific problem settings and mathematical models related to BVPs arising in electromagnetics and acoustics that are solved on the basis of the spectral theory of OVFs have become known under the common name of the spectral theory of open structures [14]; this theory was constructed and developed during the last two decades on the basis of the spectral theory of OVFs and specially developed methods using pseudodifferential equations [21]. References 1. D. Hilbert, Grundzüge einer allgemeinen Theorie der linearen Integralgleichungen, Leipzig (1924). 2. G. Giraud, Equations a integrales principales, Ann. Sci. Ec. Norm. Sup., 51, 251--272 (1934). 3. M. Keldysh, On the Characteristic Values and Characteristic Functions of Certain Classes of Nonelfadjoint Equations, Doklady Akad. Nauk SSSR Maths., 77, 11--14 1951). 4. I. Gohberg, On Linear Operators Depending Analytically on a Parameter, Doklady Akad. Nauk SSSR Maths., 78, 629--632 (1951). 5. I. Gohberg, ,M. Krein, Fundamental Aspects of Defect Numbers, Root Numbers and Indexes of Linear Operators, Uspehi Mat. Nauk, 12, 43--118 (1957). 6. I. Gohberg and E. Sigal, Operator Generalization of the Logarithmic Residue Theorem and Rouchet's Theorem, Mat. Sbornik, 84, 607--629 (1971). 7. G. Vainikko, O. Karma, The Convergence of Approximate methods for the Solution of Linear and Nonlinear Operator Equations, Zh. Vychisl. Mat. i Mat. Fiz., 14, 828--837 (1974). 8. I. Gohberg, M. Krein, Introduction to the Theory of Linear Nonselfadjoint Operators, Amer. Math. Soc., Providence, RI AMS (1969). 9. M. Reed, B. Simon, Methods of Modern Mathematical Physics, Academic Press, New York (1979). 10. C. Müller, Foundations of the Mathematical Theory of Electromagnetic Waves, Springer, New York, Berlin, Heidelberg (1969). 11. E. Sanchez-Palencia. Nonhomogeneous Media and Vibration Theory, Springer, New York, Berlin, Heidelberg (1980). 12. D. Colton, R. Kress, Integral Equation Methods in Scattering Theory, Wiley, New York (1983). 13. J-C. Nedelec, Acoustic and Electromagnetic Equations, Springer, New York, Berlin, Heidelberg (2000). 14. V. Shestopalov, Y. Shestopalov, Spectral Theory and Excitation of Open Structures, Peter Peregrinus Ltd, London (1996). 15. G. Hanson, A. Yakovlev, Operator Theory for Electromagnetics. An Introduction, Springer, New York, Berlin, Heidelberg (2001). 16. T. Kato, Perturbation Theory for Linear Operators, Springer, New York, Berlin, Heidelberg (1966). 17. V. Arnold, S. Gusein-Zade, A. Varchenko, Singularities of Differentiable Maps, Birkhäuser, Boston (1988). 18. H.W. Schürmann, V. Serov and Y. Shestopalov, TE-polarized Waves Guided by a Lossless Nonlinear Three-layer Structure, Physical Review E, 58, 1, pp. 1040--1050 (1998). 19. Y. Smirnov, H.W. Schürmann, and Y. Shestopalov, Integral Equation Approach for the Propagation of TE-Waves in a Nonlinear Dielectric Cylindrical Waveguide, J. Nonlin. Math. Phys., 11, 2, pp. 256--268 (2004). 20. Y. Smirnov, H.W. Schürmann, and Y. Shestopalov, Propagation of TE-waves in cylindrical nonlinear dielectric waveguides, Phys. Rev. E, 71, pp. 0166141-10 (2005). 21. A. Il'inski, Y. Smirnov, Electromagnetic Wave Diffraction by Conducting Screens, Y. Shestopalov, Ed., VSP Int. Science Publishers, Utrecht, Boston, Köln, Tokyo (1998).