Physics:Quantum Bose–Einstein statistics: Difference between revisions

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{{Short description|Quantum statistics for bosons}}
{{Short description|Quantum statistics for bosons}}
{{Quantum matter backlink|Atoms}}
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{{Quantum article nav|previous=Physics:Quantum Fermi–Dirac statistics|previous label=Fermi-Dirac statistics|next=Physics:Quantum Bose-Einstein condensate|next label=Bose-Einstein condensate}}
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[[File:Quantum_Bose_Einstein_statistics_educational_yellow.png|thumb|right|Bose-Einstein statistics allow many bosons to occupy the same quantum state.]]
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'''Bose–Einstein statistics''' describe the occupation of quantum states by identical [[Physics:Quantum boson|bosons]]. They apply to particles with integer spin, including [[Physics:Quantum photon|photons]], gluons, phonons, and many composite particles.
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'''Bose–Einstein statistics''' is a Book II topic in the Quantum Collection. '''Bose–Einstein statistics''' describe the occupation of quantum states by identical [[Physics:Quantum boson|bosons]]. They apply to particles with integer spin, including [[Physics:Quantum photon|photons]], gluons, phonons, and many composite particles.<ref>{{Cite book |last=Annett |first=James F. |title=Superconductivity, Superfluids and Condensates |location=New York |publisher=Oxford University Press |year=2004 |isbn=0-19-850755-0}}</ref> Bose-Einstein statistics allow many identical bosons to occupy the same quantum state, which makes collective quantum behavior possible. They explain blackbody radiation, photon bunching, superfluidity, and Bose-Einstein condensation. The statistics arise from symmetric many-particle wavefunctions and contrast sharply with the exclusion behavior of fermions.
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[[File:Quantum_Bose_Einstein_statistics_educational_yellow.png|thumb|280px|Bose-Einstein statistics allow many bosons to occupy the same quantum state.]]
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== Description ==
== Description ==
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== Physical meaning ==
== Physical meaning ==
Bose-Einstein statistics explain blackbody radiation, collective excitations such as phonons, and the possibility of macroscopic occupation of a single quantum state. At low temperature, some bosonic systems can form a [[Physics:Quantum Bose-Einstein condensate|Bose-Einstein condensate]].
Bose-Einstein statistics explain blackbody radiation, collective excitations such as phonons, and the possibility of macroscopic occupation of a single quantum state. At low temperature, some bosonic systems can form a Bose-Einstein condensate.<ref>{{Cite journal |last=Ziff |first=R. M. |last2=Kac |first2=M. |last3=Uhlenbeck |first3=G. E. |title=The ideal Bose-Einstein gas, revisited |journal=Physics Reports |year=1977 |volume=32 |pages=169-248}}</ref>


== Historical names ==
== Historical names ==
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* [[Biography:Albert Einstein|Albert Einstein]] extended Bose's idea to material particles.
* [[Biography:Albert Einstein|Albert Einstein]] extended Bose's idea to material particles.


== Related concepts ==
== See also ==
* [[Physics:Quantum boson]]
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also/Matter}}
* [[Physics:Quantum photon]]
* [[Physics:Quantum Fermi–Dirac statistics]]
* [[Physics:Quantum Bose-Einstein condensate]]


== References ==
== References ==
{{reflist|3}}
{{reflist|3}}
* {{Cite journal |last=Bose |first=S. N. |title=Plancks Gesetz und Lichtquantenhypothese |journal=Zeitschrift für Physik |year=1924 |volume=26 |pages=178-181 |doi=10.1007/BF01327326}}
* {{Cite web |title=Bose-Einstein statistics |url=https://www.britannica.com/science/Bose-Einstein-statistics |website=Encyclopaedia Britannica |access-date=2026-05-23}}


{{Author|Harold Foppele}}
{{Author|Harold Foppele}}

Latest revision as of 22:58, 23 May 2026

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Bose–Einstein statistics is a Book II topic in the Quantum Collection. Bose–Einstein statistics describe the occupation of quantum states by identical bosons. They apply to particles with integer spin, including photons, gluons, phonons, and many composite particles.[1] Bose-Einstein statistics allow many identical bosons to occupy the same quantum state, which makes collective quantum behavior possible. They explain blackbody radiation, photon bunching, superfluidity, and Bose-Einstein condensation. The statistics arise from symmetric many-particle wavefunctions and contrast sharply with the exclusion behavior of fermions.

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Bose-Einstein statistics allow many bosons to occupy the same quantum state.

Description

Unlike fermions, bosons are not restricted by the Pauli exclusion principle. Many identical bosons can occupy the same quantum state. For a system in thermal equilibrium, the average occupation of a state with energy E is

n(E)=1exp((Eμ)/kBT)1

where μ is the chemical potential, kB is the Boltzmann constant, and T is temperature.

Physical meaning

Bose-Einstein statistics explain blackbody radiation, collective excitations such as phonons, and the possibility of macroscopic occupation of a single quantum state. At low temperature, some bosonic systems can form a Bose-Einstein condensate.[2]

Historical names

See also

Table of contents (84 articles)

Index

Full contents

References

  1. Annett, James F. (2004). Superconductivity, Superfluids and Condensates. New York: Oxford University Press. ISBN 0-19-850755-0. 
  2. Ziff, R. M.; Kac, M.; Uhlenbeck, G. E. (1977). "The ideal Bose-Einstein gas, revisited". Physics Reports 32: 169-248. 


Author: Harold Foppele