Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

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Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd , 2004

Transcript of Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Page 1: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Planar Waveguides

Michael MoeweEE290F, Professor Kaminow

March 2nd, 2004

Page 2: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Contents Planar Waveguides

Overview Uses

Infinitely wide planar waveguide theory Maxwells Equations in Slab Waveguide Simplifcation of Maxwell’s Equations TE and TM Mode Wavenumbers & Boundary Conditions Dispersion Curves Power Carried in Waveguide

Rectangular Waveguides Marcatili’s method of solving & E-field distribution Kumar’s method

Page 3: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Planar Waveguides: Overview

Similar function as optical fibers Easily fabricated on substrates

with a mask

Image from NTT-AT (http://www.keytech.ntt-at.co.jp/optic2/prd_e0015.html)

Page 4: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Uses for planar waveguides Routing Light Devices

Modulators Erbium Doped Planar Waveguide

Amplifiers (EDWA) (with curved guides) Resonators

http://www.ee.ic.ac.uk/optical/Optics.htmlhttp://www.netzartfedorov.com/clients/nanonics/newnanon/text-industry.html

Page 5: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Maxwells Equations in Slab Waveguide

Maxwell’s Equations

Simplifications

Page 6: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Simplifcation of Maxwell’s Equations

Substituting into Maxwell’s Equations

Page 7: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

TE and TM Mode

TE/TM Mode, No y-axis dependency

(and )TE Mode TM Mode

Page 8: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Wavenumbers

Fields are confined to core, so:

With wavenumbers:

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Boundary Conditions

Hz components continuous at boundaries, so based on previous eq:

Continuity of these boundaries gives:

Page 10: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Substitutions

Substitution:

Gives the relations:

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Dispersion Curves for TE and TM modes

Dispersion Curves

Page 12: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Power Carried in Waveguide

Power Equation

Simplifies to (for TE mode):

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Rectangular Waveguides (Marcatili’s method)

(Assumed no field in corner areas)

Page 14: Planar Waveguides Michael Moewe EE290F, Professor Kaminow March 2 nd, 2004.

Electric Field Distributions in Rectangular Waveguides

Marcatili’s Method: (assumes no field in corners of waveguide)

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Kumar’s method for Rectangular Waveguides

Finite Field inCorners

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References Okamoto K. 2000 Fundamentals of Optical Waveguides

(San Diego, CA: Academic) Prototype trial manufacture of polymer optical

waveguide. 2 Mar. 2004. NTT-AT. http://www.keytech.ntt-at.co.jp/optic2/prd_e0015.html

Nanonics – Industry Applications. 2 Mar. 2004. Nanonics. http://www.netzartfedorov.com/clients/nanonics/newnanon/text-industry.html

Syms R., Tate T., Syahriar A. Waveguide Devices by Electron Beam Irradiation of Silica. 2 Mar 2004. Imperial College of Science, Technology & Medicine. http://www.ee.ic.ac.uk/optical/Optics.html