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- Fermionic_field abstract "In quantum field theory, a fermionic field is a quantum field whose quanta are fermions; that is, they obey Fermi–Dirac statistics. Fermionic fields obey canonical anticommutation relations rather than the canonical commutation relations of bosonic fields.The most prominent example of a fermionic field is the Dirac field, which describes fermions with spin-1/2: electrons, protons, quarks, etc. The Dirac field can be described as either a 4-component spinor or as a pair of 2-component Weyl spinors. Spin-1/2 Majorana fermions, such as the hypothetical neutralino, can be described as either a dependent 4-component Majorana spinor or a single 2-component Weyl spinor. It is not known whether the neutrino is a Majorana fermion or a Dirac fermion (see also Neutrinoless double-beta decay for experimental efforts to determine this).".
- Fermionic_field wikiPageExternalLink qft.html.
- Fermionic_field wikiPageID "2240310".
- Fermionic_field wikiPageRevisionID "598850351".
- Fermionic_field hasPhotoCollection Fermionic_field.
- Fermionic_field subject Category:Quantum_field_theory.
- Fermionic_field subject Category:Spinors.
- Fermionic_field comment "In quantum field theory, a fermionic field is a quantum field whose quanta are fermions; that is, they obey Fermi–Dirac statistics. Fermionic fields obey canonical anticommutation relations rather than the canonical commutation relations of bosonic fields.The most prominent example of a fermionic field is the Dirac field, which describes fermions with spin-1/2: electrons, protons, quarks, etc.".
- Fermionic_field label "Campo di Dirac".
- Fermionic_field label "Campo fermiónico".
- Fermionic_field label "Fermionic field".
- Fermionic_field label "狄拉克場".
- Fermionic_field sameAs Campo_fermiónico.
- Fermionic_field sameAs Campo_di_Dirac.
- Fermionic_field sameAs m.06ygvy.
- Fermionic_field sameAs Q768979.
- Fermionic_field sameAs Q768979.
- Fermionic_field wasDerivedFrom Fermionic_field?oldid=598850351.
- Fermionic_field isPrimaryTopicOf Fermionic_field.