Relativistic Collisions & Decays
In relativistic mechanics, both energy and momentum are conserved in collisions and decays — 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/c²) 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 ✓. Total momentum = 0 ✓.
Exercises
7 problemsWatch a π⁰ at rest decay into two back-to-back photons. By momentum conservation, both photons have equal energy. Find the energy of each photon (in MeV) when $m_\pi c^2 = 135$ MeV.
m_π c² = 135 MeV. Pion at rest, massless photons.
A K⁰ meson ($Mc^2 = 494$ MeV) at rest decays into π⁺ and π⁻ (each $m_1c^2 = 140$ MeV). Watch the animation and find the momentum of each pion (in MeV/c).
Mc² = 494 MeV (kaon), m_π c² = 140 MeV (each pion)
Two protons ( MeV) collide head-on, each with energy MeV. Find the CM energy (in GeV).
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Upgrade to Pro →In 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 →Perfectly inelastic relativistic collision: particle ( GeV, GeV) hits stationary particle ( GeV). Find the mass of the composite (in GeV/c²). . GeV.
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Upgrade to Pro →Compton scattering: photon ( MeV) scatters at from an electron at rest ( MeV). Find scattered photon energy (in MeV). .
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Upgrade to Pro →An 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 →Key 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.