Quantum Non-Demolition Measurements and Back-Action-Induced Squeezing in Atomic-Three-Level Systems View Full Text


Ontology type: schema:Chapter     


Chapter Info

DATE

1994

AUTHORS

P. Grangier , J.-Ph. Poizat , P. Grelu , F. Castelli , L. A. Lugiato , A. Sinatra

ABSTRACT

This paper deals with two topics: (a) the implementation of a quantum non-demolition (QND) measurement in the optical domain, using the two-photon non-linearity of three-level atoms placed inside a doubly-resonant optical cavity. (b) the experimental observation and theoretical interpretation of a squeezing effect which occurs in the same set-up, when the optical cavity is detuned from the exciting laser beams. The origin of this effect can be attributed to the transfer of the intensity fluctuations of one beam to the phase fluctuations of the other one, (similar to the information transfer which occurs in the QND measurement), followed by an optical feedback onto the intensity of the initial beam. This feedback effect is obtained through mixing of the phase and intensity quadratures, due to the detuning of the optical cavity which contains the nonlinear medium. More... »

PAGES

123-133

References to SciGraph publications

Book

TITLE

Quantum Optics VI

ISBN

978-3-642-79103-1
978-3-642-79101-7

Identifiers

URI

http://scigraph.springernature.com/pub.10.1007/978-3-642-79101-7_13

DOI

http://dx.doi.org/10.1007/978-3-642-79101-7_13

DIMENSIONS

https://app.dimensions.ai/details/publication/pub.1007603161


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32 schema:description This paper deals with two topics: (a) the implementation of a quantum non-demolition (QND) measurement in the optical domain, using the two-photon non-linearity of three-level atoms placed inside a doubly-resonant optical cavity.  (b) the experimental observation and theoretical interpretation of a squeezing effect which occurs in the same set-up, when the optical cavity is detuned from the exciting laser beams. The origin of this effect can be attributed to the transfer of the intensity fluctuations of one beam to the phase fluctuations of the other one, (similar to the information transfer which occurs in the QND measurement), followed by an optical feedback onto the intensity of the initial beam. This feedback effect is obtained through mixing of the phase and intensity quadratures, due to the detuning of the optical cavity which contains the nonlinear medium.  
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