Difference between revisions of "Boson" - New World Encyclopedia
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In [[particle physics]], '''bosons''' are [[subatomic particle|particles]] that obey [[Bose-Einstein statistics]] and are named after [[Satyendra Nath Bose]] and [[Albert Einstein]]. In contrast to [[fermion]]s, which obey [[Fermi-Dirac statistics]], several bosons can occupy the same [[quantum state]]. Thus, bosons with the same energy can occupy the same place in space. Therefore, bosons are often considered as [[force carrier]] particles, whereas fermions are usually associated with [[matter]], although the distinction between the two concepts is not clear cut in [[quantum physics]]. | In [[particle physics]], '''bosons''' are [[subatomic particle|particles]] that obey [[Bose-Einstein statistics]] and are named after [[Satyendra Nath Bose]] and [[Albert Einstein]]. In contrast to [[fermion]]s, which obey [[Fermi-Dirac statistics]], several bosons can occupy the same [[quantum state]]. Thus, bosons with the same energy can occupy the same place in space. Therefore, bosons are often considered as [[force carrier]] particles, whereas fermions are usually associated with [[matter]], although the distinction between the two concepts is not clear cut in [[quantum physics]]. | ||
Bosons may be either [[Elementary particle|elementary]], like the [[photon]], or [[Composite particle|composite]], like [[meson]]s. All observed bosons have [[integer]] [[Spin (physics)|spin]], as opposed to fermions, which have [[half-integer]] spin. This is in accordance with the [[spin-statistics theorem]] which states that in any reasonable [[relativistic]] [[quantum field theory]], particles with integer spin are bosons, while particles with half-integer spin are fermions. | Bosons may be either [[Elementary particle|elementary]], like the [[photon]], or [[Composite particle|composite]], like [[meson]]s. All observed bosons have [[integer]] [[Spin (physics)|spin]], as opposed to fermions, which have [[half-integer]] spin. This is in accordance with the [[spin-statistics theorem]] which states that in any reasonable [[relativistic]] [[quantum field theory]], particles with integer spin are bosons, while particles with half-integer spin are fermions. | ||
| − | + | {{toc}} | |
Most bosons are [[composite particle]]s, but in the [[Standard Model]], there are five bosons that are elementary: | Most bosons are [[composite particle]]s, but in the [[Standard Model]], there are five bosons that are elementary: | ||
| − | * | + | * The [[gauge boson]]s ({{SubatomicParticle|link=yes|Photon}} · {{SubatomicParticle|link=yes|Gluon}} · {{SubatomicParticle|link=yes|W boson+-}} · {{SubatomicParticle|link=yes|Z boson}}); |
| − | * | + | * The [[Higgs boson]] ({{SubatomicParticle|link=yes|Higgs Boson}}). |
| − | Composite bosons are important in | + | Composite bosons are important in [[superfluidity]] and other applications of [[Bose-Einstein condensate]]s. |
==Definition and basic properties== | ==Definition and basic properties== | ||
| + | The name ''boson'' was coined by [[Paul Dirac]]<ref>Graham Farmelo, ''The Strangest Man: The Hidden Life of Paul Dirac, Mystic of the Atom'' (Basic Books, 2011, ISBN 978-0465022106).</ref> to commemorate the contribution of [[Satyendra Nath Bose]], an [[India]]n physicist and professor of physics at the [[University of Calcutta]] and at the [[University of Dhaka]], who developed, in conjunction with [[Albert Einstein]], the theory characterizing such particles, now known as [[Bose–Einstein statistics]].<ref>Hartosh Singh Bal, [https://archive.nytimes.com/latitude.blogs.nytimes.com/2012/09/19/indians-clamor-for-credit-for-the-bose-in-boson/ The Bose in the Boson] ''The New York Times'', September 19, 2012. Retrieved September 17, 2022. </ref> | ||
| − | By definition, bosons are particles which obey [[Bose-Einstein statistics]]: | + | By definition, bosons are particles which obey [[Bose-Einstein statistics]]: When one swaps two bosons, the [[wavefunction]] of the system is unchanged.<ref>Mark Allen Srednicki, ''Quantum Field Theory'' (Cambridge: Cambridge University Press, 2007, ISBN 978-0521864497), 28-29.</ref> Fermions, on the other hand, obey [[Fermi-Dirac statistics]] and the [[Pauli exclusion principle]]: Two fermions cannot occupy the same [[quantum state]] as each other, resulting in a "rigidity" or "stiffness" of matter which includes fermions. Thus fermions are sometimes said to be the constituents of [[matter]], while bosons are said to be the particles that transmit interactions ([[force carrier]]s), or the constituents of [[radiation]]. The [[quantum field]]s of bosons are [[bosonic field]]s, obeying [[canonical commutation relation]]s. |
| − | The properties of [[lasers]] and [[masers]], [[superfluid]] [[helium|helium-4]] and [[Bose–Einstein condensate]]s are all consequences of statistics of bosons. | + | The properties of [[lasers]] and [[masers]], [[superfluid]] [[helium|helium-4]] and [[Bose–Einstein condensate]]s are all consequences of statistics of bosons. Another result is that the spectrum of a photon gas in thermal equilibrium is a [[Planck spectrum]], one example of which is [[black-body]] radiation; another is the thermal radiation of the opaque early Universe seen today as [[microwave background radiation]]. |
Interaction of [[virtual particle|virtual]] bosons with real fermions are called [[fundamental interaction]]s, and these result in all [[force]]s we know. The bosons involved in these interactions are called [[gauge bosons]]. | Interaction of [[virtual particle|virtual]] bosons with real fermions are called [[fundamental interaction]]s, and these result in all [[force]]s we know. The bosons involved in these interactions are called [[gauge bosons]]. | ||
| − | All known elementary and composite particles are bosons or fermions, depending on their [[spin (physics)|spin]]: particles with [[half-integer]] spin are [[fermions]]; particles with [[integer]] spin are bosons. In the framework of nonrelativistic [[quantum mechanic]]s, this is a purely empirical observation. However, in [[relativistic]] [[quantum field theory]], the [[spin-statistics theorem]] shows that half-integer spin particles cannot be bosons and integer spin particles cannot be fermions.<ref>Sakurai (1994), | + | All known elementary and composite particles are bosons or fermions, depending on their [[spin (physics)|spin]]: particles with [[half-integer]] spin are [[fermions]]; particles with [[integer]] spin are bosons. In the framework of nonrelativistic [[quantum mechanic]]s, this is a purely empirical observation. However, in [[relativistic]] [[quantum field theory]], the [[spin-statistics theorem]] shows that half-integer spin particles cannot be bosons and integer spin particles cannot be fermions.<ref>J. J. Sakurai and San Fu Tuan, ''Modern Quantum Mechanics'' (Reading, MA: Addison-Wesley, 1994, ISBN 0201539292), 362.</ref> |
| − | In large systems, the difference between bosonic and fermionic statistics is only apparent at large densities—when their wave functions overlap. | + | In large systems, the difference between bosonic and fermionic statistics is only apparent at large densities—when their wave functions overlap. At low densities, both types of statistics are well approximated by [[Maxwell-Boltzmann statistics]], which is described by [[classical mechanics]]. |
==Elementary bosons== | ==Elementary bosons== | ||
| − | + | All observed [[elementary particle]]s are either f[[ermion]]s or bosons. The observed elementary bosons are all [[gauge boson]]s: [[Photon]]s, [[W and Z bosons]], and [[gluon]]s. | |
| + | * Photons are the [[force carrier]]s of the [[electromagnetic field]] | ||
| + | * W and Z bosons are the force carriers which mediate the [[weak nuclear force]] | ||
| + | * Gluons are the fundamental force carriers underlying the [[strong nuclear force]] | ||
| − | + | In addition, the [[Standard Model]] postulates the existence of [[Higgs boson]]s, which give other particles their mass via the [[Higgs mechanism]]. In particular, the Higgs boson explains why the photon has no mass, while the [[W and Z bosons]] are very heavy. Elementary particle masses, and the differences between [[electromagnetism]] (mediated by the photon) and the [[weak force]] (mediated by the W and Z bosons), are critical to many aspects of the structure of microscopic (and hence macroscopic) matter. In [[electroweak interaction|electroweak theory]], the Higgs boson generates the masses of the leptons (electron, muon, and tau) and quarks. As the Higgs boson is massive, it must interact with itself. | |
| − | |||
| − | |||
| − | |||
| − | + | On July 4, 2012 the two main experiments at the LHC ([[ATLAS experiment|ATLAS]] and [[Compact Muon Solenoid|CMS]]) both reported independently that they found a new particle with a mass of about 125 and 127 GeV/c2 (about 133 proton masses, on the order of 10<sup>−25</sup> kg), which is "consistent with the Higgs boson."<ref>Matt Strassler, [https://profmattstrassler.com/articles-and-posts/the-higgs-particle/the-discovery-of-the-higgs/higgs-discovery-is-it-a-higgs/ Higgs Discovery: Is it a Higgs?] July 10, 2012. Retrieved September 14, 2022.</ref> On March 14, 2013 the Higgs Boson was tentatively confirmed to exist,<ref> [https://home.web.cern.ch/news/news/physics/new-results-indicate-new-particle-higgs-boson New results indicate that new particle is a Higgs boson] CERN, March 14, 2013. Retrieved September 14, 2022.</ref> with subsequent experiments confirming the finding. In the mainstream media, the Higgs boson has been called the "God particle" after the 1993 book ''[[The God Particle (book)|The God Particle]]'' by [[Nobel Laureate]] [[Leon Lederman]].<ref>Leon Lederman, ''The God Particle: If the Universe Is the Answer, What Is the Question?'' (Delta, 1994, ISBN 978-0385312110).</ref> | |
| − | Finally, many views about quantum gravity postulate a force carrier for gravity, the [[graviton]], which is a boson of spin 2. | + | Finally, many views about quantum gravity postulate a force carrier for [[gravity]], the [[graviton]], which is a boson of spin 2. |
==Composite bosons== | ==Composite bosons== | ||
| − | |||
[[Composite particle]]s (such as [[hadron]]s, [[atomic nucleus|nuclei]], and [[atom]]s) can be bosons or fermions depending on their constituents. More precisely, because of the relation between spin and statistics, a particle containing an even number of fermions is a boson, since it has [[integer]] spin. | [[Composite particle]]s (such as [[hadron]]s, [[atomic nucleus|nuclei]], and [[atom]]s) can be bosons or fermions depending on their constituents. More precisely, because of the relation between spin and statistics, a particle containing an even number of fermions is a boson, since it has [[integer]] spin. | ||
Examples include the following: | Examples include the following: | ||
| − | *A [[meson]] contains two fermionic [[quark]]s and is therefore a boson | + | *A [[meson]] contains two fermionic [[quark]]s and is therefore a boson |
| − | *The [[atomic nucleus|nucleus]] of a [[carbon-12]] atom contains 6 protons and 6 neutrons (all fermions) and is therefore a boson | + | *The [[atomic nucleus|nucleus]] of a [[carbon-12]] atom contains 6 protons and 6 neutrons (all fermions) and is therefore a boson |
| − | *The atom [[helium-4]] (<sup>4</sup>He) is made of 2 protons, 2 neutrons and 2 electrons and is therefore a boson | + | *The atom [[helium-4]] (<sup>4</sup>He) is made of 2 protons, 2 neutrons and 2 electrons and is therefore a boson |
The number of bosons within a composite particle made up of simple particles bound with a potential has no effect on whether it is a boson or a fermion. | The number of bosons within a composite particle made up of simple particles bound with a potential has no effect on whether it is a boson or a fermion. | ||
| − | Fermionic or bosonic behavior of a composite particle (or system) is only seen at large (compared to size of the system) distance. At proximity, where spatial structure begins to be important, a composite particle (or system) behaves according to its constituent makeup. For example, two atoms of [[helium-4]] cannot share the same space if it is comparable by size to the size of the inner structure of the helium atom itself (~10<sup>−10</sup> m)—despite bosonic properties of the | + | Fermionic or bosonic behavior of a composite particle (or system) is only seen at large (compared to size of the system) distance. At proximity, where spatial structure begins to be important, a composite particle (or system) behaves according to its constituent makeup. For example, two atoms of [[helium-4]] cannot share the same space if it is comparable by size to the size of the inner structure of the helium atom itself (~10<sup>−10</sup> m)—despite bosonic properties of the helium-4 atoms. Thus, liquid helium has finite density comparable to the density of ordinary [[liquid]] matter. |
== See also == | == See also == | ||
| − | |||
* [[Elementary particle]] | * [[Elementary particle]] | ||
* [[Fermion]] | * [[Fermion]] | ||
| Line 56: | Line 56: | ||
* [[Photon]] | * [[Photon]] | ||
* [[Quark]] | * [[Quark]] | ||
| − | |||
== Notes == | == Notes == | ||
| Line 62: | Line 61: | ||
== References == | == References == | ||
| − | + | * Farmelo, Graham. ''The Strangest Man: The Hidden Life of Paul Dirac, Mystic of the Atom''. Basic Books, 2011. ISBN 978-0465022106 | |
| − | * Greene, Brian | + | * Greene, Brian. ''The Elegant Universe: Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory.'' New York: Norton, 2003. ISBN 0393058581 |
| − | + | * Gribbin, John R. ''Q Is for Quantum: An Encyclopedia of Particle Physics.'' New York: Touchstone, 2000. ISBN 0684863154 | |
| − | * Gribbin, John R | + | * Lederman, Leon. ''The God Particle: If the Universe Is the Answer, What Is the Question?'' Delta, 1994. ISBN 978-0385312110 |
| − | + | * Sakurai, J. J., and San Fu Tuan. ''Modern Quantum Mechanics.'' Reading, MA: Addison-Wesley, 1994. ISBN 0201539292 | |
| − | * Sakurai, J. J., and San Fu Tuan | + | * Schumm, Bruce A. ''Deep Down Things: The Breathtaking Beauty of Particle Physics.'' Baltimore, MD: Johns Hopkins University Press, 2004. ISBN 080187971X |
| − | + | * Seiden, Abraham. ''Particle Physics: A Comprehensive Introduction.'' San Francisco: Addison Wesley, 2005. ISBN 978-0805387360 | |
| − | * Schumm, Bruce A | + | * Srednicki, Mark Allen. ''Quantum Field Theory.'' Cambridge: Cambridge University Press, 2007. ISBN 978-0521864497 |
| − | |||
| − | * Seiden, | ||
| − | |||
| − | * Srednicki, Mark Allen | ||
---- | ---- | ||
Latest revision as of 17:22, 22 December 2022
In particle physics, bosons are particles that obey Bose-Einstein statistics and are named after Satyendra Nath Bose and Albert Einstein. In contrast to fermions, which obey Fermi-Dirac statistics, several bosons can occupy the same quantum state. Thus, bosons with the same energy can occupy the same place in space. Therefore, bosons are often considered as force carrier particles, whereas fermions are usually associated with matter, although the distinction between the two concepts is not clear cut in quantum physics.
Bosons may be either elementary, like the photon, or composite, like mesons. All observed bosons have integer spin, as opposed to fermions, which have half-integer spin. This is in accordance with the spin-statistics theorem which states that in any reasonable relativistic quantum field theory, particles with integer spin are bosons, while particles with half-integer spin are fermions.
Most bosons are composite particles, but in the Standard Model, there are five bosons that are elementary:
Composite bosons are important in superfluidity and other applications of Bose-Einstein condensates.
Definition and basic properties
The name boson was coined by Paul Dirac[1] to commemorate the contribution of Satyendra Nath Bose, an Indian physicist and professor of physics at the University of Calcutta and at the University of Dhaka, who developed, in conjunction with Albert Einstein, the theory characterizing such particles, now known as Bose–Einstein statistics.[2]
By definition, bosons are particles which obey Bose-Einstein statistics: When one swaps two bosons, the wavefunction of the system is unchanged.[3] Fermions, on the other hand, obey Fermi-Dirac statistics and the Pauli exclusion principle: Two fermions cannot occupy the same quantum state as each other, resulting in a "rigidity" or "stiffness" of matter which includes fermions. Thus fermions are sometimes said to be the constituents of matter, while bosons are said to be the particles that transmit interactions (force carriers), or the constituents of radiation. The quantum fields of bosons are bosonic fields, obeying canonical commutation relations.
The properties of lasers and masers, superfluid helium-4 and Bose–Einstein condensates are all consequences of statistics of bosons. Another result is that the spectrum of a photon gas in thermal equilibrium is a Planck spectrum, one example of which is black-body radiation; another is the thermal radiation of the opaque early Universe seen today as microwave background radiation. Interaction of virtual bosons with real fermions are called fundamental interactions, and these result in all forces we know. The bosons involved in these interactions are called gauge bosons.
All known elementary and composite particles are bosons or fermions, depending on their spin: particles with half-integer spin are fermions; particles with integer spin are bosons. In the framework of nonrelativistic quantum mechanics, this is a purely empirical observation. However, in relativistic quantum field theory, the spin-statistics theorem shows that half-integer spin particles cannot be bosons and integer spin particles cannot be fermions.[4]
In large systems, the difference between bosonic and fermionic statistics is only apparent at large densities—when their wave functions overlap. At low densities, both types of statistics are well approximated by Maxwell-Boltzmann statistics, which is described by classical mechanics.
Elementary bosons
All observed elementary particles are either fermions or bosons. The observed elementary bosons are all gauge bosons: Photons, W and Z bosons, and gluons.
- Photons are the force carriers of the electromagnetic field
- W and Z bosons are the force carriers which mediate the weak nuclear force
- Gluons are the fundamental force carriers underlying the strong nuclear force
In addition, the Standard Model postulates the existence of Higgs bosons, which give other particles their mass via the Higgs mechanism. In particular, the Higgs boson explains why the photon has no mass, while the W and Z bosons are very heavy. Elementary particle masses, and the differences between electromagnetism (mediated by the photon) and the weak force (mediated by the W and Z bosons), are critical to many aspects of the structure of microscopic (and hence macroscopic) matter. In electroweak theory, the Higgs boson generates the masses of the leptons (electron, muon, and tau) and quarks. As the Higgs boson is massive, it must interact with itself.
On July 4, 2012 the two main experiments at the LHC (ATLAS and CMS) both reported independently that they found a new particle with a mass of about 125 and 127 GeV/c2 (about 133 proton masses, on the order of 10−25 kg), which is "consistent with the Higgs boson."[5] On March 14, 2013 the Higgs Boson was tentatively confirmed to exist,[6] with subsequent experiments confirming the finding. In the mainstream media, the Higgs boson has been called the "God particle" after the 1993 book The God Particle by Nobel Laureate Leon Lederman.[7]
Finally, many views about quantum gravity postulate a force carrier for gravity, the graviton, which is a boson of spin 2.
Composite bosons
Composite particles (such as hadrons, nuclei, and atoms) can be bosons or fermions depending on their constituents. More precisely, because of the relation between spin and statistics, a particle containing an even number of fermions is a boson, since it has integer spin.
Examples include the following:
- A meson contains two fermionic quarks and is therefore a boson
- The nucleus of a carbon-12 atom contains 6 protons and 6 neutrons (all fermions) and is therefore a boson
- The atom helium-4 (4He) is made of 2 protons, 2 neutrons and 2 electrons and is therefore a boson
The number of bosons within a composite particle made up of simple particles bound with a potential has no effect on whether it is a boson or a fermion.
Fermionic or bosonic behavior of a composite particle (or system) is only seen at large (compared to size of the system) distance. At proximity, where spatial structure begins to be important, a composite particle (or system) behaves according to its constituent makeup. For example, two atoms of helium-4 cannot share the same space if it is comparable by size to the size of the inner structure of the helium atom itself (~10−10 m)—despite bosonic properties of the helium-4 atoms. Thus, liquid helium has finite density comparable to the density of ordinary liquid matter.
See also
Notes
- ↑ Graham Farmelo, The Strangest Man: The Hidden Life of Paul Dirac, Mystic of the Atom (Basic Books, 2011, ISBN 978-0465022106).
- ↑ Hartosh Singh Bal, The Bose in the Boson The New York Times, September 19, 2012. Retrieved September 17, 2022.
- ↑ Mark Allen Srednicki, Quantum Field Theory (Cambridge: Cambridge University Press, 2007, ISBN 978-0521864497), 28-29.
- ↑ J. J. Sakurai and San Fu Tuan, Modern Quantum Mechanics (Reading, MA: Addison-Wesley, 1994, ISBN 0201539292), 362.
- ↑ Matt Strassler, Higgs Discovery: Is it a Higgs? July 10, 2012. Retrieved September 14, 2022.
- ↑ New results indicate that new particle is a Higgs boson CERN, March 14, 2013. Retrieved September 14, 2022.
- ↑ Leon Lederman, The God Particle: If the Universe Is the Answer, What Is the Question? (Delta, 1994, ISBN 978-0385312110).
ReferencesISBN links support NWE through referral fees
- Farmelo, Graham. The Strangest Man: The Hidden Life of Paul Dirac, Mystic of the Atom. Basic Books, 2011. ISBN 978-0465022106
- Greene, Brian. The Elegant Universe: Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory. New York: Norton, 2003. ISBN 0393058581
- Gribbin, John R. Q Is for Quantum: An Encyclopedia of Particle Physics. New York: Touchstone, 2000. ISBN 0684863154
- Lederman, Leon. The God Particle: If the Universe Is the Answer, What Is the Question? Delta, 1994. ISBN 978-0385312110
- Sakurai, J. J., and San Fu Tuan. Modern Quantum Mechanics. Reading, MA: Addison-Wesley, 1994. ISBN 0201539292
- Schumm, Bruce A. Deep Down Things: The Breathtaking Beauty of Particle Physics. Baltimore, MD: Johns Hopkins University Press, 2004. ISBN 080187971X
- Seiden, Abraham. Particle Physics: A Comprehensive Introduction. San Francisco: Addison Wesley, 2005. ISBN 978-0805387360
- Srednicki, Mark Allen. Quantum Field Theory. Cambridge: Cambridge University Press, 2007. ISBN 978-0521864497
| 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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