Abstract

We use the third- and fourth-order autocorrelation functions g(3)(τ1,τ2)g^{(3)}(τ_1,τ_2) and g(4)(τ1,τ2,τ3)g^{(4)}(τ_1,τ_2, τ_3) to detect the non-classical character of the light transmitted through a photonic-crystal nanocavity containing a strongly-coupled quantum dot probed with a train of coherent light pulses. We contrast the value of g(3)(0,0)g^{(3)}(0, 0) with the conventionally used g(2)(0)g^{(2)}(0) and demonstrate that in addition to being necessary for detecting two-photon states emitted by a low-intensity source, g(3)g^{(3)} provides a more clear indication of the non-classical character of a light source. We also present preliminary data that demonstrates bunching in the fourth-order autocorrelation function g(4)(τ1,τ2,τ3)g^{(4)}(τ_1,τ_2, τ_3) as the first step toward detecting three-photon states.

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