Generated by DeepSeek V3.2| down quark | |
|---|---|
| Name | down quark |
| Composition | Elementary particle |
| Statistics | Fermionic |
| Group | Quark |
| Generation | First |
| Interaction | Strong, Weak, Electromagnetic, Gravitational |
| Antiparticle | Antidown quark |
| Theorized | Murray Gell-Mann (1964), George Zweig (1964) |
| Discovered | SLAC National Accelerator Laboratory (1968) |
| Mass | ~4.7 MeV/c² |
| Electric charge | −1/3 ''e'' |
| Spin | 1/2 |
| Weak isospin | L: −1/2, R: 0 |
| Weak hypercharge | L: +1/3, R: −2/3 |
down quark. The down quark is a first-generation fermion and a fundamental constituent of matter, classified within the Standard Model of particle physics. With an electric charge of −1/3, it is one of the lightest quarks and a key building block of stable hadrons, most notably the proton and the neutron. Its existence was independently proposed by Murray Gell-Mann and George Zweig in 1964 as part of the quark model, and it was first observed in deep inelastic scattering experiments at the SLAC National Accelerator Laboratory in 1968.
The down quark is characterized by a relatively small mass of approximately 4.7 MeV/c², making it nearly twice as heavy as its partner, the up quark. It carries a fractional electric charge of −1/3, contrasting with the +2/3 charge of the up quark, and possesses a color charge, participating in the strong interaction mediated by gluons. As a spin-½ particle, it is subject to the Pauli exclusion principle and undergoes weak interactions, allowing it to decay into an up quark via the emission of a W boson. Its properties are defined within the framework of quantum chromodynamics, and its precise mass is a parameter in the Standard Model influenced by the Higgs mechanism.
The theoretical foundation for the down quark emerged from the work of Murray Gell-Mann and, independently, George Zweig in 1964, who sought to explain the patterns observed in the hadron spectrum. Gell-Mann's Eightfold Way classification scheme predicted the existence of fundamental constituents, which he termed quarks. Experimental confirmation came from the SLAC MIT team led by Richard E. Taylor, Henry W. Kendall, and Jerome I. Friedman, whose deep inelastic scattering experiments on protons at the Stanford Linear Accelerator Center in 1968 provided the first direct evidence for point-like particles inside nucleons, a discovery later recognized with the Nobel Prize in Physics in 1990. These findings solidified the quark model and the role of the down quark in the structure of atomic nuclei.
The down quark is a primary component of many hadrons, which are particles bound by the strong force. Most importantly, it combines with up quarks to form baryons such as the neutron (composed of two down quarks and one up quark) and the proton (composed of two up quarks and one down quark). It also appears in various mesons, including the pion (π⁻, consisting of a down quark and an antiup quark) and the kaon (K⁰, containing a down quark and a strange antiquark). Other particles like the Δ⁰ baryon and numerous resonances cataloged by the Particle Data Group also contain down quarks, playing crucial roles in strong interaction dynamics and nuclear physics.
* Up quark * Strange quark * Quantum chromodynamics * Deep inelastic scattering * Neutron * Proton * Quark model * Standard Model
Category:Quarks Category:Elementary particles Category:Subatomic particles