In particle physics, a hadron i// (Greek: ἁδρός, hadrós, "stout, thick") is a composite particle made of quarks held together by the strong force (in the same way as atoms and molecules are held together by the electromagnetic force).
Hadrons are categorized into two families:
- baryons, such as protons and neutrons, made of three quarks
- mesons, such as pions, made of one quark and one antiquark.
Of the hadrons, protons and neutrons bound to atomic nuclei are stable, while others are unstable under ordinary conditions; free neutrons decay in 15 minutes. Experimentally, hadron physics is studied by colliding protons or nuclei of heavy elements such as lead, and detecting the debris in the produced particle showers.
Not withstanding the fact that this report deals with weak interactions, we shall frequently have to speak of strongly interacting particles. These particles pose not only numerous scientific problems, but also a terminological problem. The point is that "strongly interacting particles" is a very clumsy term which does not yield itself to the formation of an adjective. For this reason, to take but one instance, decays into strongly interacting particles are called non-leptonic. This definition is not exact because "non-leptonic" may also signify "photonic". In this report I shall call strongly interacting particles "hadrons", and the corresponding decays "hadronic" (the Greek ἁδρός signifies "large", "massive", in contrast to λεπτός which means "small", "light"). I hope that this terminology will prove to be convenient. –Lev B. Okun, 1962
According to the quark model, the properties of hadrons are primarily determined by their so-called valence quarks. For example, a proton is composed of two up quarks (each with electric charge +2⁄3, for a total of +4⁄3 together) and one down quark (with electric charge −1⁄3). Adding these together yields the proton charge of +1. Although quarks also carry color charge, hadrons must have zero total color charge because of a phenomenon called color confinement. That is, hadrons must be "colorless" or "white". These are the simplest of the two ways: three quarks of different colors, or a quark of one color and an antiquark carrying the corresponding anticolor. Hadrons with the first arrangement are called baryons, and those with the second arrangement are mesons.
Like all subatomic particles, hadrons are assigned quantum numbers corresponding to the representations of the Poincaré group: JPC(m), where J is the spin quantum number, P the intrinsic parity (or P-parity), and C, the charge conjugation (or C-parity), and the particle's mass, m. Note that the mass of a hadron has very little to do with the mass of its valence quarks; rather, due to mass–energy equivalence, most of the mass comes from the large amount of energy associated with the strong interaction. Hadrons may also carry flavor quantum numbers such as isospin (or G parity), and strangeness. All quarks carry an additive, conserved quantum number called a baryon number (B), which is +1⁄3 for quarks and −1⁄3 for antiquarks. This means that baryons (groups of three quarks) have B = 1 while mesons have B = 0.
Hadrons have excited states known as resonances. Each ground state hadron may have several excited states; several hundreds of resonances have been observed in particle physics experiments. Resonances decay extremely quickly (within about 10−24 seconds) via the strong nuclear force.
In other phases of matter the hadrons may disappear. For example, at very high temperature and high pressure, unless there are sufficiently many flavors of quarks, the theory of quantum chromodynamics (QCD) predicts that quarks and gluons will no longer be confined within hadrons because the strength of the strong interaction diminishes with energy. This property, which is known as asymptotic freedom, has been experimentally confirmed in the energy range between 1 GeV (gigaelectronvolt) and 1 TeV (teraelectronvolt).
All known baryons are made of three valence quarks, so they are fermions (i.e. they have odd half-integral spin because they have an odd number of quarks). As quarks possess baryon number B = 1⁄3, baryons have baryon number B = 1. The best-known baryons are the proton and the neutron.
One can hypothesise baryons with further quark–antiquark pairs in addition to their three quarks. Hypothetical baryons with one extra quark–antiquark pair (5 quarks in all) are called pentaquarks. Several pentaquark candidates were found in the early 2000s, but upon further review these states have now been established as non-existent. (This does not rule against pentaquarks in general, only the candidates put forward).
Each type of baryon has a corresponding antiparticle (antibaryon) in which quarks are replaced by their corresponding antiquarks. For example: just as a proton is made of two up-quarks and one down-quark, its corresponding antiparticle, the antiproton, is made of two up-antiquarks and one down-antiquark.
Mesons are hadrons composed of a quark–antiquark pair. They are bosons (integral spin – i.e. 0, 1, or -1 – as they have an even number of quarks). They have baryon number B = 0. Examples of mesons commonly produced in particle physics experiments include pions and kaons. Pions also play a role in holding atomic nuclei together via the residual strong force.
In principle, mesons with more than one quark–antiquark pair may exist; a hypothetical meson with two pairs is called a tetraquark. Several tetraquark candidates were found in the 2000s, but their status is under debate. Several other hypothetical "exotic" mesons lie outside the quark model of classification. These include glueballs and hybrid mesons (mesons bound by excited gluons).
See also 
|Look up hadron in Wiktionary, the free dictionary.|
- Hadronization, the formation of hadrons out of quarks and gluons
- Large Hadron Collider (LHC)
- List of particles
- Standard model
- Subatomic particles
- Hadron therapy, aka Particle beam therapy
- W.-M. Yao et al. (2006): Particle listings – Θ+
- C. Amsler et al. (2008): Pentaquarks
- L.B. Okun (1962). "The Theory of Weak Interaction". Proceedings of 1962 International Conference on High-Energy Physics at CERN. Geneva. p. 845. Bibcode:1962hep..conf..845O.
- C. Amsler et al. (Particle Data Group) (2008). "Review of Particle Physics – Quark Model". Physics Letters B 667: 1. Bibcode:2008PhLB..667....1P. doi:10.1016/j.physletb.2008.07.018.
- S. Bethke (2007). "Experimental tests of asymptotic freedom". Progress in Particle and Nuclear Physics 58 (2): 351. arXiv:hep-ex/0606035. Bibcode:2007PrPNP..58..351B. doi:10.1016/j.ppnp.2006.06.001.
- S. Kabana (2005). "AIP Conference Proceedings". arXiv:hep-ex/0503020 [hep-ex]. doi:10.1063/1.1920947.
- C. Amsler et al. (Particle Data Group) (2008). "Review of Particle Physics – Pentaquarks". Physics Letters B 667: 1. Bibcode:2008PhLB..667....1P. doi:10.1016/j.physletb.2008.07.018.