A hadron is a composite subatomic particle made of quarks held together by the strong nuclear force.Hadrons are a class of subatomic particles that participate in the strong interaction. They are not fundamental but consist of quarks held together by gluons (carriers of the strong interaction). The name comes from the Greek 'hadros' meaning massive, reflecting their relatively large mass compared to leptons (e.g., electrons). Hadrons include protons and neutrons (baryons, fermions with half-integer spin), as well as mesons (bosons with integer spin). Inside a hadron, quarks are bound so tightly that free quarks are not observed—this is the property of confinement.
The concept of hadrons became established by the mid-20th century as the number of discovered particles grew rapidly. In 1961, Murray Gell-Mann and Yuval Ne'eman proposed a classification of hadrons based on the SU(3) group, leading to the prediction of the Ω⁻ baryon. In 1964, Gell-Mann and, independently, George Zweig introduced the quark hypothesis. Experimental confirmation of quarks was obtained in the late 1960s in electron-proton scattering experiments at SLAC. The development of QCD in the 1970s (Gross, Wilczek, Politzer) explained the dynamics of the strong interaction.
Hadrons arise due to confinement: the color charges of quarks are attracted by gluons so strongly that the potential energy grows linearly with distance. When attempting to separate quarks, the gluon field string breaks, producing a quark-antiquark pair from the vacuum, leading to hadronization—the formation of jets of hadrons. This is described by the laws of QCD, in which asymptotic freedom and infrared slavery are important. Hadron masses are calculated using lattice QCD. The Pauli principle explains why baryons have an antisymmetric color wave function: the three quarks must be of different colors.
Understanding hadrons explains the structure of matter and allows studying the forces inside atomic nuclei, which is applied in nuclear energy and medical imaging (PET scanning).
Although the proton appears stable, some theories predict that it could decay over an unimaginably long time—more than 10³⁴ years. Such decay has not yet been observed.










