共查询到16条相似文献,搜索用时 62 毫秒
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介绍了用于保护HL-2A装置远红外激光干涉仪探测器的双色滤波器。根据双色滤波器理论优化设计了双色滤波器的外型和结构,并首次用于HL-2A远红外激光干涉仪密度测量系统。实验结果表明,当双色滤波器长度l=0.2mm,直径d=0.23mm,孔之间的间隔s=0.33mm时,双色滤波器能够很好地隔离68GHz的ECRH波带来的干扰,并对890GHz的HCN激光波有较好的透过率。 相似文献
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介绍了用激光干涉法测定测量等离子体电子密度的原理,研究了HCN激光器及其输出模式和传输特性,并给出七道远红HCN激光干涉仪的改进及其最新结果,在光路改进中解决了原光路的一些重要问题,使信号提高了近一个量级。 相似文献
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测等离子体电子密度用的远红外HCN激光干涉仪 总被引:1,自引:1,他引:0
等离子体电子密度是等离子体的最重要参数之一。Tokamak型磁约束随着Tokamak型装置等离子体电子密度的提高,给微波干涉测量增加了困难,因为电磁波只能穿过电子密度小于截止密度n_0的等离子体。即 相似文献
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利用EAST装置单道远红外HCN激光干涉仪测量了等离子体中心道(R=1.82m)线平均电子密度。通过充气加料连续提升主等离子体密度,首次在EAST装置上观察到偏滤器等离子体的三种不同状态:低再循环(偏滤器靶板处等离子体温度较高,密度较低),高再循环(偏滤器靶板处等离子体温度较低,密度较高)和脱靶(偏滤器靶板处等离子体温度和密度都很低)等离子体状态。分析了EAST偏滤器在这三种不同状态下的物理现象。 相似文献
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一种处理远红外激光干涉仪相移信号的新方法 总被引:2,自引:2,他引:0
一、引言 在等离子体物理实验中,电子密度的获取十分重要。对于中小型托卡马克装置,其密度范围正好在HCN远红外激光干涉仪(波长337μm)的可测范围,国内外许多装置都用HCN激光干涉仪来测其电子密度n_e。测量来自于干涉仪的两路信号—探测信号V_D和参考信号V_R之间的相位差即可得到n_e。密度相移信号的产生及与n_e的对应关系、传统测量相位差的方法已有专文叙述。传统处理方法由于存在相移过2π时计数值的跳变问题,在密度起伏较频繁 相似文献
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测量托卡马克装置等离子体电子密度分布的远红外HCN激光干涉仪 总被引:5,自引:1,他引:4
本文介绍了用电磁波干涉的方法测量等离子体电子密度的原理、七道远红外HON激光干涉仪的结构及其在HT-6M托卡马克(TOKAMAK)装置上的测量结果.干涉仪的光源县一台腔长3.4m的连续辉光放电的HCN激光器,波长337μm;输出功率约100mW.干涉仪可以给出七道弦上的平均电子密度,最小可测相移为115条纹,时间分辨为0.1ms.也可以由七道弦上相移的线积分值通过非对称的Abel变换给出不同时刻的电子密度的空间分布或时-空分布的三维图形. 相似文献
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七道远红外HCN激光干涉仪的数据处理和实验结果 总被引:1,自引:1,他引:0
本文用非对称Abel变换,研制了一套计算机程序,对七道远红外HCN激光干涉仪测量的信号进行数据处理,并在HT-6M托卡马克中获得了等离子体电子密度时空分布的实验结果。 相似文献
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<正> 科研工作中常用到各种平行度很高的光学件,例如研究激光频率用的法卜里——珀洛标准具必须具有二十分之一波长的平行度。因此,如何在加工过程中方便准确地测量光学件的微小楔角乃是光学工艺经常需要解决的一个问题。目前,在光学加工中激光平面干涉仪用得比较普遍,通常用等厚干涉法,即通过测量工件自身两个表面产生的等厚干涉条纹的宽度而求出光学零件平行度的方法。下表给出了λ=0.6328微米时在玻璃平板(n=1.5)和空气平板(n=1)中的楔角θ与条纹宽度B的对应数值。 相似文献
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利用EAST装置单道远红外HCN激光干涉仪测量了等离子体中心道(R=1.82m)线平均电子密度。通过充气加料连续提升主等离子体密度,首次在EAST装置上观察到偏滤器等离子体的三种不同状态:低再循环(偏滤器靶板处等离子体温度较高,密度较低),高再循环(偏滤器靶板处等离子体温度较低,密度较高)和脱靶(偏滤器靶板处等离子体温度和密度都很低)等离子体状态。分析了EAST偏滤器在这三种不同状态下的物理现象。 相似文献
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Jerald R. Izatt Bimal K. Deka 《International Journal of Infrared and Millimeter Waves》1984,5(11):1473-1482
Using the isotopic species13CH3F in the methyl-fluoride Raman laser, we have observed kilowatt-level laser pulses which can be tuned over a series of intervals that are centered on pure-rotational transitions in thev
3 ground state with initial-state J values between 35 and 43, inclusively. Taken together, these tuning intervals cover 35% of the spectrum between 142 and 174 m. Several straightforward improvements in the experimental setup, including the use of isotopically purer13CH3F, should enhance the spectral coverage in this region. 相似文献
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In this paper we investigate the performance of a quasi-analytic synthesis approach for dispersion compensating optical finite impulse response filters. It is shown by eye opening penalty and optical signal to noise ratio penalty calculations that with this method the filters dispersion can be adjusted reliably and with low effort to compensate for a specific amount of residual chromatic dispersion in optical transmission systems. The maximum attainable dispersion is then only limited by the filter order and the free spectral range rather then by optimization problems within the filter design. 相似文献
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D. K. Mansfield L. C. Johnson A. Mendelsohn 《International Journal of Infrared and Millimeter Waves》1980,1(4):631-640
A modulated far-infrared laser interferometer which is presently operating on the PDX experiment at Princeton is described. The interferometer geometry permits the characterization of inside D, outside D as well as circular discharges. To achieve this versatility, a titanium corner cube reflector, mounted inside the PDX vacuum vessel is used in conjunction with a second visible wavelength interferometer for vibration corrections. In addition, the use of room temperature quasi-optical Schottky diodes in the far-infrared interferometer is reported. The minimum detectable line average density of the system is 5×1011 cm–3. 相似文献
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A method is proposed to solve the problem of direction discrimination for laser feedback interferometers.By vibrating the feedback mirror with a small-amplitude and high-frequency sine wave,laser intensity is modulated accordingly.The modulation amplitude can be extracted using a phase sensitive detector(PSD).When the feedback mirror moves,the PSD output shows a quasi-sine waveform similar to a laser intensity interference fringe but with a phase difference of approximately ±π/2.If the movement direction of the feedback mirror changes,the phase difference sign reverses.Therefore,the laser feedback interferometer offers a potential application in displacement measurement with a resolution of 1/8 wavelength and in-time direction discrimination.Without using optical components such as polarization beam splitters and wave plates,the interferometer is very simple,easy to align,and less costly. 相似文献