Relativistic Particle Collisions with Photons: Understanding Momentum and Energy

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Discussion Overview

The discussion revolves around relativistic particle collisions involving photons and pions, focusing on the transformation of energy and momentum in different reference frames. Participants explore the implications of these transformations on collision outcomes and the conditions necessary for particle production.

Discussion Character

  • Exploratory
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether it is possible to use a frame where the pion is at rest, suggesting that the momentum of the photon remains constant across frames due to its speed being c.
  • Another participant asserts that it is indeed possible to have a frame where the pion is at rest, emphasizing that the energy and momentum of the photon do change with different frames.
  • Some participants discuss the transformation properties of the photon’s four-vector and its implications for energy and momentum conservation, referencing the Doppler effect as an example.
  • A participant expresses confusion about the relationship between the speed of the photon and its momentum in different frames but acknowledges understanding after further explanation.
  • In a follow-up question, a participant presents a scenario involving energy conservation and momentum conservation equations for producing a particle N from a photon and a pion, noting discrepancies between the two approaches.
  • Another participant suggests that the equations can be solved for the energies involved, indicating that there is a specific energy configuration required to produce particle N at rest.
  • One participant challenges the formulation of one of the equations presented, indicating a potential error in the energy conservation equation.

Areas of Agreement / Disagreement

Participants express differing views on the possibility of using a rest frame for the pion and the implications of energy and momentum transformations. The discussion includes corrections and challenges to earlier claims, indicating that multiple competing views remain without a clear consensus.

Contextual Notes

Participants reference specific equations and conservation laws, but there are unresolved aspects regarding the conditions under which particle N can be produced at rest, as well as the correct formulation of the equations involved.

soupdejour
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I have never done relativistic collisions when a photon is involved, and it's messing wtih me.

For example, I have a photon colliding with a pion moving at a speed 3c/4. Is it possible to use a frame so that the pion is at rest? I think not, because the momentum of the photon is the same in all frames because it travels at c.

Or does the momentum or energy of the photon change in different frames?
 
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soupdejour said:
Is it possible to use a frame so that the pion is at rest?
Yes, the pion has a finite (non-vanishing) mass of approximately 135 or 139 MeV.
soupdejour said:
does the momentum or energy of the photon change in different frames?
Certainly yes. Energy and momentum of a photon depend on the frame, and as usual for the components of a 4-vector, their transformation is such that the corresponding mass is conserved (here zero mass). The Lorentz transformation of a photon 4-vector is how the Doppler red(blue)shift formula is derived for instance.
 
soupdejour said:
For example, I have a photon colliding with a pion moving at a speed 3c/4. Is it possible to use a frame so that the pion is at rest?
Yes, of course, it is well possible.
I think not, because the momentum of the photon is the same in all frames because it travels at c.
No, your conclusion is wrong. The energy-momentum is a four-vector that transforms from one reference frame to another as any four-vector.
 
Bob S said:
Transfer to the pion rest frame. The photon energy increases.

It is only in case when the momenta of involved particles have opposite signs.
 
humanino said:
The Lorentz transformation of a photon 4-vector is how the Doppler red(blue)shift formula is derived for instance.

OK, I think I can visualize the wavelength of light changing in different frames.

I was confused that the momentum was different in different frames even though the speed was the same (c). But it makes sense that a photon just has a special four vector with "length" zero.

Thanks to both of you.
 
A closely related follow-up question:

If I have a photon colliding with this pion, and I want to try to find the minimum energy of the pion to create some particle N. I know the mass of N and the wavelength of the photon.

\gamma + \pi \rightarrow N

For the minimum energy of pion to produce N, I just make N at rest.

I do energy conservation:

E_{\pi} = m_{N} c^2 - E_{\gamma}

If I do 3-momentum conservation:

E_{\pi} = \sqrt{ m_{p}^2 c^4 + E_{\gamma}^2 }

These two equations give me different answers! Is it possible that the N cannot be produced at rest? Thats weird...
 
Last edited:
You have two equations in two unknowns. You can certainly solve them for E_\pi and E_\gamma. This just means that, for a given m_N, there is only one specific value for each of the energies that will produce and N at rest.
 
Your second equation is wrong. It should be E_gamma+e_pi=m_N.
 
  • #10
Parlyne said:
You have two equations in two unknowns. You can certainly solve them for E_\pi and E_\gamma. This just means that, for a given m_N, there is only one specific value for each of the energies that will produce and N at rest.

Right. So for a given frequency of light, it isn't necessarily possible to produce N at rest. Only one frequency can produce N at rest.

Thanks!
 

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