What is the correction to the wavelength of an emitted photon due to recoil?

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Homework Help Overview

The discussion revolves around the correction to the wavelength of an emitted photon due to the recoil of the emitting atom. The problem is situated within the context of momentum conservation and energy transfer during photon emission, specifically addressing how the recoil affects the wavelength of the emitted photon.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between the energy of the photon and the recoil of the atom, questioning the assumptions made about energy conservation and momentum. Some express frustration over deriving the correction to the wavelength, while others reference similarities to Compton scattering.

Discussion Status

The discussion is ongoing, with participants providing insights and corrections to each other's reasoning. Some guidance has been offered regarding the relationship between the energies involved, and there are indications of multiple interpretations being explored.

Contextual Notes

Participants are grappling with the implications of the recoil on the energy of the emitted photon and the resulting wavelength correction. There is mention of the smallness of the correction and the need for approximations, as well as references to specific equations and their derivations.

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Homework Statement



When a photon is emitted by an atom, the atom must recoil to conserve momentum. This means that the photon and the recoiling atom share the transition energy. (a) For an atom with mass m, calculate the correction Δλ due to recoil to the wavelength of an emitted photon. Let λ be the wavelength of the photon if recoil is not taken into consideration. (Hint: The correction is very small, so use this fact to obtain an approximate but very accurate expression for Δλ.)

Homework Equations

The Attempt at a Solution


[/B]
E = energy of system
E' = energy of the photon
K = kinetic energy of the atom
Conservation of energy gives: Einitial = Efinal
0 = K + E'
0.5 x mv² = - (hc / λ)

By conservation of momentum:
0 = pphoton + patom
mv = - (h / λ)

Solving the above equations, we get:
λ = h / 2mc

The book's answer is h / 2mc. The problem is that the speed found here is twice greater than c. :H
 
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This isn't correct. It's true that the momenta of the photon and the atom are equal and opposite. But it isn't true that the energy of the photon is equal to the energy of the atom. In fact the energy of the atom is much less than the energy of the photon. You are supposed to calculate how much the emitted energy of the photon is reduced by the momentum carried by the atom as compared to the energy of the photon if the atom doesn't carry away any energy.
 
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I noticed that the equation for Δλ in this case is the same as for Compton scattering if we take angles such as the direction of our "new" wavelength is the same as the "older" wavelength. I've tried working this problem several different ways and I don't get the Δλ. :cry: It's annoying.
 
kent davidge said:
I've tried working this problem several different ways.
Perhaps you could post one.
Did you understand phyzguy's comment? Do you have some revisions as a result?
 
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phyzguy thank you for remembering me that the change in the wavelength is due to the change in the energy.
haruspex I think what I posted below is finally the correct answer.

I got it

Eatom before = Eatom final + Ephoton
(mc² - pphotonc)² = (mc²)² + (patomc)²
...
pphoton / 2mc = -(patom² / pphoton2mc) + 1
Using the fact that the momentum of the atom is equal to the negative momentum of the photon and p = h / λ, results:
λ = h / mc
Now, the atom doesn't move at all:
pphoton / 2mc = -0 + 1
and
λ' = h / 2mc

|Δλ| is then λ' - λ = h / 2mc.
 
Last edited:

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