Multilayer model in optics. New analitic results. M.D.Kovalev BMSTU mdkovalev@mtu-net.ru.

Презентация:



Advertisements
Похожие презентации
PAT312, Section 21, December 2006 S21-1 Copyright 2007 MSC.Software Corporation SECTION 21 GROUPS.
Advertisements

Schrodingers Equation for Three Dimensions. QM in Three Dimensions The one dimensional case was good for illustrating basic features such as quantization.
1 Another useful model is autoregressive model. Frequently, we find that the values of a series of financial data at particular points in time are highly.
Time-Series Analysis and Forecasting – Part IV To read at home.
Derivation of modified Smyshlyaev's formulae using integral transform of Kontorovich-Lebedev type Valyaev V. Yu, Shanin A.V Moscow State University Days.
Multiples Michael Marchenko. Definition In mathematics, a multiple is the product of any quantity and an integer. in other words, for the quantities a.
AVL-Trees COMP171 Fall AVL Trees / Slide 2 Balanced binary tree * The disadvantage of a binary search tree is that its height can be as large as.
Quadratic sequences. If the difference between the terms changes, this is called a quadratic sequence. If you use the formula n 2 + n to make a sequence,
S12-1 NAS122, Section 12, August 2005 Copyright 2005 MSC.Software Corporation SECTION 12 RESIDUAL VECTOR METHOD.
How can we measure distances in open space. Distances in open space.
S16-1 NAS122, Section 16, August 2005 Copyright 2005 MSC.Software Corporation SECTION 16 COMPLEX MODAL ANALYSIS.
© 2009 Avaya Inc. All rights reserved.1 Chapter Two, Voic Pro Components Module Two – Actions, Variables & Conditions.
BREADTH FIRST TRAVERSAL Lesson Plan -3. Evocation.
Here are multiplication tables written in a code. The tables are not in the correct order. Find the digit, represented by each letter.
Linear Block Codes Mahdi Barhoush Mohammad Hanaysheh.
7/23/ :59:31 AMRefresher course in Chemistry; Sept.20-Oct.12, Magnetic Resonance Phenomenon is a manifestation due to the presence of INTRINSIC.
WS6-1 PAT328, Workshop 6, May 2005 Copyright 2005 MSC.Software Corporation WORKSHOP 6 NESTED COORDINATE SYSTEMS.
S8-1 PAT325, Section 8, February 2004 Copyright 2004 MSC.Software Corporation SECTION 8 RESULTS FOR PLIES.
Our City – Kursk. Presentation about the city. Presentation was created by pupil of the 10A class – Losev Vladimir.
WS9-1 PAT328, Workshop 9, May 2005 Copyright 2005 MSC.Software Corporation WORKSHOP 9 PARAMETERIZED GEOMETRY SHAPES.
Транксрипт:

Multilayer model in optics. New analitic results. M.D.Kovalev BMSTU

Planar multilayer waveguide

For ТЕ-waves propagating along Oz axis this is a boundary-value problem for the equation

Reduced variables

First example. 7 layers. The number of ТЕ-modes: K=6.

Traditional dispersion equations –equations for the eigenvalues of the propagation constant Type 1 – equation, is obtained by equating to zero of the determinant of homogenius linear system due to boundary conditions. Type 2 equation, obtained by the known method of characteristic matrices This equations have too many terms if the number of layers is more then 4. Investigation of waveguides with many layers is now actual.

The properties of the dispersion equations Th.1. Type 1 equation has roots, coinsiding with the refraction indexes of the inner layers of the waveguide. This roots may not be the eigenvalues of propagation constant. Th.2. The set of roots of type 2 equation is exactly the set of the eigenvalues of propagation constant. We propose a new one form of the dispersion equation. This equation in some known cases have no parasitic roots, and moreover it may be treated geometrically.

Multilayer equation

Homogenius variables,vectors

Vectors

Theorem 3. Vectors rotate counter-clockwise when is decreasing. Theorem 4. If then the directions of this vectors are converging to the direction of Ox axis.

The multilayer equation in vector form

The formulae for the number of TE-modes.

Transform

The second example, K=7. The difference from the first example is only

Thank you for the attention Ковалев М.Д., Число TE- и TM-мод в многослойном планарном волноводе со слоями двух типов. Электромагнитные волны и электронные системы, 2009, т. 14, 2, С Ковалев М.Д. Многослойное уравнение. Чебышевский сборник. Тула, т. 7, выпуск 2 (18), 2006, С Майер А.А., Ковалев М.Д.. Дисперсионное уравнение для собственных значений эффективного показателя преломления в многослойной волноводной структуре. ДАН, 2006, т. 407, 6, С Ковалев М.Д., Многослойная модель в оптике и квантовой механике. ЖВМ и МФ, 2009, т. 49, 8, С Ковалев М.Д., Об энергетических уровнях частицы в гребенчатой структуре. ДАН, 2008, Том 419, 6, С