The optical equivalence theorem in quantum optics asserts an equivalence between the expectation value of an operator in Hilbert space and the expectation value of its associated function in the phase space formulation with respect to a quasiprobability distribution.
The theorem was first reported by George Sudarshan in 1963 for normally ordered operators[1] and generalized later that decade to any ordering.
[2][3][4][5] Let Ω be an ordering of the non-commutative creation and annihilation operators, and let
Then the optical equivalence theorem is succinctly expressed as
Here, α is understood to be the eigenvalue of the annihilation operator on a coherent states and is replaced formally in the power series expansion of g. The left side of the above equation is an expectation value in the Hilbert space whereas the right hand side is an expectation value with respect to the quasiprobability distribution.
This means that g can be written in a power series of the following form: The quasiprobability distribution associated with the normal order is the Glauber–Sudarshan P representation.
In these terms, we arrive at This theorem implies the formal equivalence between expectation values of normally ordered operators in quantum optics and the corresponding complex numbers in classical optics.