Prove n1<N<n2 for effective index N....

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SUMMARY

The discussion focuses on proving the relationship n2 < N < n1 for the effective index N in a symmetric, 3-layer slab waveguide. The effective index is defined as N = n1sin(theta), where n1 is the refractive index of the core and n2 is the refractive index of the cladding. The participants clarify that for total internal reflection (TIR) to occur, N must be strictly less than n1, and they seek to establish the upper bound of N in relation to n2. The conclusion emphasizes that the effective index must satisfy the inequality n2 < N < n1 for guided modes.

PREREQUISITES
  • Understanding of Snell's Law and its application in optics.
  • Familiarity with the concept of total internal reflection (TIR).
  • Knowledge of refractive indices in optical waveguides.
  • Basic principles of waveguide theory, particularly for symmetric, multi-layer structures.
NEXT STEPS
  • Study the derivation of Snell's Law in the context of waveguides.
  • Explore the mathematical proof of total internal reflection conditions.
  • Investigate the properties of guided modes in optical waveguides.
  • Learn about the design and analysis of symmetric slab waveguides.
USEFUL FOR

Optical engineers, physicists, and students studying waveguide theory or working on optical communication systems will benefit from this discussion.

Alvis
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Homework Statement


Prove for effective index N that n1<N<n2.

Homework Equations


[/B]
N=n1sin(theta)
TIR is theta>thetacritical
snells law-n1sin(theta)=n2sin(theta2)

The Attempt at a Solution



I know why N is strictly less than n1 since sin(theta) goes from 0 to 1 and if its at 1 theta has to be 90. For TIR to actually happen N must be strictly less than n1. But I'm having trouble proving the n2<N part.
 
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Alvis said:
I know why N is strictly less than n1
Yet your "to be shown" has it > n1. Reversing that doesn't help since from Snell's law it should also be less than n2.
Please describe the set- up and define effective index. Even if it is a standard term, many on this forum would need to look it up.
 
Ah, my mistake. It should be show n2<N<n1.

Effective index is n1sin(theta). This is for the symmetric, 3-layer slab waveguide. The core thickness is d and its index is n1. The clad indices have the same value of n2.
My task is to prove the effective index N of any of the guided modes obeys the relationships n2<N<n1.

I know N<n1 because in(theta) goes from 0 to 1. If it is at 1, theta must be 90 degrees, meaning the light never hit the surface in front of the plane. Therefore, for TIR to actually happen, N must be strictly less than n1.

My apologies!
 
Alvis said:
Ah, my mistake. It should be show n2<N<n1.

Effective index is n1sin(theta). This is for the symmetric, 3-layer slab waveguide. The core thickness is d and its index is n1. The clad indices have the same value of n2.
My task is to prove the effective index N of any of the guided modes obeys the relationships n2<N<n1.

I know N<n1 because in(theta) goes from 0 to 1. If it is at 1, theta must be 90 degrees, meaning the light never hit the surface in front of the plane. Therefore, for TIR to actually happen, N must be strictly less than n1.

My apologies!
Ok.
Snell's Law is for a wave which penetrates the boundary. Your wave at angle theta is to be reflected.
If N<n2, what will happen?
 

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