An ideal projective measurement of the field's photon number selects the coefficient of . ThereforeWhenever this probability is nonzero, normalization of the projected joint quantum state gives the atomic Bell stateup to a common global phase. The maximum heralding probability is , attained at . At a time with , that conditioning event is impossible, so a conditional state is not defined there. The interpretation is a photon number measurement at the selected time; continuous monitoring of escaping photons would instead change the dynamics and require a different model.
Articles by others on the same topic
There are currently no matching articles.