期刊文献+

基于四波混频效应实现弱光对强光信噪比优化的研究 被引量:1

The Optimization of SNR of Strong Beams by Weak Beams Based on FWM
原文传递
导出
摘要 我们理论上研究了基于热铷原子系综中的四波混频效应实现信噪比优化的系统。我们分析了非相敏放大器与相敏放大器中信号光信噪比的变化情况。在非相敏放大器中,信号光为相干态注入,闲置光为真空态注入,此时信号光在被放大的同时,信噪比降低,其噪声系数大于1。在相敏放大器中,信号光和闲置光均为相干态注入,此时在特定的条件下,信号光在被放大的同时信噪比得到提高,其噪声系数小于1。在注入光束间的相对相位=2 kπ(k为整数)时,信号光的有效增益最大且噪声系数最小。在这样的相对相位下,只要注入闲置光光强高于注入信号光光强的17.2%时,信号光就能够在被放大的同时信噪比得到提高。特别地,当注入闲置光光强同时低于注入信号光光强时,就实现了弱光对强光信噪比的优化作用。 We reseached a system based on four-wave mixing process in hot rubidium vapor to realize the optimization of signal-to-noise ratio(SNR).We also analyzed the change of SNR of signal beam both in phase-insensitive amplifier(PIA)and phase-sensitive amplifier(PSA).In PIA,the input signal was coherent state and the input idler is vacuum state and we find that the noise figure(NF)of the process was greater than 1,i.e.the SNR of signal beam reduces.In PSA,the input signal and idler were both coherent states and found that the NF of the process was less than 1in some particular areas,i.e.the SNR of signal beam increased in the particular areas.The relative phase between input beams,the ratio of intensity of input signal and input idler,the intensity gain of rubidium cell were represented by,β,G,respectively.We found that when=2 kπ(kis integer),the effective gain of signal beam was maximum and the NF was minimum.Under the condition of=2 kπ(kis integer),as long as the intensity of input idler beam was greater than 17.2% of input signal beam,the SNR of signal beam increasesl in amplification process.Particularly,when the intensity of input idler beam was less than the intensity of input signal beam at the same time,the optimization of SNR of strong beams by weak beams was realized.
出处 《量子光学学报》 北大核心 2016年第3期226-234,共9页 Journal of Quantum Optics
基金 国家自然科学基金(91436211 11374104 10974057) 上海市东方学者研究计划 上海市曙光学者计划(11SG26)
关键词 四波混频 光学放大器 有效增益 信噪比 噪声系数 four-wave mixing optical amplifier effective gain signal-to-noise ratio noise figure
  • 相关文献

参考文献30

  • 1Caves C M.Quantum Limits on Noise in Linear Amplifiers[J].Phys Rev D,1982,26:1817-1839.DOI:10.1103/PhysRevD.26.1817.
  • 2Kolobov M.I.Quantum Imaging[M].Springer,2007.DOI:10.1007/0-387-33988-4.
  • 3Fossier S,Diamanti E,Debuisschert T,et al.Improvement of Continuous-Variable Quantum Key Distribution Systems by Using Optical Preamplifiers[J].J Phys B:At Mol Opt Phys,2009,42(11):114014.DOI:10.1088/0953-4075/42/11/114014.
  • 4Braunstein S L and Loock P v.Quantum Information with Continuous Variables[J].Rev Mod Phys,2005,77:513-577.DOI:10.1103/RevModPhys.77.513.
  • 5Lim O K,Dutton Z,Alon G,et al.Enhanced Optical Resolution in Target Detection with Phase-Sensitive Versus Phase-Insensitive Pre-Amplification[J].Proc SPIE,2011,8163:816306.DOI:10.1117/12.895210.
  • 6Santivanez C A,Guha S,Dutton Z,et al.Quantum Enhanced LIDAR Resolution with Multi-Spatial-Mode Phase Sensitive Amplification[J].Proc SPIE,2011,8163:81630Z.DOI:10.1117/12.903351.
  • 7Levenson J A,Abram I,Rivera Th,et al.Reduction of Quantum Noise in Optical Parametric Amplification[J].J Opt Soc Am B,1993,10:2233-2238.DOI:10.1364/JOSAB.10.002233.
  • 8Tang R,Devgan P S,Grigoryan V S,et al.In-line Phase-Sensitive Amplification of Multi-Channel CW Signals Based on Frequency Nondegenerate Four-Wave-Mixing in Fiber[J].Opt Express,2008,16:9046-9053.DOI:10.1364/OE.16.009046.
  • 9Tong Z,Lundstrom C,Andrekson P A,et al.Towards Ultrasensitive Optical Links Enabled By Low-Noise PhaseSensitive Amplifiers[J].Nat Photonics,2011,5:430-436.DOI:10.1038/nphoton.2011.79.
  • 10McKinstrie C and Radic S.Phase-Sensitive Amplification in a Fiber[J].Opt Express,2004,12:4973-4979.DOI:10.1364/OPEX.12.004973.

同被引文献14

引证文献1

二级引证文献3

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部