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Annihilation

In particle physics, annihilation is the process that occurs when a subatomic particle collides with its respective antiparticle to produce other particles, such as an electron colliding with a positron to produce two photons.[1] The total energy and momentum of the initial pair are conserved in the process and distributed among a set of other particles in the final state. Antiparticles have exactly opposite additive quantum numbers from particles, so the sums of all quantum numbers of such an original pair are zero. Hence, any set of particles may be produced whose total quantum numbers are also zero as long as conservation of energy, conservation of momentum, and conservation of spin are obeyed.[2]

This article is about the physical process of particle–antiparticle annihilation. For other uses, see Annihilation (disambiguation).

During a low-energy annihilation, photon production is favored, since these particles have no mass. High-energy particle colliders produce annihilations where a wide variety of exotic heavy particles are created.


The word "annihilation" takes use informally for the interaction of two particles that are not mutual antiparticles – not charge conjugate. Some quantum numbers may then not sum to zero in the initial state, but conserve with the same totals in the final state. An example is the "annihilation" of a high-energy electron antineutrino with an electron to produce a W boson.


If the annihilating particles are composite, such as mesons or baryons, then several different particles are typically produced in the final state.


The inverse of annihilation is pair production, the process in which a high-energy photon converts its energy into mass.

Production of a single boson[edit]

If the initial two particles are elementary (not composite), then they may combine to produce only a single elementary boson, such as a photon (
γ
), gluon (
g
),
Z
, or a Higgs boson (
H0
). If the total energy in the center-of-momentum frame is equal to the rest mass of a real boson (which is impossible for a massless boson such as the
γ
), then that created particle will continue to exist until it decays according to its lifetime. Otherwise, the process is understood as the initial creation of a boson that is virtual, which immediately converts into a real particle + antiparticle pair. This is called an s-channel process. An example is the annihilation of an electron with a positron to produce a virtual photon, which converts into a muon and anti-muon. If the energy is large enough, a
Z
could replace the photon.

Pair production

Creation and annihilation operators

Photon energy

Kragh, H. (1999). . Princeton University Press. ISBN 0-691-01206-7.

Quantum Generations : A history of physics in the twentieth century