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

Nondegenerate four-wave mixing in a cavity: instabilities and quantum noise reduction

Massimo Brambilla, F. Castelli, Luigi A. Lugiato, Franco Prati, G. Strini

Published Jun 1, 1991• 34 citations
Publisher
DOI
10.1016/0030-4018(91)90072-l

Related papers

Quantum Noise Reduction and Instabilities in Nondegenerate Four-Wave-Mixing

Massimo Brambilla, F. Castelli, Luigi A. Lugiato +2 more

NATO ASI series. Series B : Physics•Jan 1, 1992•1 citation

Quantum noise reduction in non-degenerate four-wave-mixing oscillators

F. Castelli, Pierfranco Dotti

Optics Communications•Dec 1, 1994•6 citations

Polarization instability in anisotropic-cavity degenerate four-wave mixing

V. J. Sánchez-Morcillo, Germán J. de Valcárcel, Eugenio Roldán

Optics Communications•Jan 1, 2000•6 citations

Instabilities and quantum noise reduction in nonlinear optical mixing

Massimo Brambilla, F. Castelli, A. Gatti +2 more

Nondegenerate four-wave-mixing (fwm) is a process by which one or two pump fields generate two signal beams, with conservation of the total photon energy and momentum. The signal beams can be distinguished by their frequency, or by their wave vector, or by their polarization. When the nonlinear medium which creates the fwm process is contained in a resonant cavity, the signal generation is caused by an instability, because the signal fields experience gain (fwm gain), and when this gain overcomes the cavity losses the signal beams build up. This chapter discusses several static and dynamical instabilities which arise from nondegenerate fwm. It considers a cavity with plane mirrors and examines the properties of quantum noise reduction which arise in the intensity difference between the signal beams generated by the fwm process. The chapter illustrates the problem of Gauss-Laguerre transverse modes in a ring cavity with spherical mirrors.

CRC Press eBooks•May 4, 2018•3 citations

Quantum Noise Measurements in Degenerate Four-Wave Mixing

Prem Kumar, Roy S. Bondurant, Jeffrey H. Shapiro +1 more

Springer eBooks•Jan 1, 1984•0 citations

Strong low-frequency quantum correlations from a four-wave-mixing amplifier

Colin F. McCormick, Alberto M. Marino, Vincent Boyer +1 more

Using a simple scheme based on nondegenerate four-wave mixing in a hot vapor, we generate bright twin beams which display a quantum noise reduction in the intensity difference of more than $8\phantom{\rule{0.3em}{0ex}}\mathrm{dB}$. The absence of a cavity makes the system immune to external perturbations, and strong quantum noise reduction is observed at frequencies as low as $4.5\phantom{\rule{0.3em}{0ex}}\mathrm{kHz}$ and over a large frequency range.

arXiv:quant-ph/0703111•Physical Review A•Oct 15, 2008•265 citations
Nondegenerate four-wave-mixing (fwm) is a process by which one or two pump fields generate two signal beams, with conservation of the total photon energy and momentum. The signal beams can be distinguished by their frequency, or by their wave vector, or by their polarization. When the nonlinear medium which creates the fwm process is contained in a resonant cavity, the signal generation is caused by an instability, because the signal fields experience gain (fwm gain), and when this gain overcomes the cavity losses the signal beams build up. This chapter discusses several static and dynamical instabilities which arise from nondegenerate fwm. It considers a cavity with plane mirrors and examines the properties of quantum noise reduction which arise in the intensity difference between the signal beams generated by the fwm process. The chapter illustrates the problem of Gauss-Laguerre transverse modes in a ring cavity with spherical mirrors.
Using a simple scheme based on nondegenerate four-wave mixing in a hot vapor, we generate bright twin beams which display a quantum noise reduction in the intensity difference of more than 8dB8\phantom{\rule{0.3em}{0ex}}\mathrm{dB}8dB. The absence of a cavity makes the system immune to external perturbations, and strong quantum noise reduction is observed at frequencies as low as 4.5kHz4.5\phantom{\rule{0.3em}{0ex}}\mathrm{kHz}4.5kHz and over a large frequency range.