Difference between revisions of "Antiproton" - New World Encyclopedia
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| − | + | == Properties == | |
| − | In mid-June 2006, scientists at CERN succeeded in determining the mass of the antiproton, which they measured at {{val|1836.153674|(5)}} times more massive than an [[electron]]. This is exactly the same as the mass of a "regular" proton, | + | The properties of the antiproton are predicted by [[CPT symmetry]] to be exactly related to those of the proton. In particular, CPT symmetry predicts the mass and lifetime of the antiproton to be the same as those of the proton, and the electric charge and magnetic moment of the antiproton to be opposite in sign and equal in magnitude to those of the proton. (CPT symmetry is a basic consequence of [[quantum field theory]] and no violations of it have ever been detected.) |
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| + | In mid-June 2006, scientists at [[CERN]] (the European Organization for Nuclear Research, or, in French, ''Organisation Européenne pour la Recherche Nucléaire'') succeeded in determining the mass of the antiproton, which they measured at {{val|1836.153674|(5)}} times more massive than an [[electron]]. This is exactly the same as the mass of a "regular" proton, as predicted. The formation of antimatter is related to questions about what happened around the time of the [[Big Bang]], and why such a small amount of antimatter remains in our Solar System today. | ||
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| + | == Artificial production == | ||
| + | |||
| + | The formation of antiprotons requires energy equivalent to a temperature of 10 trillion [[Kelvin|K]] (10<sup>13</sup> K), which is not attained under most natural conditions. However, at [[CERN]] (the European Organization for Nuclear Research, or, in French, ''Organisation Européenne pour la Recherche Nucléaire''), protons are accelerated in the Proton [[Synchrotron]] (PS) to an energy of 26 [[giga|G]][[electron volt|eV]], and then smashed into an [[iridium]] rod. The protons bounce off the iridium nuclei with [[mass-energy equivalence|enough energy for matter to be created]]. A range of particles and antiparticles are formed, and the antiprotons are separated off using magnets in [[vacuum]]. | ||
==Occurrence in nature== | ==Occurrence in nature== | ||
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* [[Antihydrogen]] [[Penning trap]] of Gabrielse et al: {{val|0.28|u=year}} <ref>Caso, C., et al. (Particle Data Group). 1998. [http://pdg.ihep.su/1999/s041.pdf B<sup>±</sup>]. ''Eur. Phys. J.'' C3:613. Retrieved October 9, 2008.</ref> | * [[Antihydrogen]] [[Penning trap]] of Gabrielse et al: {{val|0.28|u=year}} <ref>Caso, C., et al. (Particle Data Group). 1998. [http://pdg.ihep.su/1999/s041.pdf B<sup>±</sup>]. ''Eur. Phys. J.'' C3:613. Retrieved October 9, 2008.</ref> | ||
* APEX collaboration at [[Fermilab]]: {{val|50000|u=years}} for {{SubatomicParticle|Antiproton}} → {{SubatomicParticle|link=yes|Muon}} + X<!-- What is "X"?? —> and {{val|300000|u=years}} for {{SubatomicParticle|Antiproton}} → {{SubatomicParticle|link=yes|Electron}} + {{SubatomicParticle|link=yes|Gamma}} | * APEX collaboration at [[Fermilab]]: {{val|50000|u=years}} for {{SubatomicParticle|Antiproton}} → {{SubatomicParticle|link=yes|Muon}} + X<!-- What is "X"?? —> and {{val|300000|u=years}} for {{SubatomicParticle|Antiproton}} → {{SubatomicParticle|link=yes|Electron}} + {{SubatomicParticle|link=yes|Gamma}} | ||
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==Recent antiproton cosmic ray detection experiments== | ==Recent antiproton cosmic ray detection experiments== | ||
Revision as of 20:42, 9 October 2008
The antiproton (p, pronounced p-bar) is the antiparticle of the proton. Antiprotons are stable, but they are typically short-lived since any collision with a proton will cause both particles to be annihilated in a burst of energy. It was discovered in 1955 by University of California, Berkeley physicists Emilio Segrè and Owen Chamberlain, for which they were awarded the 1959 Nobel Prize in Physics. An antiproton consists of two anti-up quarks and one anti-down quark (uud).
| Antimatter | |
| Overview | |
| Annihilation | |
Devices
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Antiparticles
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Uses
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Scientific Bodies
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People
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| AntiProton | |
 The quark structure of the proton. | |
| Classification: | Baryon |
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Properties
The properties of the antiproton are predicted by CPT symmetry to be exactly related to those of the proton. In particular, CPT symmetry predicts the mass and lifetime of the antiproton to be the same as those of the proton, and the electric charge and magnetic moment of the antiproton to be opposite in sign and equal in magnitude to those of the proton. (CPT symmetry is a basic consequence of quantum field theory and no violations of it have ever been detected.)
In mid-June 2006, scientists at CERN (the European Organization for Nuclear Research, or, in French, Organisation Européenne pour la Recherche Nucléaire) succeeded in determining the mass of the antiproton, which they measured at 1,836.153674(5) times more massive than an electron. This is exactly the same as the mass of a "regular" proton, as predicted. The formation of antimatter is related to questions about what happened around the time of the Big Bang, and why such a small amount of antimatter remains in our Solar System today.
Artificial production
The formation of antiprotons requires energy equivalent to a temperature of 10 trillion K (1013 K), which is not attained under most natural conditions. However, at CERN (the European Organization for Nuclear Research, or, in French, Organisation Européenne pour la Recherche Nucléaire), protons are accelerated in the Proton Synchrotron (PS) to an energy of 26 GeV, and then smashed into an iridium rod. The protons bounce off the iridium nuclei with enough energy for matter to be created. A range of particles and antiparticles are formed, and the antiprotons are separated off using magnets in vacuum.
Occurrence in nature
Antiprotons have been detected in cosmic rays for over 25 years, first by balloon-borne experiments and more recently by satellite-based detectors. The standard picture for their presence in cosmic rays is that they are produced in collisions of cosmic ray protons with nuclei in the interstellar medium, via the reaction:
p A → p p p A
The secondary antiprotons (p) then propagate through the galaxy, confined by the galactic magnetic fields. Their energy spectrum is modified by collisions with other atoms in the interstellar medium, and antiprotons can also be lost by "leaking out" of the galaxy.
The antiproton cosmic ray energy spectrum is now measured reliably and is consistent with this standard picture of antiproton production by cosmic ray collisions.[1] This sets upper limits on the number of antiprotons that could be produced in exotic ways, such as from annihilation of supersymmetric dark matter particles in the galaxy, or from the evaporation of primordial black holes. This also provides a lower limit on the antiproton lifetime of about 1-10 million years. Since the galactic storage time of antiprotons is about 10 million years, an intrinsic decay lifetime would modify the galactic residence time and distort the spectrum of cosmic ray antiprotons. This is significantly more stringent than the best laboratory measurements of the antiproton lifetime:
- LEAR collaboration at CERN: 0.8 year
- Antihydrogen Penning trap of Gabrielse et al: 0.28 year [2]
- APEX collaboration at Fermilab: 50,000 years for p → μ− + X and 300,000 years for p → e− + γ
Recent antiproton cosmic ray detection experiments
- BESS: balloon-borne experiment, flown in 1993, 1995, and 1997.
- CAPRICE: balloon-borne experiment, flown in 1994.[3]
- HEAT: balloon-borne experiment, flown in 2000.
- AMS: space-based experiment, prototype flown on the space shuttle in 1998, intended for the International Space Station but not yet launched.
- PAMELA: satellite experiment to detect cosmic rays and antimatter from space, launched June 2006.
Uses
Antiprotons are routinely produced at Fermilab for collider physics operations in the Tevatron, where they are collided with protons. The use of antiprotons allows for a higher average energy of collisions between quarks and antiquarks than would be possible in proton-proton collisions. This is because the valence quarks in the proton, and the valence antiquarks in the antiproton, tend to carry the largest fraction of the proton or antiproton's momentum.
See also
- Antimatter
- Elementary particle
- Positron
- Proton
Notes
- ↑ Kennedy, Dallas C. 2000. Cosmic Ray Antiprotons. Astrophysics. (doi=10.1117/12.253971). Retrieved October 9, 2008.
- ↑ Caso, C., et al. (Particle Data Group). 1998. B±. Eur. Phys. J. C3:613. Retrieved October 9, 2008.
- ↑ Cosmic AntiParticle Ring Imaging Cherenkov Experiment (CAPRICE). Retrieved October 9, 2008.
ReferencesISBN links support NWE through referral fees
- Forward, Robert L. 2001. Mirror Matter: Pioneering Antimatter Physics. Lincoln, NE: Backinprint.com. ISBN 0595198171.
- Fraser, Gordon. 2002. Antimatter: The Ultimate Mirror. Cambridge, UK: Cambridge University Press. ISBN 0521893097.
- Kondo, K., and S. Kim. 1994. 9th Topical Workshop on Proton-Antiproton Collider Physics. Frontier Science Series No. 11. Tokyo, Japan: Universal Academy Press. ASIN B000RFVPI4.
- Santilli, Ruggero Maria. 2006. Isodual Theory of Antimatter: with applications to Antigravity, Grand Unification and Cosmology (Fundamental Theories of Physics). New York, NY: Springer. ISBN 1402045174.
External links
- Antiproton weighs in. physicsworld.com. Retrieved October 9, 2008.
- The Golden Anniversary of the Antiproton. Science@BerkeleyLab. (Gives history of antiproton discovery.) Retrieved October 9, 2008.
- FAIR: Facility for Antiproton and Ion Research. Retrieved October 9, 2008.
- Introduction to the Antiproton Decelerator. CERN. Retrieved October 9, 2008.
| Particles in physics | |
|---|---|
| elementary particles | Elementary fermions: Quarks: u · d · s · c · b · t • Leptons: e · μ · τ · νe · νμ · ντ Elementary bosons: Gauge bosons: γ · g · W± · Z0 • Ghosts |
| Composite particles | Hadrons: Baryons(list)/Hyperons/Nucleons: p · n · Δ · Λ · Σ · Ξ · Ω · Ξb • Mesons(list)/Quarkonia: π · K · ρ · J/ψ · Υ Other: Atomic nucleus • Atoms • Molecules • Positronium |
| Hypothetical elementary particles | Superpartners: Axino · Dilatino · Chargino · Gluino · Gravitino · Higgsino · Neutralino · Sfermion · Slepton · Squark Other: Axion · Dilaton · Goldstone boson · Graviton · Higgs boson · Tachyon · X · Y · W' · Z' |
| Hypothetical composite particles | Exotic hadrons: Exotic baryons: Pentaquark • Exotic mesons: Glueball · Tetraquark Other: Mesonic molecule |
| Quasiparticles | Davydov soliton · Exciton · Magnon · Phonon · Plasmon · Polariton · Polaron |
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