In quantum electrodynamics, Furry's theorem states that if a Feynman diagram consists of a closed loop of fermion lines with an odd number of vertices, its contribution to the amplitude vanishes. As a corollary, a single photon cannot arise from the vacuum or be absorbed by it. The theorem was first derived by Wendell H. Furry in 1937, as a direct consequence of the conservation of energy and charge conjugation symmetry.
Theory Quantum electrodynamics has a number of symmetries, one of them being the discrete symmetry of charge conjugation. This acts on fields through a unitary charge conjugation operator C {\displaystyle C} which anticommutes with the photon field A μ ( x ) {\displaystyle A_{\mu }(x)} as C A μ ( x ) C † = − A μ ( x ) {\displaystyle CA^{\mu }(x)C^{\dagger }=-A^{\mu }(x)} , while leaving the vacuum state invariant C | Ω ⟩ = | Ω ⟩ {\displaystyle C|\Omega \rangle =|\Omega \rangle } . Considering the simplest case of the correlation function of a single photon operator gives
⟨ Ω | A μ ( x ) | Ω ⟩ = ⟨ Ω | C † C A μ ( x ) C † C | Ω ⟩ = − ⟨ Ω | A μ ( x ) | Ω ⟩ , {\displaystyle \langle \Omega |A^{\mu }(x)|\Omega \rangle =\langle \Omega |C^{\dagger }CA^{\mu }(x)C^{\dagger }C|\Omega \rangle =-\langle \Omega |A^{\mu }(x)|\Omega \rangle ,}
so this correlation function must vanish. For n {\displaystyle n} photon operators, this argument shows that under charge conjugation this picks up a factor of ( − 1 ) n {\displaystyle (-1)^{n}} and thus vanishes when n {\displaystyle n} is odd. More generally, since the charge conjugation operator also anticommutes with the vector current j μ ( x ) {\displaystyle j^{\mu }(x)} , Furry's theorem states that the correlation function of any odd number of on-shell or off-shell photon fields and/or currents must vanish in quantum electrodynamics. Since the theorem holds at the non-perturbative level, it must also hold at each order in perturbation theory. At leading order this means that any fermion loop with an odd number of vertices must have a vanishing contribution to the amplitude. An explicit calculation of these diagrams reveals that this is because the diagram with a fermion going clockwise around the loop cancels with the second diagram where the fermion goes anticlockwise. The vanishing of the three vertex loop can also be seen as a consequence of the renormalizability of quantum electrodynamics since the bare Lagrangian does not have any counterterms involving three photons.
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