共查询到18条相似文献,搜索用时 171 毫秒
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利用光纤飞秒光频梳和外腔可调谐半导体激光器, 建立了一套双频He-Ne激光器频率测量系统. 选用铷钟作为系统的频率基准, 通过将外腔半导体激光锁定至光频梳使得其频率溯源至铷钟, 再利用外腔可调谐半导体激光与双频He-Ne激光器输出的正交偏振激光拍频, 同时测量两路正交偏振激光频率. 将可调谐半导体激光器锁定至光频梳第1894449个梳齿, 其绝对频率为473612190000.0±2.7 kHz, 相对不确定度为5.7×10-12. 对商品双频He-Ne激光器进行频率测量实验, 双频He-Ne激光器水平方向偏振激光频率均值为473612229934 kHz, 竖直方向偏振激光频率均值为473612232111 kHz, 平均时间为1024 s的相对Allan标准差为5.2×10-11, 频差均值为2.177 MHz, 标准偏差为2 kHz. 相似文献
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研究了一种全新的纳米尺度位移测量系统。将双折射元件插入He-Ne激光器谐振腔内产生频率分裂效应,使原本单模谐振的激光器输出变成了频差可调的2个正交偏振频率(o光和e光),而形成双频激光器。在激光谐振腔外放置沿激光轴线位移的反射表面,将输出的激光束反射回腔内,以便对激光的光强进行调制,可实现高分辨率非接触式可判向位移测量。提出了一种细分方法,该方法突破了传统干涉系统的衍射极限(1/2波长)。对于633nm波长He-Ne激光,本系统的理想分辨率为1/8波长(约为79nm)。 相似文献
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激光谐振腔内相位各向异性会引起频率分裂,两分裂模的频差大小由表现出的相位延迟所决定.对于腔内相位延迟较小的He-Ne激光器,两分裂模很接近,处于烧孔重叠区,存在模式竞争而不能同时振荡,形成隐频率分裂.同时,使得激光器两正交偏振方向上的相邻级纵模产生固定的变动量,其大小等于隐频率分裂量的2倍.如果沿激光偏振方向施加横向磁场,Ne原子谱线发生横向Zeeman分裂,增益原子分成两群,分别为平行于磁场和垂直于磁场方向偏振的光提供增益,大大减弱模竞争,使得激光器的两分裂模可同时振荡并测得频差.在谐振腔内放入倾斜的石英晶体片或半波片,由两种方法分别测量频率分裂量并进行比较.实验表明两种方法测量的结果均与理论计算相符,平均相对偏差不超过1%.据此可以准确得到Zeeman双频激光器的频差大小,并为半波片测量提供了新方法. 相似文献
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简要介绍了激光纵模分裂的基本原理,研究了腔内含有1个和2个1/4波片时产生Nd∶YAG激光纵模分裂的规律。实验结果表明:在1064nm Nd∶YAG激光的腔内放置一个1/4波片时,每一激光纵模分裂为2个正交的线偏振模,在波片表面垂直于激光光线的条件下,纵模分裂量(即频率差或波长差)恰好等于激光纵模间隔的一半;当在Nd∶YAG激光腔内沿垂直光线方向平行放置2个1/4波片时,也能产生纵模分裂现象,其纵模分裂量取决于2波片快(慢)轴之间的夹角。在0°~ 90°范围内调节角度,可使纵模分裂量在一个激光纵模间隔内线性调谐。实验结果与理论分析相吻合。 相似文献
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In this letter, a thin slab of glass is used as Fabry–Perot etalon inside a cavity of a continuous wave (CW) Nd:YAG laser to change the behavior of its output longitudinal modes. The slab etalon is used as tuning element when it turns around the laser cavity axis. Two simultaneous longitudinal modes with a relatively wide tuning range from 5.83 MHz to 0.02 THz are obtained when the Nd:YAG laser is operated at moderate output power of about 120 mW. The mode structure of this configuration is modeled and simulated. Computer-generated diagrams are also presented schematically and compared with the experimental results. 相似文献
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Xinrui Xu Rongwei Fan Renpeng Yan Yufei Ma Zhiwei Dong Xudong Li Deying Chen 《Journal of Russian Laser Research》2017,38(5):475-481
We propose a linearly frequency-tuning single-frequency Nd:YVO4 laser. We achieve a single-frequency tuning operation with a tuning range of 6.3 GHz and a maximum power of 0.5 W at 1,064 nm by tilting a thin coated etalon and changing the voltage applied to an RTP crystal in a synchronous way. The laser is linearly tuned with a standard frequency variation of ~190 MHz. We estimate the average tuning speed to be 0.81 GHz/s. The tuning range obtained is more than three times the longitudinal mode spacing of the laser resonator. 相似文献
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1 Introductionace--pumped SOlid-state laser (DPSL) have given rise to an attractive researchinterest and become one of the research focus in the field of laser due to theiradvantageS, such as high efficiency, compactness, steadiness, lOng lifetime and allsolldstate construction. The dual--frequency laser belongs tO the rather complex andadVanced techniqUe. It is applied widely in precise interferometry, laser ranger, laserradar, and heterodyne vibrometry.At present, there are lotS of pape… 相似文献
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Dual-frequency laser resulting from fine detuning twisted-mode cavity is discussed in this paper. Two measurement systems, a Fabry-Perot etalon and a confocal spherical interferometer, are adopted. The former reflects directly the interferogram of multimode and single mode. The latter can judge accurately the mode spectrum of single frequency and dual-frequency laser. Moreover, the experimental results provide the relationship between frequency difference and the angle of the relative rotation of the two quarter-wave plates and agree well with the theoretical analyses. The range of difference frequency is from 50 MHz to 1 GHz. 相似文献
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V.G. Gudelev V.V. Mashko N.K. Nikeenko G.I. Ryabtsev A.B. Stalmashonak L.L. Teplyashin 《Applied physics. B, Lasers and optics》2003,76(3):249-252
Using the mode splitting that can be achieved by exploiting the effect of photoelasticity and the mode selection properties
of coupled resonators, single- and two-frequency operation of a diode pumped cw YAG:Nd3+ laser was observed. In the two-frequency case, a regime with two orthogonal linearly polarized modes was realized. The frequency
difference between the adjacent modes could be varied from 50 MHz to 8.4 GHz. A maximum laser output power of 12 mW was achieved
at a pump level of 240 mW .
Received: 1 November 2002 / Revised version: 14 January 2003 / Published online: 19 March 2003
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ID="*"Corresponding author. Fax: +375-17/2840-879, E-mail: ryabtsev@dragon.bas-net.by 相似文献
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A Brillouin fiber laser (BFL) consisting of a fiber ring resonator with different fiber temperatures emits two-frequency light output. The two-frequency BFL yields an optical beat output which can be utilized as an optical frequency shifter. The output beat frequency is controllable by the temperature difference in the fiber ring resonator and changes with a step of a resonant frequency interval of BFL. The temperature dependence of the BFL output frequency was 2.4 MHz/°C. The stability of the output beat frequency to the temperature fluctuation was estimated as 1.04°C/2.5 MHz. 相似文献
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We report on to our knowledge the first time a diode-side-pumped simultaneous dual-wavelength Nd:YAG laser at 1116 and 1123 nm. By inserting an etalon to balance the gain and loss, a stable dual-wavelength oscillation is acquired. The numerical simulations for wavelength tuning are discussed by principles of laser threshold and Fabry-Perot etalon. Under the pump power of 250 W, a total output power of 23 W is obtained. Meanwhile, the two components have approximately equal intensities. The beam quality of M2 factor was measured to be 7.52. 相似文献