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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. It's trace is often a useful computation.".
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- (−1)F wikiPageExternalLink v=onepage&q=%22(-1)F%22&f=false.
- (−1)F wikiPageExternalLink v=onepage&q=fermion%20%22(-1)F%22&f=false.
- (−1)F wikiPageExternalLink v=onepage&q=fermion%20%22(-1)F%22&f=false.
- (−1)F wikiPageID "2704038".
- (−1)F wikiPageLength "2871".
- (−1)F wikiPageOutDegree "21".
- (−1)F wikiPageRevisionID "637966854".
- (−1)F wikiPageWikiLink Anticommutativity.
- (−1)F wikiPageWikiLink Anticommute.
- (−1)F wikiPageWikiLink Boson.
- (−1)F wikiPageWikiLink Category:Quantum_field_theory.
- (−1)F wikiPageWikiLink Category:Supersymmetry.
- (−1)F wikiPageWikiLink Commutative_property.
- (−1)F wikiPageWikiLink Commutativity.
- (−1)F wikiPageWikiLink Fermion.
- (−1)F wikiPageWikiLink Hermitian_operator.
- (−1)F wikiPageWikiLink Internal_symmetry.
- (−1)F wikiPageWikiLink Involution_(mathematics).
- (−1)F wikiPageWikiLink Local_symmetry.
- (−1)F wikiPageWikiLink Möbius_function.
- (−1)F wikiPageWikiLink Number_operator.
- (−1)F wikiPageWikiLink Operator_(mathematics).
- (−1)F wikiPageWikiLink Parity_(physics).
- (−1)F wikiPageWikiLink Particle_number_operator.
- (−1)F wikiPageWikiLink Primon_gas.
- (−1)F wikiPageWikiLink Quantum_field_theory.
- (−1)F wikiPageWikiLink Self-adjoint_operator.
- (−1)F wikiPageWikiLink Superselection.
- (−1)F wikiPageWikiLink Superselection_sector.
- (−1)F wikiPageWikiLink Supersymmetry.
- (−1)F wikiPageWikiLink Unitary_operator.
- (−1)F wikiPageWikiLink Witten_index.
- (−1)F wikiPageWikiLinkText "(−1)F".
- (−1)F hasPhotoCollection (−1)F.
- (−1)F wikiPageUsesTemplate Template:Cite_book.
- (−1)F wikiPageUsesTemplate Template:Merge.
- (−1)F wikiPageUsesTemplate Template:Multiple_issues.
- (−1)F wikiPageUsesTemplate Template:Quantum-stub.
- (−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 m.07z16q.
- (−1)F sameAs Q4544968.
- (−1)F sameAs Q4544968.
- (−1)F wasDerivedFrom (−1)F?oldid=637966854.
- (−1)F isPrimaryTopicOf (−1)F.