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Wick's Theorem


Wick's theorem expands a time-ordered product of free-field operators as a normal-ordered product plus the sum of all possible contractions. If the contraction of two operators is denoted by

 C_(ij)=T(A_iA_j)-:A_iA_j:,

then the four-operator bosonic case is

 T(A_1A_2A_3A_4)=:A_1A_2A_3A_4:+C_(12):A_3A_4:+C_(13):A_2A_4:+C_(14):A_2A_3:+C_(23):A_1A_4:+C_(24):A_1A_3:+C_(34):A_1A_2:+C_(12)C_(34)+C_(13)C_(24)+C_(14)C_(23).

Fermionic operators acquire signs from the permutations needed to form the contractions. The theorem reduces free-field correlation functions to two-point functions and is the operator counterpart of the Wick-Isserlis formula. Generalized Wick theorems replace vacuum normal ordering by contractions defined relative to another reference state, including particle-hole and multireference formulations.


See also

Normal Order, Quantum Field Theory, Wick-Isserlis Formula

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References

Wick, G. C. "The Evaluation of the Collision Matrix." Phys. Rev. 80, 268-272, 1950. https://doi.org/10.1103/PhysRev.80.268.

Cite this as:

Weisstein, Eric W. "Wick's Theorem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/WicksTheorem.html

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