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Title: Guidance properties of a cylindrical defocusing waveguide (English)
Author: John, Oldřich
Author: Stuart, Charles A.
Language: English
Journal: Commentationes Mathematicae Universitatis Carolinae
ISSN: 0010-2628 (print)
ISSN: 1213-7243 (online)
Volume: 35
Issue: 4
Year: 1994
Pages: 653-673
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Category: math
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Summary: We discuss the propagation of electromagnetic waves of a special form through an inhomogeneous isotropic medium which has a cylindrical symmetry and a nonlinear dielectric response. For the case where this response is of self-focusing type the problem is treated in [1]. Here we continue this study by dealing with a defocusing dielectric response. This tends to inhibit the guidance properties of the medium and so guidance can only be expected provided that the cylindrical stratification is such that guidance would occur for the linear response that is obtained in the limit of zero field strength. The guided modes that we seek correspond to solutions of the boundary value problem $-u'' + \frac 34 \frac u{r^2} - q(r) u + p( r, u ) u = \lambda u $ for $r > 0$ with $ u \in H^1_0 ( 0, \infty )$ and its linearisation is $-u'' + \frac 34 \frac u{r^2} - q( r ) u = \lambda u$ with $ u \in H_0^1 ( 0, \infty )$. This linear problem has the interval $[0, \infty )$ as its essential spectrum and the requirement that guidance should occur in the limit of zero field strength leads us to suppose that it has at least one negative eigenvalue. Solutions of the nonlinear problem are then obtained by bifurcation from such an eigenvalue. The main interest concerns the global behaviour of a branch of solutions since this determines the principal features of the waveguide. If the branch is bounded in $ L^2 ( 0, \infty )$ there is an upper limit to the intensity of the guided beams (high-power cut-off), whereas if the branch is unbounded in $ L^2 ( 0, \infty )$ then guidance is possible at arbitrarily high intensities. Our results show how these behaviours depend upon the properties of dielectric response. (English)
Keyword: Schrödinger's equation
Keyword: waveguides
MSC: 34A47
MSC: 34B15
MSC: 34C23
MSC: 35Q60
MSC: 47H15
MSC: 78A50
idZBL: Zbl 0819.35137
idMR: MR1321236
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Date available: 2009-01-08T18:14:10Z
Last updated: 2012-04-30
Stable URL: http://hdl.handle.net/10338.dmlcz/118707
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Reference: [1] Stuart C.A.: Self-trapping of an electromagnetic field and bifurcation from the essential spectrum.Arch. Rat. Mech. Anal. 113 (1991), 65-96. Zbl 0745.35044, MR 1079182
Reference: [2] Stuart C.A.: Global properties of components of solutions of nonlinear second order ordinary differential equations on the half-line.Ann. Sc. Norm. Sup. Pisa II (1975), 265-286. MR 0380013
Reference: [3] Stuart C.A.: The behaviour of branches of solutions of nonlinear eigenvalue problems.Rend. Ist. Matem. Univ. Trieste XIX (1987), 139-154. Zbl 0667.34027, MR 0988378
Reference: [4] Kato T.: Perturbation Theory for Linear Operators.Springer-Verlag Berlin (1966). Zbl 0148.12601, MR 0203473
Reference: [5] Weidmann J.: Linear Operators in Hilbert Space.Springer-Verlag Berlin (1980). MR 0566954
Reference: [6] Eastham, M.S.P.: Theory of Ordinary Differential Equations.Van Nostrand (1970). Zbl 0195.37001
Reference: [7] Akhmanov R.V., Khokhlov R.V., Sukhorukov A.P.: Self-focusing, self-defocusing and self-modulation of laser beams.Laser Handbook (ed. by F.T. Arecchi and E.O. Schulz Dubois), North Holland, Amsterdam, 1972.
Reference: [8] Mathew J.G.H., Kar A.K., Heckenberg N.R., Galbraigth I.: Time resolved self-defocusing in InSb at room temperature.IEEE J. Quantum Elect. 21 (1985), 94-99.
Reference: [9] Stegeman G.I., Wright E.M., Seaton C.T., Moloney J.V., Shen T.-P., Maradudin A.A., Wallis R.F.: Nonlinear slab-guided waves in non-Kerr-like media.IEEE J. Quantum Elect. 22 (1986), 977-983.
Reference: [10] Stuart C.A.: Guidance Properties of Nonlinear Planar Waveguides.Arch. Rational Mech. Anal. 125 (1993), 145-200. Zbl 0801.35136, MR 1245069
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