Mandel Q parameter
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The Mandel Q parameter measures the departure of the occupation number distribution from Poissonian statistics. It was introduced in quantum optics by Leonard Mandel.{{cite journal|last1=Mandel|first1=L.|title=Sub-Poissonian photon statistics in resonance fluorescence|journal=Optics Letters|volume=4|issue=7|year=1979|pages=205–7|issn=0146-9592|doi=10.1364/OL.4.000205|pmid=19687850|bibcode=1979OptL....4..205M}} 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:
:
where is the photon number operator and is the normalized second-order correlation function as defined by Glauber.{{cite journal|last1=Glauber|first1=Roy J.|title=The Quantum Theory of Optical Coherence|journal=Physical Review|volume=130|issue=6|year=1963|pages=2529–2539|issn=0031-899X|doi=10.1103/PhysRev.130.2529|bibcode=1963PhRv..130.2529G|doi-access=free}}
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.
:
The minimal value is obtained for photon number states (Fock states), which by definition have a well-defined number of photons and for which .
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 .Mandel, L., and Wolf, E., Optical Coherence and Quantum Optics (Cambridge 1995)
Coherent states have a Poissonian photon-number statistics for which .
References
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