Transverse Effects and Noise in Optical Instabilities
We analyse the simplest model that describes the dynamics of a two-level, optically bistable system in a ring cavity, and incorporates a Gaussian radial variation of the electric field. We find that the most favourable situation to achieve self-pulsing instabilities is that of atomic and cavity detu...
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Veröffentlicht in: | Philosophical transactions of the Royal Society of London. Series A: Mathematical and physical sciences 1984-12, Vol.313 (1525), p.291-297 |
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container_title | Philosophical transactions of the Royal Society of London. Series A: Mathematical and physical sciences |
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creator | Lugiato, L. A. Horowicz, R. J. Strini, G. Narducci, L. M. |
description | We analyse the simplest model that describes the dynamics of a two-level, optically bistable system in a ring cavity, and incorporates a Gaussian radial variation of the electric field. We find that the most favourable situation to achieve self-pulsing instabilities is that of atomic and cavity detunings with opposite sign. The results are compared with those of plane-wave theory. We show that noise plays a primary role at the onset of self-oscillatory instabilities, and that its effects are governed by an equation formally identical to the Risken equation for the laser. |
doi_str_mv | 10.1098/rsta.1984.0109 |
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A</addtitle><date>1984-12-18</date><risdate>1984</risdate><volume>313</volume><issue>1525</issue><spage>291</spage><epage>297</epage><pages>291-297</pages><issn>1364-503X</issn><issn>0080-4614</issn><eissn>1471-2962</eissn><eissn>2054-0272</eissn><abstract>We analyse the simplest model that describes the dynamics of a two-level, optically bistable system in a ring cavity, and incorporates a Gaussian radial variation of the electric field. We find that the most favourable situation to achieve self-pulsing instabilities is that of atomic and cavity detunings with opposite sign. The results are compared with those of plane-wave theory. We show that noise plays a primary role at the onset of self-oscillatory instabilities, and that its effects are governed by an equation formally identical to the Risken equation for the laser.</abstract><cop>London</cop><pub>The Royal Society</pub><doi>10.1098/rsta.1984.0109</doi><tpages>7</tpages></addata></record> |
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subjects | Circles Electric fields Lasers Modeling Optical bistability Optics Quadrants Resonance |
title | Transverse Effects and Noise in Optical Instabilities |
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