In particle physics, a **boson** (/ˈboʊzɒn/^{[1]} /ˈboʊsɒn/^{[2]}) is a subatomic particle whose spin quantum number has an integer value (0,1,2 ...). Bosons form one of the two fundamental classes of subatomic particle, the other being fermions, which have odd half-integer spin (1⁄2,3⁄2,5⁄2 ...). Every observed subatomic particle is either a boson or a fermion.

Some bosons are elementary particles occupying a special role in particle physics, distinct from the role of fermions (which are sometimes described as the constituents of "ordinary matter"). Certain elementary bosons (e.g. gluons) act as force carriers, which give rise to forces between other particles, while one (the Higgs boson) gives rise to the phenomenon of mass. Other bosons, such as mesons, are composite particles made up of smaller constituents.

Outside the realm of particle physics, multiple identical composite bosons (in this context sometimes known as '**bose particles**') behave at high densities or low temperatures in a characteristic manner described by Bose–Einstein statistics: for example a gas of helium-4 atoms condenses to becomes a superfluid at temperatures close to absolute zero. Similarly, superconductivity arises because some quasiparticles, such as Cooper pairs, behave in the same way.

The name *boson* was coined by Paul Dirac^{[3]}^{[4]} 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,^{[5]}^{[6]} who developed, in conjunction with Albert Einstein, the theory characterising such particles, now known as Bose–Einstein statistics.^{[7]}

Standard Model of particle physics |
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See also: List of particles § Bosons |

All observed elementary particles are either bosons (with integer spin) or fermions (with odd half-integer spin).^{[8]} Whereas the elementary particles that make up ordinary matter (leptons and quarks) are fermions, elementary bosons occupy a special role in particle physics. They act either as force carriers which give rise to forces between other particles, or in one case give rise to the phenomenon of mass.

According to the Standard Model of Particle Physics there are five elementary bosons:

- One
*scalar boson*(spin=0)^{}_{}H^{0}_{}Higgs boson – the particle that gives rise to the phenomenon of mass via the Higgs mechanism

- Four
*vector bosons*(spin=1) that act as force carriers. These are the gauge bosons:^{}_{}γ^{}_{}Photon – the force carrier of the electromagnetic field^{}_{}g^{}_{}Gluons (eight different types) – force carriers that mediate the strong force^{}_{}Z^{}_{}Neutral weak boson – the force carrier that mediates the weak force^{}_{}W^{±}_{}Charged weak bosons (two types) – also force carriers that mediate the weak force

A *tensor boson* (spin=2) called the graviton (G) has been hypothesised as the force carrier for gravity, but so far all attempts to incorporate gravity into the Standard Model have failed.^{[a]}

See also: List of particles § Composite particles |

Composite particles (such as hadrons, nuclei, and atoms) can be bosons or fermions depending on their constituents. Since bosons have integer spin and fermions odd half-integer spin, any composite particle made up of an even number of fermions is a boson.

Composite bosons include:

- All types of meson
- Stable nuclei of even mass number such as deuterium, helium-4 (the alpha particle),
^{[9]}carbon-12 and lead-208.^{[b]}

As quantum particles, the behaviour of multiple indistinguishable bosons at high densities is described by Bose–Einstein statistics. One characteristic which becomes important in superfluidity and other applications of Bose–Einstein condensates is that there is no restriction on the number of bosons that may occupy the same quantum state. As a consequence, when for example a gas of helium-4 atoms is cooled to temperatures very close to absolute zero and the kinetic energy of the particles becomes negligible, it condenses into a low-energy state and becomes a superfluid.

Certain quasiparticles are observed to behave as bosons and to follow Bose–Einstein statistics, including Cooper pairs, plasmons and phonons.^{[10]}^{: 130 }