Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Optics Communications

Quantum statistics of light after saturated two-photon emission processes and the photon statistics of a two-photon laser

A. Bandilla, H. Voigt

Published Oct 1, 1982• 10 citations
Publisher
DOI
10.1016/0030-4018(82)90397-2

Related papers

Quantum Statistics of Light after Two-photon Absorption and Emission Processes

Optica Acta International Journal of Optics•Nov 1, 1980•15 citations

Amplitude squeezing and sub-poissonian photon statistics in a two-photon correlated-spontaneous-emission laser

Luigi A. Lugiato, Ning Lü, Marlan O. Scully

Optics Communications•Jan 1, 1990•9 citations

Comparison of statistical properties of two models for saturated laser-light amplifier

C. Bendjaballah, Guy Oliver

Two models of saturated coherent light amplifier are studied and compared from the statistical point of view. For one of the models the absorption process is not saturated. The first- and second-order moments of the photon distribution exhibit very different behaviors according to the considered model. The reduced second-order moment measuring the fluctuations becomes more important when the absorption process is not saturated.

Physical Review A•Dec 1, 1980•8 citations

Photon Statistics of a Two-Mode Laser in the Presence of Two-Photon Processes

M. P. Sharma, P. R. P. Silva

Springer eBooks•Jan 1, 1984•0 citations

Lasing in Random Media

Hui W. Cao

A photon, unlike an electron, can stimulate an excited atom to emit a second photon into the same electromagnetic mode. This stimulated emission process is the foundation for light amplification and oscillation (i.e., self-generation). Initially, the term LASER referred to Light Amplification by Stimulated Emission of Radiation. Nowadays laser often means Light Oscillation by Stimulated Emission, which should literally be called "€œLOSER"€ instead of "€œLASER." To distinguish the above two devices, the former is called a laser amplifier, the latter a laser oscillator (Siegman 1986). Laser oscillation occurs when the photon generation rate exceeds the photon loss rate in a system. If gain saturation were absent, the photon number in a laser oscillator would diverge in time. In other words, the rate equation for the photon number would acquire an unstable solution above the oscillation threshold. In reality, gain saturation reduces the photon generation rate to the photon loss rate so that the number of photons in the oscillator remains at a finite value.

SPIE eBooks•Mar 16, 2010•3 citations

Photon statistics of a two-photon laser

Muhammad Suhail Zubairy

Physics Letters A•Dec 1, 1980•25 citations
A photon, unlike an electron, can stimulate an excited atom to emit a second photon into the same electromagnetic mode. This stimulated emission process is the foundation for light amplification and oscillation (i.e., self-generation). Initially, the term LASER referred to Light Amplification by Stimulated Emission of Radiation. Nowadays laser often means Light Oscillation by Stimulated Emission, which should literally be called "€œLOSER"€ instead of "€œLASER." To distinguish the above two devices, the former is called a laser amplifier, the latter a laser oscillator (Siegman 1986). Laser oscillation occurs when the photon generation rate exceeds the photon loss rate in a system. If gain saturation were absent, the photon number in a laser oscillator would diverge in time. In other words, the rate equation for the photon number would acquire an unstable solution above the oscillation threshold. In reality, gain saturation reduces the photon generation rate to the photon loss rate so that the number of photons in the oscillator remains at a finite value.