Squeezing in multiphoton absorption with and without a resonator

U. Herzog
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引用次数: 1

Abstract

Squeezing in both intracavity and travelling-wave multiphoton absorption is investigated theoretically for incident intense nearly coherent light. It is shown that after sufficiently strong travelling-wave k-photon absorption (k=2,3...) a squeezed state of the radiation field is reached that is not a minimum uncertainty state. In this state the inphase and quadrature variances of the normalized electric field strength approach the asymptotic values k/(4(2k-1)) and k/4, respectively. With the help of an approximate Heisenberg picture treatment of a continuous mode field travelling through a broad-band k-photon absorber an analytical expression is obtained for the evolution of the squeezing spectrum in dependence on the degree of absorption. For intracavity multiphoton absorption the spectrum of output squeezing is investigated with the help of the usual Langevin equation approach. It turns out that the squeezing bandwidth in intracavity and travelling-wave multiphoton absorption is determined by the cavity bandwidth and the absorber linewidth, respectively.
有和没有谐振器的压缩多光子吸收
从理论上研究了入射强近相干光的腔内压缩和行波多光子吸收。结果表明,在足够强的行波k光子吸收(k=2,3…)后,达到了辐射场的压缩状态,该状态不是最小不确定性状态。在此状态下,归一化电场强度的相位和正交方差分别接近渐近值k/(4(2k-1))和k/4。利用近似海森堡图像处理方法,得到了连续模场穿过宽波段k光子吸收体的压缩光谱随吸收程度的演化解析表达式。对于腔内多光子吸收,利用常用的朗之万方程方法研究了输出压缩谱。结果表明,腔内和行波多光子吸收的压缩带宽分别由腔带宽和吸收线宽决定。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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