Mandel Q parameter

The Mandel Q parameter measures the departure of the occupation number distribution from Poissonian statistics. It was introduced in quantum optics by L. Mandel.^[1] It is a convenient way to characterize non-classical states with negative values indicating a sub-Poissonian statistics, which have no classical analog. It is defined as the normalized variance of the boson distribution:

Q={\frac {\left\langle (\Delta {\hat {n}})^{2}\right\rangle -\langle {\hat {n}}\rangle }{\langle {\hat {n}}\rangle }}={\frac {\langle {\hat {n}}^{(2)}\rangle -\langle {\hat {n}}\rangle ^{2}}{\langle {\hat {n}}\rangle }}-1=\langle {\hat {n}}\rangle \left(g^{(2)}(0)-1\right)

where ${\hat {n}}$ is the photon number operator and $g^{{(2)}}$ is the normalized second-order correlation function as defined by Glauber.^[2]

Non-classical value

Negative values of Q corresponds to state which variance of photon number is less than the mean (equivalent to sub-Poissonian statistics). In this case, the phase space distribution cannot be interpreted as a classical probability distribution.

-1\leq Q<0\Leftrightarrow 0\leq \langle (\Delta {\hat {n}})^{2}\rangle \leq \langle {\hat {n}}\rangle

The minimal value $Q=-1$ is obtained for photon number states, which by definition have a well-defined number of photon and for which $\Delta n=0$ .

Examples

For black-body radiation, the phase-space functional is Gaussian. The resulting occupation distribution of the number state is characterized by a Bose–Einstein statistics for which $Q=\langle n\rangle$ .^[3]

Coherent states have a Poissonian photon-number statistics for which $Q=0$ .

References

↑ Mandel, L., Sub-Poissonian photon statistics in resonance fluorescence, Opt. Lett. 4:205 (1979)
↑ Glauber, R. J., The Quantum Theory of Optical Coherence, Phys. Rev. 130:2529 (1963)
↑ Mandel, L., and Wolf, E., Optical Coherence and Quantum Optics (Cambridge 1995)

Mandel Q parameter

Non-classical value

Examples

References

Further reading