Delta baryon
Template:Short description Template:Infobox Particle
The Delta baryons (or Template:Math baryons, also called Delta resonances) are a family of subatomic particle made of three up or down quarks (u or d quarks), the same constituent quarks that make up the more familiar protons and neutrons.
Properties
Four closely related Template:Math baryons exist: Template:SubatomicParticle (constituent quarks: uuu), Template:Subatomic Particle (uud), Template:SubatomicParticle (udd), and Template:SubatomicParticle (ddd), which respectively carry an electric charge of Template:Val, Template:Val, Template:Val, and Template:Val.
The Template:Math baryons have a mass of about Template:Val; their third component of isospin and they are required to have an intrinsic spin of Template:Sfrac or higher (half-integer units). Ordinary nucleons (symbol N, meaning either a proton or neutron), by contrast, have a mass of about Template:Val, and both intrinsic spin and isospin of Template:Sfrac. The Template:Math (uud) and Template:Math (udd) particles are higher-mass spin-excitations of the proton (Template:SubatomicParticle, uud) and neutron (Template:SubatomicParticle, udd), respectively. The Template:Math and Template:Math, however, have no direct nucleon analogues: For example, even though their charges are identical and their masses are similar, the Template:Math (ddd), is not closely related to the antiproton (Template:SubatomicParticle, uud).
The Delta states discussed here are only the lowest-mass quantum excitations of the proton and neutron. At higher spins, additional higher mass Delta states appear, all defined by having constant Template:Sfrac or Template:Sfrac isospin (depending on charge), but with spin Template:Sfrac, Template:Sfrac, Template:Sfrac, ..., Template:Sfrac multiplied by [[reduced Planck constant|Template:Mvar]]. A complete listing of all properties of all these states can be found in Beringer et al. (2013).[1]
There also exist antiparticle Delta states with opposite charges, made up of the corresponding antiquarks.
Discovery
The states were established experimentally at the University of Chicago cyclotron[2][3] and the Carnegie Institute of Technology synchro-cyclotron[4] in the mid-1950s using accelerated positive pions on hydrogen targets. The existence of the Template:Math, with its unusual electric charge of Template:Val, was a crucial clue in the development of the quark model.
Formation and decay
The Delta states are created when a sufficiently energetic probe – such as a photon, electron, neutrino, or pion – impinges upon a proton or neutron, or possibly by the collision of a sufficiently energetic nucleon pair.
All of the Δ baryons with mass near Template:Val quickly decay via the strong interaction into a nucleon (proton or neutron) and a pion of appropriate charge. The relative probabilities of allowed final charge states are given by their respective isospin couplings. More rarely, the Template:SubatomicParticle can decay into a proton and a photon and the Template:SubatomicParticle can decay into a neutron and a photon.
List
[a] <templatestyles src="Citation/styles.css"/>^ PDG reports the resonance width (Γ). Here the conversion is given instead.
References
Bibliography
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