This article is about the physical process of particle–antiparticle annihilation. For other uses, see Annihilation (disambiguation).
A Feynman diagram showing the mutual annihilation of a bound state electron positron pair into two photons. This bound state is more commonly known as positronium.
Antimatter
Antiparticles
Positron
Antiproton
Antineutron
Antihydrogen
Antihelium
Onia
Antiprotonic hydrogen
Antiprotonic helium
Muonium
True muonium
Pionium
Positronium
Quarkonium
Concepts and phenomena
Annihilation
Baryogenesis
Baryon asymmetry
Comet
CP violation
Gravitational interaction
Positron emission
Devices
Cloud chamber
Particle accelerator
Antiproton decelerator
Relativistic Heavy Ion Collider
Penning trap
Uses
Positron emission tomography
Fuel
Weapon
People and bodies
Carl David Anderson
Paul Dirac
Andrei Sakharov
CERN
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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]
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.
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"Antimatter". Lawrence Berkeley National Laboratory. Archived from the original on 23 August 2008. Retrieved 3 September 2008.
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"The Standard Model – Particle decays and annihilations". The Particle Adventure: The Fundamentals of Matter and Force. Lawrence Berkeley National Laboratory. Retrieved 17 October 2011.
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