Fabry-Perot Interferometer: Energy Conservation

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SUMMARY

The discussion centers on the behavior of light in a Fabry-Perot Interferometer with identical mirrors, specifically addressing the phenomenon where 100% of the light appears to be transmitted despite initial conditions suggesting otherwise. The mathematical explanation provided utilizes the equation I_t = I_0 * {T^2 / (1-R^2)} * {1 / (1 + F * sin^2(\Delta/2))}, demonstrating that when the phase difference \Delta is an integer multiple of pi, the transmitted intensity I_t equals the original intensity I_0. This indicates that energy conservation is maintained, as the system allows for complete transmission under specific conditions.

PREREQUISITES
  • Understanding of Fabry-Perot Interferometer principles
  • Familiarity with optical properties such as transmittance (T) and reflectance (R)
  • Knowledge of phase differences in wave optics
  • Ability to manipulate and interpret mathematical equations related to optics
NEXT STEPS
  • Study the mathematical derivation of the Fabry-Perot Interferometer equations
  • Explore the concept of finesse (F) in optical systems
  • Research the physical implications of phase differences in interference patterns
  • Examine practical applications of Fabry-Perot Interferometers in spectroscopy
USEFUL FOR

Students and professionals in optics, physicists, and engineers interested in understanding the principles of light behavior in interferometric systems and energy conservation in optical setups.

smithg86
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Homework Statement



This is regarding a Fabry-Perot Interferometer with identical mirrors:

If you shine a beam of light on a 99% reflecting mirror, 1% goes through and the other 99% is reflected. But if a second mirror is placed behind the first one, where there is only 1% of the light present, somehow 100% of the light appears. Explain this, also explain how energy is conserved.

Homework Equations



I_t = I_0 * {T^2 / (1-R^2)} * { 1 / (1 + F * sin^2([tex]\Delta[/tex]/2))}

F = finesse = 4R / (1-R)^2

I_t = transmitted intensity
I_0 = original intensity

T = transmittance
R = reflectance

[tex]\Delta[/tex] = [tex]\delta[/tex] + [tex]\delta[/tex]_r
[tex]\delta[/tex] = phase difference per round trip between mirrors
[tex]\delta[/tex]_r = phase difference due to reflection = 0 or pi

The Attempt at a Solution



I understand mathematically why it's true. If you set [tex]\Delta[/tex] to an integer multiple of pi, then sin [tex]\Delta[/tex] = 0 and then

I_t/I_0 = {T^2 / (1-R^2)} * { 1 / (1 + F*(0)) }

I_t/I_0 = T^2 / (1 - R^2) = 1

so I_t = I_0, so 100% of the light appears.

I really don't know how to explain this physically. Help?
 
Last edited:
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Can you write down the question EXACTLY as it was given to you?

I can't seem to make much sense of it. First of all, the interferometer set-up I'm familiar with has the mirrors facing each other, not one behind the other. Secondly, in this geometry, I expect that only about half the incident power is transmitted through in the forward direction, the rest is transmitted backwards.

What does the question mean by "100% of the light appears"? Appears where?

I may be completely off here, so it would help if someone else takes a look.
 
"I really don't know how to explain this physically. Help?"

Has anyone an answer to this question?

That is the question of my life too.
 

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