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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

Four-Momentum Conservation
PinitialΞΌ=PfinalΞΌP^\mu_{\rm initial}=P^\mu_{\rm final}. This is four equations (energy + three momentum components), encapsulating both relativistic energy and momentum conservation simultaneously.
Invariant Mass
M2c4=PΞΌPΞΌM^2c^4=P_\mu P^\mu is invariant β€” the same in all frames. It equals the total rest energy available in the CM frame. For a single particle at rest: Mc2=Mc^2= rest mass.
Threshold Energy
The minimum lab energy for a reaction to occur. At threshold, all products are at rest in the CM frame. Using s=(p1+p2)ΞΌ(p1+p2)ΞΌ=(βˆ‘mf)2c4s=(p_1+p_2)^\mu(p_1+p_2)_\mu=(\sum m_f)^2c^4.
Two-Body Decay
Parent of mass MM at rest decays to m1+m2m_1+m_2. Conservation gives E1=(M2+m12βˆ’m22)c4/(2Mc2)E_1=(M^2+m_1^2-m_2^2)c^4/(2Mc^2) and the momentum ∣pβƒ—1∣=∣pβƒ—2∣|\vec p_1|=|\vec p_2|.

Key Equations

Invariant mass squared
S=PΞΌPΞΌ=Ecm2/c2S = P_\mu P^\mu = E_{\rm cm}^2/c^2
The Mandelstam variable s; equals square of CM energy.
Threshold condition
sth=βˆ‘fmfc2\sqrt{s_{\rm th}} = \sum_f m_f c^2
At threshold, all final-state particles are at rest in the CM frame.
Two-body decay energy
E1=(M2+m12βˆ’m22)c42Mc2E_1 = \frac{(M^2 + m_1^2 - m_2^2)c^4}{2Mc^2}
Energy of decay product 1 in the rest frame of parent M.
Worked Example

Pion Decay

Problem

A neutral pion (mΟ€=135m_\pi=135 MeV/cΒ²) at rest decays into two photons. Find each photon's energy.

Solution

By symmetry, both photons have equal energy (momentum conservation gives equal and opposite momenta).

EΞ³=mΟ€c22=1352=67.5Β MeVE_\gamma = \frac{m_\pi c^2}{2} = \frac{135}{2} = 67.5\text{ MeV}

Check: total energy =2Γ—67.5=135=2\times67.5=135 MeV = rest energy βœ“. Total momentum = 0 βœ“.

Answer Each photon has EΞ³=67.5E_\gamma=67.5 MeV.
Practice

Exercises

7 problems
1 of 7

A pion (mΟ€c2=135m_\pi c^2=135 MeV) at rest decays into two photons. Find the energy of each photon (in MeV).

MeV
2 of 7

A kaon (Mc2=494Mc^2=494 MeV) at rest decays into Ο€+\pi^+ (m1c2=140m_1c^2=140 MeV) and Ο€βˆ’\pi^- (m2c2=140m_2c^2=140 MeV). Find the momentum of each pion (in MeV/c). Use pc=E12βˆ’(m1c2)2pc=\sqrt{E_1^2-(m_1c^2)^2}, E1=Mc2/2=247E_1=Mc^2/2=247 MeV.

MeV/c
3 of 7

Two protons (mpc2=938m_pc^2=938 MeV) collide head-on, each with energy E=5000E=5000 MeV. Find the CM energy s=2E\sqrt{s}=2E (in GeV).

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4 of 7

In a fixed-target experiment, a proton (mpc2=938m_pc^2=938 MeV) beam hits a proton at rest. The invariant s=2mpc2(Ebeam+mpc2)s=2m_pc^2(E_\text{beam}+m_pc^2). Find the CM energy s\sqrt{s} (in GeV) for Ebeam=100E_{\rm beam}=100 GeV. (mpc2β‰ˆ1m_pc^2\approx1 GeV.)

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5 of 7

Perfectly inelastic relativistic collision: particle (m1c2=1m_1c^2=1 GeV, p1c=3p_1c=3 GeV) hits stationary particle (m2c2=1m_2c^2=1 GeV). Find the mass MM of the composite (in GeV/cΒ²). M2c4=(E1+E2)2βˆ’βˆ£p1c∣2M^2c^4=(E_1+E_2)^2-|p_1c|^2. E1=9+1=10E_1=\sqrt{9+1}=\sqrt{10} GeV.

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6 of 7

Compton scattering: photon (E0=1.00E_0=1.00 MeV) scatters at ΞΈ=90Β°\theta=90Β° from an electron at rest (mec2=0.511m_ec^2=0.511 MeV). Find scattered photon energy EfE_f (in MeV). Ef=E0/(1+E0/(mec2))E_f=E_0/(1+E_0/(m_ec^2)).

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7 of 7

An electron (mec2=0.511m_ec^2=0.511 MeV) and positron each with kinetic energy K=1.0K=1.0 MeV annihilate. Find the total energy (in MeV) available for the two photons produced.

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Key Takeaways

  • Four-momentum conservation PbeforeΞΌ=PafterΞΌP^\mu_{\rm before}=P^\mu_{\rm after} combines energy and momentum into one covariant law.
  • Invariant mass Mc2=PΞΌPΞΌMc^2=\sqrt{P_\mu P^\mu} 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.