### Abstract

The higher order Q-parameter, Q^{(N)}, N = 1,2,3, ..., is introduced to generalize the sub-Poissonian photon statistics of light into higher order. By the definition, Q^{(1)} is identical to the well-known Mandel's Q-parameter. We show that Q^{(N)}s are -1 for the number state and 0 for the coherent state for all N. For the thermal light, however, Q^{(N)} s depend upon the average photon number. We discussed the characteristics of the higher order Q-parameter in particular examples where the light fields have higher order (N ≥ 2) sub-Poissonian photon statistics but not the ordinary (N = 1) sub-Poissonian photon statistics. It is also shown that the nonclassical measure of the higher order sub-Poissonian photon statistics of the number state are 1/2 as same as that of the known lowest order. It means that a superposition with thermal noise with the average photon number 1/2 remove the higher order sub-Poissonian photon statistics from the number state.

Original language | English |
---|---|

Pages (from-to) | 107-114 |

Number of pages | 8 |

Journal | Optics Communications |

Volume | 212 |

Issue number | 1-3 |

DOIs | |

Publication status | Published - 2002 Oct 15 |

Externally published | Yes |

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### ASJC Scopus subject areas

- Atomic and Molecular Physics, and Optics

### Cite this

*Optics Communications*,

*212*(1-3), 107-114. https://doi.org/10.1016/S0030-4018(02)01981-8

**Higher order sub-Poissonian photon statistics of light.** / Kim, Youngchul; Yoon, Tai Hyun.

Research output: Contribution to journal › Article

*Optics Communications*, vol. 212, no. 1-3, pp. 107-114. https://doi.org/10.1016/S0030-4018(02)01981-8

}

TY - JOUR

T1 - Higher order sub-Poissonian photon statistics of light

AU - Kim, Youngchul

AU - Yoon, Tai Hyun

PY - 2002/10/15

Y1 - 2002/10/15

N2 - The higher order Q-parameter, Q(N), N = 1,2,3, ..., is introduced to generalize the sub-Poissonian photon statistics of light into higher order. By the definition, Q(1) is identical to the well-known Mandel's Q-parameter. We show that Q(N)s are -1 for the number state and 0 for the coherent state for all N. For the thermal light, however, Q(N) s depend upon the average photon number. We discussed the characteristics of the higher order Q-parameter in particular examples where the light fields have higher order (N ≥ 2) sub-Poissonian photon statistics but not the ordinary (N = 1) sub-Poissonian photon statistics. It is also shown that the nonclassical measure of the higher order sub-Poissonian photon statistics of the number state are 1/2 as same as that of the known lowest order. It means that a superposition with thermal noise with the average photon number 1/2 remove the higher order sub-Poissonian photon statistics from the number state.

AB - The higher order Q-parameter, Q(N), N = 1,2,3, ..., is introduced to generalize the sub-Poissonian photon statistics of light into higher order. By the definition, Q(1) is identical to the well-known Mandel's Q-parameter. We show that Q(N)s are -1 for the number state and 0 for the coherent state for all N. For the thermal light, however, Q(N) s depend upon the average photon number. We discussed the characteristics of the higher order Q-parameter in particular examples where the light fields have higher order (N ≥ 2) sub-Poissonian photon statistics but not the ordinary (N = 1) sub-Poissonian photon statistics. It is also shown that the nonclassical measure of the higher order sub-Poissonian photon statistics of the number state are 1/2 as same as that of the known lowest order. It means that a superposition with thermal noise with the average photon number 1/2 remove the higher order sub-Poissonian photon statistics from the number state.

UR - http://www.scopus.com/inward/record.url?scp=0037107946&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=0037107946&partnerID=8YFLogxK

U2 - 10.1016/S0030-4018(02)01981-8

DO - 10.1016/S0030-4018(02)01981-8

M3 - Article

AN - SCOPUS:0037107946

VL - 212

SP - 107

EP - 114

JO - Optics Communications

JF - Optics Communications

SN - 0030-4018

IS - 1-3

ER -