Four Δ baryons exist: Δ++ (constituent quarks: uuu), Δ+ (uud), Δ0 (udd), and Δ− (ddd), which respectively carry an electric charge of +2 e, +1 e, 0 e, and −1 e.
The Δ baryons have a mass of about , a 1232 MeV/c2spin of 3/, and an isospin of 3/. In many ways, a Δ baryon is an 'excited' nucleon (symbol N). Nucleons are made of the same constituent quarks, but they are in a lower-energy spin configuration (spin 1/). The Δ+ (uud) and Δ0 (udd) particles are the higher-energy equivalent of the proton (N+, uud) and neutron (N0, udd), respectively. However, the Δ++ and Δ− have no nucleon equivalent.
The four Δ baryons are distinguished by their electrical charges, which is the sum of the charges of the quarks from which they are composed. There are also four antiparticles with opposite charges, made up of the corresponding antiquarks. The existence of the Δ++, with its unusual +2 charge, was a crucial clue in the development of the quark model.
All varieties of Δ baryons quickly decay via the strong force into a nucleon (proton or neutron) and a pion of appropriate charge. The amplitudes of various final charge states given by their respective isospin couplings. More rarely and more slowly, the Δ+ can decay into a proton and a photon and the Δ0 can decay into a neutron and a photon.
|Rest mass (MeV/c2)||I3||JP||Q (e)||S||C||B′||T||Mean lifetime (s)||Commonly decays to|
|Delta||Δ++(1232)||uuu||1,232 ± 2||+3⁄2||3⁄2+||+2||0||0||0||0||±0.14)×10−24(5.63[a]||p+ + π+|
|Delta||Δ+(1232)||uud||1,232 ± 2||+1⁄2||3⁄2+||+1||0||0||0||0||±0.14)×10−24(5.63[a]||π+ + n0 or
|Delta||Δ0(1232)||udd||1,232 ± 2||−1⁄2||3⁄2+||0||0||0||0||0||±0.14)×10−24(5.63[a]||π0 + n0 or
|Delta||Δ−(1232)||ddd||1,232 ± 2||−3⁄2||3⁄2+||−1||0||0||0||0||±0.14)×10−24(5.63[a]||π− + n0|
- J. Beringer et al. (2013): Particle listings – Δ(1232)