Relativistic Collisions & Decays
In relativistic mechanics, both energy and momentum are conserved in collisions and decays β encapsulated in conservation of four-momentum $P^\mu_{\rm total}=$ const. The invariant mass $M^2c^4=P_\mu P^\mu$ is the key tool for finding threshold energies and understanding what products are kinematically allowed.
Key Concepts
Key Equations
Pion Decay
A neutral pion ( MeV/cΒ²) at rest decays into two photons. Find each photon's energy.
By symmetry, both photons have equal energy (momentum conservation gives equal and opposite momenta).
Check: total energy MeV = rest energy β. Total momentum = 0 β.
Exercises
7 problemsA pion ( MeV) at rest decays into two photons. Find the energy of each photon (in MeV).
A kaon ( MeV) at rest decays into ( MeV) and ( MeV). Find the momentum of each pion (in MeV/c). Use , MeV.
Two protons ( MeV) collide head-on, each with energy MeV. Find the CM energy (in GeV).
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Upgrade to Pro βIn a fixed-target experiment, a proton ( MeV) beam hits a proton at rest. The invariant . Find the CM energy (in GeV) for GeV. ( GeV.)
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Upgrade to Pro βPerfectly inelastic relativistic collision: particle ( GeV, GeV) hits stationary particle ( GeV). Find the mass of the composite (in GeV/cΒ²). . GeV.
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Upgrade to Pro βCompton scattering: photon ( MeV) scatters at from an electron at rest ( MeV). Find scattered photon energy (in MeV). .
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Upgrade to Pro βAn electron ( MeV) and positron each with kinetic energy MeV annihilate. Find the total energy (in MeV) available for the two photons produced.
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Upgrade to Pro βKey Takeaways
- Four-momentum conservation combines energy and momentum into one covariant law.
- Invariant mass is the CM-frame total energy; it's frame-independent.
- Threshold energies: at threshold all products are at rest in the CM frame, minimizing the required energy.
- Fixed-target vs. collider: a 100 GeV fixed-target beam gives only ~14 GeV of CM energy; a 50 GeV collider gives 100 GeV.