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

Springer eBooks

Generalised Dispersion Relations and Optical Bistability in Squeezed Vacua

R. K. Bullought, Hanan Ali Batarfi, Saad S. M. Hassan, Munir Ibrahim, R. Saunders

Published Jan 1, 1996• 1 citation
Publisher
DOI
10.1007/978-1-4757-9742-8_106

Related papers

Generalized Dispersion Relations for Dielectrics in Squeezed Vacua

Saad S. M. Hassan, R. Bullough, R. Saunders +1 more

Springer eBooks•Jan 1, 1995•0 citations

Bistable behaviour in squeezed vacua: II. Stability analysis and chaos

Hanan Ali Batarfi, Saad S. M. Hassan, R. Saunders +1 more

The European Physical Journal D•Jul 1, 2000•16 citations

Bistable behaviour in squeezed vacua: I. Stationary analysis

Saad S. M. Hassan, Hanan Ali Batarfi, R. Saunders +1 more

The European Physical Journal D•Feb 1, 2000•20 citations

Generalized dispersion relations and optical bistability in squeezed vacua

R. Bullough, Hanan Ali Batarfi, Saad S. M. Hassan +2 more

We derive c-number Bloch-Maxwell (B-M) type equations from a quantum theory for 2-level atoms occupying a macroscopic slab-like region V of width L stimulated by a coherent-state electromagnetic field of radial frequency (omega) plus a broad-band correlated squeezed vacuum field with carrier frequency (omega) p. The squeezed vacuum field is in principle of arbitrary 3-dimensional geometry including geometries created by an optical parametric oscillator. The c-number spatially dependent B-M equations are solved self-consistently and 'exactly' in terms of a nonlinear dispersive refractive index m((omega) ) while the slab V acts, also self-consistently, as a natural Fabry-Perot cavity of finite spacing L. Very preliminary results for optical bistability in the squeezed vacuum and more exact results for anomalous dispersion and absorption in the squeezed vacuum in linearized approximation are reported. Finally we compute the effect of the dielectric on the free-field modes of the squeezed vacuum.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•May 6, 1996•5 citations

Squeezing and quantum noise correlations in dispersive two-photon optical bistability

Philippe Grangier, Jean-François Roch

Presents an analysis of a two-photon double-beam bistable device, in the dispersive and high-finesse limits. The expressions for the mean fields inside the cavity are given above the destabilization thresholds, and quantum fluctuations of the outcoming fields are analyzed below these thresholds. It appears that this device yields several new quantum noise reduction schemes, which are closely related to the mean fields behaviour.

Quantum Optics Journal of the European Optical Society Part B•Sep 1, 1989•19 citations

Generation of Squeezed States in Optical Bistability

David A. Holm, M. Sargent, Barbara A. Capron

Springer proceedings in physics•Jan 1, 1986•0 citations
We derive c-number Bloch-Maxwell (B-M) type equations from a quantum theory for 2-level atoms occupying a macroscopic slab-like region V of width L stimulated by a coherent-state electromagnetic field of radial frequency (omega) plus a broad-band correlated squeezed vacuum field with carrier frequency (omega) p. The squeezed vacuum field is in principle of arbitrary 3-dimensional geometry including geometries created by an optical parametric oscillator. The c-number spatially dependent B-M equations are solved self-consistently and 'exactly' in terms of a nonlinear dispersive refractive index m((omega) ) while the slab V acts, also self-consistently, as a natural Fabry-Perot cavity of finite spacing L. Very preliminary results for optical bistability in the squeezed vacuum and more exact results for anomalous dispersion and absorption in the squeezed vacuum in linearized approximation are reported. Finally we compute the effect of the dielectric on the free-field modes of the squeezed vacuum.