半导体激光自混合干涉类锯齿波成立条件

本文从激光系统稳态条件出发,建立了具有普遍意义的半导体激光自混合干涉系统模型,通过仿真分析,结果表明：在较强光反馈水平时,自混合干涉信号并非都是类锯齿波形。波形形状受光反馈水平及激光器线宽展宽因数的共同制约。本文结果对激光自混合干涉技术的应用具有重要的指导意义。     

仿真分析测量参数对光反馈自混合信号的影响

针对含有光反馈的半导体激光器,在外腔波动条件下,研究其光反馈干涉自混合信号模型。经计算仿真分析,得到了外腔运动参数及激光器本身参数的变化对光反馈自混合信号波形的影响规律。结果表明,利用光反馈自混合干涉效应可以进行多参数传感测量。     

基于经验模态分解的自混合干涉相位提取方法研究

为实现光反馈机理下激光自混合干涉信号相位的精确提取, 本文提出了一种基于经验模态分析(EMD)的方法.首先, 采用EMD算法对含噪的自混合干涉信号进行了降噪预处理, 提取有效的干涉信号.然后在对含有外腔物体运动信息的光反馈相位求解的过程中, 利用希尔伯特黄变换(HHT)原理实时提取每一时刻的瞬时相位, 将其去包裹处理后得到真实相位. 在弱、适度、强光反馈条件下, 分别对基于EMD的相位提取算法进行了仿真研究.最后, 搭建了基于自混合干涉效应的微位移测量实验平台, 进行实验研究.实验结果表明, 利用该方法可以实现对自混合干涉信号的相位提取, 最大误差小于1.6 rad.仿真和实验结果的一致性, 说明了EMD方法的有效性.     

大气颗粒物多参数激光自混合传感的数值模拟与特性分析

基于颗粒物米氏散射特性、激光自混合三镜腔理论和激光器稳态条件,推导出在大气颗粒物光反馈下激光器频率、功率、线宽的理论表达式,建立了大气颗粒物光反馈下的激光自混合理论模型。同时,数值模拟和分析了大气颗粒物物理参数对激光自混合干涉信号的影响。结果表明,在一定粒径范围内,激光自混合反馈强度随大气颗粒物粒径增大先增大后减小,且反馈强度峰值出现的位置随颗粒物折射率实部的增大、虚部的减小向粒径较大处移动;自混合系统的外腔长度影响自混合干涉信号的波动深度,激光器输出光信号的幅值随外腔长度增大呈指数衰减;自混合干涉信号波动频率与大气颗粒物运动速度呈线性关系。分析结果对基于激光自混合效应的大气颗粒物多物理参数传感具有重要作用。     

激光二极管自混合干涉信号随外腔长度衰减

理论分析了激光二极管自混合干涉信号随外腔长度增大的变化特点及规律。从复合谐振腔干涉函数出发,推导出激光二极管自混合干涉信号随外腔长度增加指数衰减,衰减系数与光频虚部成正比,并给出光频虚部和实部满足的超越方程组。求解该超越方程组得到,当外腔长度超过一个临界值时,光频虚部随外腔长度近似反比衰减,则激光二极管自混合干涉信号随外腔长度增加衰减很缓慢;当外腔长度小于该临界值时,外腔反馈会使光频虚部增大,而且光频虚部随外腔长度变化而振荡,激光二极管自混合干涉信号出现复杂的状态。外腔反馈强度越大,或激光单模线宽越大,这一外腔长度的临界值则越小。分析激光二极管自混合干涉还需要考虑外腔反馈对光频虚部的影响。     

差动型激光自混合干涉式位移测量系统

提出了一种利用激光自混合干涉效应的差动式位移测量系统, 建立了系统的数学模型,经仿真分析及实验验证表明： 和单激光管结构相比, 该系统位移分辨力提高了二倍, 达 １／４ 光波波长, 且能大大减小光反馈强度引起的噪声及温度干扰。     

气体激光器

对一般H二Ne激光和频率分裂激光器中偏振态相互垂直的。光和e光的自混合干涉的模式进行了研究,发现了单模变三模的现象,并进行了解释。图6参7(于晓光)TN248.22 2004042529光栅调谐TEAC认激光器理论计算模型二     

光纤激光器自混合干涉效应研究

针对光纤激光器自混合干涉传感应用,研究了光纤激光器自混合干涉特性,运用四镜法布里-珀罗腔模型对掺铒线形腔光纤激光器自混合干涉效应进行了理论分析,对不同反馈水平下的自混合干涉信号进行了数值模拟,获得了光反馈条件下光纤激光器输出特性.外腔长度的改变会调制激光器的输出强度,外腔长度变化半个波长,对应一个干涉条纹,弱反馈条件下,由反馈引起的激光器的频率变化可以忽略.设计了基于光纤激光器的自混合干涉实验,实验结果和理论分析相符合.此研究结果为进一步开展光纤激光器的自混合干涉传感应用研究奠定了理论与实验基础.     

含预反馈的激光自混合干涉型位移测量结构

提出了含预反馈的激光自混合干涉型位移测量结构，建立了系统模型，经理论分析和实验验证，结果表明，该结构具有提高温度量程，提高测量信号信噪比及获得粗糙表面的锯齿干涉信号等特点。     

多纵模激光二极管自混合干涉的观察和分析

自混合干涉信号的幅度和波形均会随外腔静态长度发生周期性变化。实验测量了干涉信号幅度和波形随外腔静态长度的变化,并用多模自混合干涉信号叠加的方法计算分析了干涉信号的幅度随外腔静态长度的变化,然后考虑反馈光对内腔反射率和激光介质增益的影响计算分析了干涉信号的波形随外腔静态长度的变化。结果表明,多模激光自混合干涉信号随外腔静态长度变化的周期为内腔的光学长度,而其主极大区域的宽度为激光的相干长度,小于内腔的光学长度。多纵模自混合干涉信号的叠加导致自混合干涉信号的幅度随外腔静态长度发生周期性变化,而波形随外腔静态长度周期性变化则是内腔反射率和激光介质增益均受反馈光影响导致的非线性的结果。     

Self-mixing interference effect of DFB semiconductor lasers

This paper analyzes the self-mixing interference in DFB (distributed feedback) semiconductor lasers. The general expression of the threshold gain and frequency in the DFB lasers was deduced. Numerical simulations indicate that, for specific coupling coefficient and cavity length value, the DFB lasers are more sensitive to optical feedback than the Fabry–Perot semiconductor laser. These results show that high-accuracy self-mixing sensors can be obtained by using the DFB lasers. PACS 42.55.Px; 42.60.Lh; 42.87.Bg     

Line shapes of near-infrared DFB and VCSEL diode lasers under the influence of system back reflections

Laser diode line widths and line shapes are experimentally investigated in dependence on the diode current and on back reflections from an optical system. Four distributed-feedback (DFB)-type diode lasers and two vertical-cavity surface-emitting lasers (VCSELs) have been tested within the same optical setup and using the same fitting methods. System back reflection ratios of light reflected back to the laser have been varied between ?1?dB and ?45?dB and were below ?60?dB when all reflections were blocked. The background of this investigation is the evaluation of different laser types with respect to their suitability for sensor applications in which optical back reflections may occur, for example tunable diode-laser spectroscopy (TDLS). While DFB-type lasers showed almost pure Lorentzian line shapes and line widths of a few MHz, the tested VCSELs had a strong Gaussian contribution to the line shape, indicating stronger 1/f noise, which was also observed in the relative intensity noise of these particular lasers. System reflection ratios above ?25?dB had strong effects on the line width in both DFB diode lasers and VCSELs, while some influences have been observed at even lower reflection ratios for DFB diode lasers. As much smaller reflection ratios are typically required in TDLS systems to avoid etalon-like fringes and self-mixing interference effects, we conclude that the influence on the line width is not the most important reason to minimize back reflections in practical TDLS systems or to choose one type of diode laser over the other.     

The simulation of self-mixing interference effects in three-section DBR lasers

The self-mixing interference in three-section distributed Bragg reflector (DBR) lasers is analyzed based on the model of F-P cavity and coupling wave equation. The oscillating frequency and threshold variation are deduced. The influence of internal and external parameters on the output intensity and the inclination degree of waveform are discussed in simulation.     

Second-order interference of two independent and tunable single-mode continuous-wave lasers

The second-order temporal interference of two independent single-mode continuous-wave lasers is discussed by employing two-photon interference in Feynman's path integral theory. It is concluded that whether the second-order temporal interference pattern can or cannot be retrieved via two-photon coincidence counting rate is dependent on the resolution time of the detection system and the frequency difference between these two lasers. Two identical and tunable single-mode continuous-wave diode lasers are employed to verify the predictions. These studies are helpful to understand the physics of two-photon interference with photons of different spectra.     

Self-mixing interference effects in tunable diode laser absorption spectroscopy

We report the effects of self-mixing interference on gas detection using tunable diode laser spectroscopy. For very weak feedback, the laser diode output intensity gains a sinusoidal modulation analogous to that caused by low finesse etalons in the optical path. Our experiments show that self-mixing interference can arise from both specular reflections (e.g. cell windows) and diffuse reflections (e.g. Spectralon^™ and retroreflective tape), potentially in a wider range of circumstances than etalon-induced interference. The form and magnitude of the modulation is shown to agree with theory. We have quantified the effect of these spurious signals on methane detection using wavelength modulation spectroscopy and discuss the implications for real gas detectors.     

Self-mixing effect in Yb3+ doped DBR fiber laser with different linewidth enhancement factor

We present a self-mixing interference model approach to stimulate the self-mixing interference in YDBR fiber laser with optical self-mixing interference operating in the weak feedback regime. The self-mixing interference model includes Yb³⁺ doped fibers pumped at 920 nm, with distributed Bragg reflector mirrors at both fiber ends and external reflector. Using the quasi-analytical YDBR fiber laser model and self-mixing three-mirror cavity model, the output power expression is deduced and the Peak-to-Peak values and asymmetry values of self-mixing waveform at different linewidth enhancement factor have been studied in detail.     

光纤耦合自混合干涉测速系统的参数研究

针对光纤耦合自混合干涉测速系统的设计,采用F-P五镜腔模型分析了自混合干涉测速的基本原理,利用数值计算软件MATLAB研究了系统中各个参数对自混合信号波形的影响。对参数引起自混合信号波形“畸变”的情况,进行了参数的优化设计。为光纤耦合自混合测速系统设计,以及将其应用于爆轰波和冲击波研究中进行高速测量提供了参考。     

Self-mixing interference effects in orthogonally polarized dual-frequency Nd:YAG lasers at different feedback levels

The self-mixing interference effects are investigated in birefringence dual-frequency Nd:YAG lasers at different optical feedback levels. For weak feedback level, both of the intensities of the two modes are sinusoidally modulated by external cavity length with a feedback period of half laser wavelength. While these two modes can only coexist in a part of feedback period at moderate feedback level, i.e., one mode reaches its maximum intensity, the other one extinguishes. At high feedback level, complete polarization switching (one mode oscillating, the other one extinguishing) between two polarized modes is observed, and every switching corresponds to quarter-wavelength variation of external cavity length. Furthermore, two feedback schemes, i.e., isotropic optical feedback (IOF) and polarized optical feedback (POF) are taken into account. The theoretical analysis based on a model of two-mode-coupled laser is presented, which is in good agreement with experimental results. Our results can advance the research of self-mixing interferometer of orthogonally polarized dual-frequency lasers.