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- (−1)F abstract "In a quantum field theory with fermions, (−1)F is a unitary, Hermitian, involutive operator where F is the fermion number operator and is equal to the sum of the lepton number plus the baryon number, F=B+L, for all particles in the Standard Model. The action of this operator is to multiply bosonic states by 1 and fermionic states by −1. This is always a global internal symmetry of any quantum field theory with fermions and corresponds to a rotation by 2π. This splits the Hilbert space into two superselection sectors. Bosonic operators commute with (−1)F whereas fermionic operators anticommute with it.This operator really shows its utility in supersymmetric theories.".
- (−1)F wikiPageID "2704038".
- (−1)F wikiPageRevisionID "598530317".
- (−1)F subject Category:Quantum_field_theory.
- (−1)F subject Category:Supersymmetry.
- (−1)F comment "In a quantum field theory with fermions, (−1)F is a unitary, Hermitian, involutive operator where F is the fermion number operator and is equal to the sum of the lepton number plus the baryon number, F=B+L, for all particles in the Standard Model. The action of this operator is to multiply bosonic states by 1 and fermionic states by −1. This is always a global internal symmetry of any quantum field theory with fermions and corresponds to a rotation by 2π.".
- (−1)F label "(−1)F".
- (−1)F sameAs (%E2%88%921)F.
- (−1)F sameAs Q4544968.
- (−1)F sameAs Q4544968.
- (−1)F wasDerivedFrom (−1)F?oldid=598530317.