Coleman–Glashow mass formula

E674929

The Coleman–Glashow mass formula is a relation in particle physics that predicts mass differences among members of hadron multiplets by incorporating electromagnetic and symmetry-breaking effects.

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Coleman–Glashow mass formula canonical 1

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Predicate Object
instanceOf mass relation
physical law
theoretical physics concept
appliesTo SU(3) flavor multiplets
baryon decuplet
baryon octet
hadron multiplets
approximationLevel first-order symmetry breaking
assumes perturbative electromagnetic corrections
small SU(3) flavor symmetry breaking
basedOn SU(3) flavor symmetry NERFINISHED
approximate flavor symmetry
category mass formula in particle physics
concerns decuplet baryon mass splittings
octet baryon mass splittings
context hadron spectroscopy
quark model
describes effects of electromagnetic interactions on hadron masses
effects of flavor symmetry breaking on hadron masses
domain strong interaction phenomenology
field hadron physics
particle physics
quantum chromodynamics
incorporates electromagnetic effects
symmetry-breaking effects
influenced later studies of hadron mass relations
involves down quark mass
electromagnetic self-energies of hadrons
strange quark mass
up quark mass
language quantum field theory
mathematicalForm linear relation among hadron masses
namedAfter Sheldon Glashow NERFINISHED
Sidney Coleman NERFINISHED
predicts mass differences among hadrons
relatedTo Gell-Mann–Okubo mass formula NERFINISHED
quark mass differences
relates masses of members of the same multiplet
typeOf mass sum rule
usedFor estimating hadron mass splittings
testing SU(3) flavor symmetry
usedIn phenomenological fits to baryon masses
uses hypercharge
isospin symmetry
validIn approximate SU(3) flavor symmetry limit
yearProposed 1961

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Gell-Mann–Okubo mass formula relatedTo Coleman–Glashow mass formula