Compton scattering; conservation of momentum violated?

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SUMMARY

The discussion centers on the apparent violation of conservation of momentum in Compton scattering, specifically regarding the momentum gained by the electron compared to the momentum lost by the photon. Participants clarify that while the magnitudes of the momenta are not equal due to their vector nature, the conservation of total 4-momentum is upheld. The energy-momentum 4-vector, which includes both energy and momentum, conserves each component separately, thus resolving the confusion surrounding momentum conservation in this context.

PREREQUISITES
  • Understanding of Compton scattering and its implications in quantum mechanics.
  • Familiarity with the concept of 4-momentum in special relativity.
  • Knowledge of vector quantities and their properties in physics.
  • Basic principles of conservation laws in physics.
NEXT STEPS
  • Study the derivation of the Compton scattering formula, \(\lambda' - \lambda = \frac{h}{m_ec}(1 - \cos(\theta))\).
  • Learn about the energy-momentum 4-vector and its role in special relativity.
  • Explore the differences between 3-momentum and 4-momentum conservation laws.
  • Investigate vector addition and the implications of directionality in momentum conservation.
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Physicists, students of quantum mechanics, and anyone interested in the principles of momentum conservation in particle interactions.

Fosheimdet
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While reading the derivation of the formula \lambda' - \lambda = \frac{h}{ m_ec}(1-cos(\theta)) on Wikipedia, they point out that the momentum gained by the electron is larger than the momentum lost by the photon:

$$ p_e=\frac{\sqrt{h^2(\nu-\nu')^2 +2h(\nu-\nu')m_ec^2}}{c} > \frac{h(\nu-\nu')}{c} = p_{\gamma}-p_{\gamma'} $$

How is this not a violation of conservation of momentum?
 
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I don't think that's the right of way talking about it! When we consider SR in analysing phenomena, we should keep in mind that it is no longer true that energy and momentum are separately conserved, but it is the total 4-momentum P^\mu=(\frac E c, \vec p) which is conserved. So such a comparison has no meaning and violates nothing!
 
Fosheimdet said:
How is this not a violation of conservation of momentum?

Momentum is a vector quantity. The incoming and outgoing photons are in different directions. The difference in the magnitudes of their momenta is not a meaningful physical quantity, as far as I know.
 
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Shyan, what you wrote is wrong. It is not necessary to reply to every single question here, particularly if you don't know the answer. If the energy-momentum 4-vector (or any 4-vector) is conserved, each and every component is separately conserved.

jtbell - and Wikipedia - has it right. Comparing the magnitudes of two vectors is, in general (and in this particular case) comparing them along two different directions. You don't expect equality here.
 
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Vanadium 50 said:
If the energy-momentum 4-vector (or any 4-vector) is conserved, each and every component is separately conserved.

...but the magnitude of the 3-momentum is not. (just to make this explicit)
 
I don't think that helps. The magnitude of the 3-momentum component is conserved, since each of the three components is conserved separately. What we have here is a comparison between two 3-vectors pointing in two different directions. These are, as you said, not going to be equal. You would only get equality if you compared the total initial 4-momentum with the total final 4-momentum.
 
You're right, that was a bad way to put it. I was thinking of the fact that the magnitude of the 3-momentum is not "additive". That is, the sum of the magnitudes of two momenta does not generally equal the magnitude of the total momentum.

Vanadium 50 said:
The magnitude of the 3-momentum component is conserved

Right, the magnitude of the total momentum is conserved. Before the interaction, the total momentum is the incoming photon's momentum. Afterwards, the total momentum is the sum of the outgoing photon's momentum and the recoiling electron's momentum. The magnitude of the sum is smaller than the magnitude of the outgoing photon's momentum.
 

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