Hadron

From Academic Kids

In particle physics, a hadron is a subatomic particle which experiences the strong nuclear force. These are not fundamental particles but are composed of fermions, called quarks and antiquarks, and of bosons, called gluons. The gluons mediate the color force that binds the quarks together.

Like all subatomic particles, hadrons have quantum numbers corresponding to the representations of the Poincare group: JPC(m), where J is the spin, P, the parity, C, the C parity, and m, the mass. In addition they may carry flavour quantum numbers such as isospion (or G parity), strangeness etc. Hadrons can be further divided into two classes—

Most hadrons can be classified by the quark model which posits that all the quantum numbers of baryons are derived from those of the valence quarks. For a baryon these are three quarks and for a meson these are a quark-antiquark pair. Clearly then, each quark is a fermion with B=1/3. Excited baryon or meson states are known as resonances. Each ground state hadron may have many excited states, and hundreds have been observed in particle experiments. Resonances decay extremely quickly (within about 10−24 s) via strong interactions.

Mesons which lie outside the quark model classification are called exotic mesons. These include glueballs, hybrid mesons and tetraquarks. The only baryons which lie outside the quark model at present are the pentaquarks, but the evidence for their existence is unclear as of 2005.

All hadrons are single particle excitations of the basic theory of strong interactions, called quantum chromodynamics. Due to a property called confinement that this theory enjoys, these excitations are not quarks and gluons, which are the basic fields, but the hadrons which are composite, and carry no color charge. In other phases of QCD matter the hadrons may disappear.

See also

References and external links

Particles in Physics - Composite particles

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