首页 | 本学科首页   官方微博 | 高级检索  
     检索      

周期力调制噪声驱动下单模激光系统的多重随机共振
引用本文:张瑞芳,程庆华,徐大海.周期力调制噪声驱动下单模激光系统的多重随机共振[J].物理学报,2015,64(2):24211-024211.
作者姓名:张瑞芳  程庆华  徐大海
作者单位:1. 长江大学物理与科学技术学院, 荆州 434023;2. 长江大学应用物理与信息技术研究中心, 荆州 434023
基金项目:湖北省高等学校优秀中青年科技创新团队计划项目(批准号: T201204)和湖北省教育厅科学技术研究计划重点项目(批准号: D20121203)资助的课题.
摘    要:在周期力调制噪声驱动下单模激光系统的光强方程中加入调幅波, 用线性化近似方法计算了系统的光强关联函数和输出信噪比, 并对信噪比进行数值计算和分析, 发现低频调制频率Ω、高频载波频率ω和周期力频率Ωλ对系统的输出信噪比有很大的影响. 具体表现为信噪比R 随低频调制频率Ω 的变化过程中出现了多重随机共振和极强的单峰共振, 当Ω << ω 时, 系统出现的是多峰共振, 且随着Ωλ 增加, 共振峰间的距离增大, 峰值位置不变; 当Ωω 时, 输出信噪比R迅速增大, 而Ωλ 的影响被削弱甚至可以忽略, 多峰共振消失; 当Ω = ω 时, 系统出现了极强的单峰共振. 此外, 信噪比随周期力频率的变化呈现振幅减小的多重随机共振, 而随载流频率的变化出现单峰随机共振.

关 键 词:多重随机共振  单峰随机共振  信噪比
收稿时间:2014-05-06

Sto chastic multi-resonance of the single-mo de laser system driven by the noise with p erio dic force mo dulation
Zhang Rui-Fang,Cheng Qing-Hua,Xu Da-Hai.Sto chastic multi-resonance of the single-mo de laser system driven by the noise with p erio dic force mo dulation[J].Acta Physica Sinica,2015,64(2):24211-024211.
Authors:Zhang Rui-Fang  Cheng Qing-Hua  Xu Da-Hai
Institution:1. School of Physics Science and Technology, Yangtze University, Jingzhou 434023, China;2. Research Center for Applied Physics and Information Technology, Yangtze University, Jingzhou 434023, China
Abstract:Using the linear approximation method, we calculate the intensity correlation function and the output signal-tonoise ratio (SNR) by adding a modulated wave to light intensity equation of a single mode laser system driven by the periodic force of modulating noise. Through the numerical calculation and analysis of the SNR, we find that the lowfrequency modulation frequency Ω, the high-frequency carrier frequency ω, and the frequency of periodic force Ωλ have a significant effect on the SNR. In particular, multi-peak stochastic resonances and strong single-peak resonance with low-frequency modulation frequency Ω appear in the SNR. When Ω << ω, the system exhibits multi-peak resonance and the distance between the resonance peaks increases with the increase of Ωλ, but the position of peak is invariant. When Ωω, the output SNR R increases rapidly, the effect of Ωλ becomes weak or negligible, and multi-peak resonance disappears. When Ω = ω, a strong single-peak resonance appears in the system. In addition, the SNR varies with the decrease of amplitude of the multi-peak stochastic resonance, and with the SNR changes with carrier frequency the single-peak stochastic resonance appears in the system.
Keywords:multi-peak stochastic resonance  single-peak stochastic resonance  signal to noise ratio
本文献已被 CNKI 万方数据 等数据库收录!
点击此处可从《物理学报》浏览原始摘要信息
点击此处可从《物理学报》下载免费的PDF全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号