Special Relativity: Pion Decay - Two Photons

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SUMMARY

The discussion focuses on the decay of a neutral pion (π0 meson) with a rest mass of 135 MeV/c² and a kinetic energy of 1 GeV, which decays into two photons. The key equations utilized include the invariant mass equation E² = P²c² + m²c⁴ and conservation laws for energy and momentum in both the lab frame and the zero momentum frame (ZMF). The solution involves calculating the energies of the two photons by applying the Doppler shift after determining their energies in the ZMF. The final energies are derived through a systematic approach using gamma factors and conservation principles.

PREREQUISITES
  • Understanding of special relativity concepts, particularly invariant mass and energy-momentum relations.
  • Familiarity with conservation laws in physics, specifically conservation of energy and momentum.
  • Knowledge of the Doppler effect as it applies to relativistic particles.
  • Proficiency in using gamma factors in relativistic equations.
NEXT STEPS
  • Study the derivation and application of the invariant mass equation in particle physics.
  • Learn about the Doppler effect in the context of relativistic particles and its mathematical formulation.
  • Explore examples of particle decay processes and their energy-momentum conservation solutions.
  • Investigate the concept of the zero momentum frame (ZMF) and its significance in analyzing particle interactions.
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying particle physics, as well as educators and researchers interested in the applications of special relativity in particle decay processes.

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Homework Statement



A (pi)0 meson whose rest mass is 135 MeV/c2 is moving with a kinetic energy of 1 GeV. It decays in flight into two photons whose paths are along the direction of motion of the meson. Find the energies of the two photons.


Homework Equations



Lab Frame:

The invariant: E^2 = P^2c^2 + m^2c^4
Conservation of Energy: E = E_1 + E_2 = hf_1 + hf_2
Conservation of Momentum: P = P_1 + P_2 = hf_1/c + hf_2/c

ZMF Frame:

The invariant: E^2 = P'^2c^2 + m^2c^4
Conservation of Energy(ZMF frame): m_0c^2 = E'_1 + E'_2 = hf'_1 + hf'_2
Conservation of Momentum(ZMF frame): P' = P'_1 + P'_2 = 0

The Attempt at a Solution



Using invariant and E = E_1 + E_2, P = P_1 + P_2 (lab frame)

We have E_1^2 + E_2^2 + 2E_1E_2 = (P_1^2 + P_2^2 + 2P_1P_2)c^2 + m_o^2c^4

Not sure what other equations I can get from conditions given. Too many unknowns?? I get the feeling this should end up with a quadratic to give the two different energies...
 
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I find it easier to treat problems of this kind by introducing gamma in the equations. Then, for a particle,

E=\gamma m_0c^2

K=(\gamma-1)m_0c^2

p=\sqrt{\gamma^2-1}m_0c

Use these in your energy and momentum conservation equations. Pay attention to the relative direction of travel of the two photons. Is the angle between the direction of the two photons zero or 180o?
 
Last edited:
Thanks a lot for the help :) I sorted it in the end by finding the energies in the ZMF after the decay and then using the doppler shift to transform them back into the lab frame.
 

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