TEA CO2激光器几种放电电极的比较

 从均匀场电极理论出发，计算并讨论了近似Rogowski电极、Chang电极(含紧凑式Chang电极)和Ernst电极的形状、理论电场分布和实际电场分布。对实验室所用的几种电极进行了脉冲放电实验，从而获得了TEA CO₂激光器的放电参数与输出特性，并对这些结果进行了比较和分析。计算表明，在基本参数相同的情况下，Ernst电极具有最紧凑的外形和最佳的均匀电场分布。实验表明，采用近似Rogowski电极的TEA CO₂激光器具有最大放电辉光范围和44 kV的最小放电击穿电压；采用Ernst电极的TEA CO₂激光器具有25 J的最高单脉冲能量和最大17.2%的斜率效率。最后提出了TEA CO₂激光器主电极的选择建议。     

TEA CO2激光器不同放电电路放电过程的比较

 利用像增强CCD相机对脉冲CO₂激光器的放电区进行观测,获得了放电辉光的发展过程,由此研究了长脉冲放电电路和短脉冲放电电路对放电过程的影响。发现普通电容放电电路（长脉冲放电电路）存在与自持放电阶段相对应的二次辉光;采用磁压缩开关的短脉冲放电电路,预电离出现较晚,但预电离辉光峰值和主放电辉光峰值之间间距较短,不存在自持放电阶段,只观测到一次强辉光。长脉冲放电电路与短脉冲放电电路在放电的后期均存在一个阴极位降区形成的过程。短脉冲放电电路有利于产生更窄的脉宽和更高的峰值功率。     

紫外预电离TEA CO2激光器放电特性的实验研究

 横向激励大气压（transversely excited atmospheric,TEA）CO₂激光器的放电稳定性是决定该类型激光器应用效果的关键因素。通过对采用电感充放电电路的紫外预电离激光器的实验研究，得到了激光器放电动态过程的规律，并发现残余振荡是主放电后发生弧光放电的主要原因。实验中采用不同配比的气体，并对电感充放电电路与改进后的硅堆充放电电路进行了比较。实验结果表明：增加充电电感值可以降低主放电结束后储能电容上的残余电压；而采用硅堆放电电路在主放电后仅有相对幅值很低的稳定残压，两种方案都大幅度抑制了弧光放电的形成，有效地提高了激光单脉冲能量。     

基于遗传算法的CO2激光器三气体组份优化

应用遗传算法和数值求解CO₂激光动力学方程,以输出激光功率为目标函数,优化了典型封离型CO₂激光器三种主要工作气体(CO₂、N₂、He)的气体压强.对1.2m长谐振腔,在放电电压15kV条件下,三种气体的优化压强分别为PCO₂=1.15×133.3Pa、PN₂=7.36×133.3Pa、PH₂=13.33×133.3Pa.优化后激光功率可提高0.96倍.     

TEA CO2激光器序列带的输出特性

 采用双光栅谐振腔和增长放电增益区,进行了TEA CO₂激光器弱线输出特性研究。在CO₂,N₂,He气体体积比为0.16∶0.21∶0.63,总压强为57.3 kPa情况下,获得6条11 μm波长附近弱线(序列带和热带)激光输出,谱线脉宽为400 ns左右。研究了011-030带的P19线的输出波形和能量,结果表明：谱线输出能量随光栅中心的位移变化而变化,当光栅中心在放电区中心轴线上时输出最强,最大输出能量达几百mJ。     

CO2激光器五种混合气体压强优化

 应用遗传算法,以输出激光功率为目标函数,优化确定了普通CO₂激光器五种工作气体（CO₂, N₂, He, Xe, H₂）的最佳充气量。对1.2m长谐振腔,在15kV放电条件下,优化的充气量分别为p_CO2=1.15×133.3Pa, p_N2=7.32×133.3Pa, p_He=12.95×133.3Pa, p_Xe=0.36×133.3Pa和p_H2=0.01×133.3Pa。优化后激光功率比未优化前可提高1.27倍。     

气体激光器射频至微波放电激发的某些规律

本文研究了射频至微波激发的Xe和He-Ne原子激光器及CO₂分子激光器,结合各具体激光器的实验结果对其放电物理进行了讨论,提出获得高效率的关键是有效控制放电空间的电子能量,得出了一些有指导意义的结论.     

羟基碳纳米管吸附SF6放电分解组分的DFT计算

本文根据密度泛函理论(density functional theory , DFT), 采用MS分子动力学仿真软件对羟基修饰的单壁碳纳米管(SWNT-OH) 吸附SF₆局部放电分解的四种主要组分SOF₂, SO₂F₂, SO₂和CF₄进行了详细的理论计算, 通过分析气体分子和SWNT-OH的前线轨道, 吸附过程中吸附能、电荷转移量和电子态密度的情况, 以及吸附前后SWNT-OH能隙的变化, 评判了SWNT-OH对气体分子的敏感性和选择性, 给出了SWNT-OH是否可以制备气体传感器检测SF₆局部放电分解组分的理论依据.     

燃烧驱动气动CO2激光器几种液体燃料性能差异的数值模拟

 在甲苯、苯、煤油和乙醇四种不同液体燃料燃烧驱动条件下,对气动CO₂激光器燃烧室的平衡组分、小信号增益沿流场方向的分布及激光器的输出功率进行了数值模拟,计算对比分析了该四种燃料的性能。计算结果表明甲苯是气动CO₂激光器四种燃料中最为理想的燃料。     

特定位点上CO2与(TiO2)n团簇相互作用的第一性原理研究

本文基于密度泛函理论系统地研究了(TiO₂)_n团簇上二氧化碳(CO₂)的吸附和活化性质. 计算结果表明,CO₂更倾向于吸附在(TiO₂)_n团簇的桥氧原子上,形成“化学吸附”碳酸盐络合物. 而CO更倾向于吸附到末端Ti-O的Ti原子上. 发现计算得到的碳酸盐振动频率值与实验获得的结果非常吻合,这表明配合物中CO₂的几何构型与其线性型相比,有微小的弯转. 通过对电子结构、电荷密度、电离势、HOMO-LUMO以及态密度的分析,证实了CO₂与团簇之间的电荷转移以及相互作用. 从预测的能量分布图来看,(TiO₂)_n团簇上的CO₂活化与结构密切有关,相比于块体的TiO₂,CO₂在团簇结构上更易于吸附和活化.     

Self-consistent structure of a dc discharge with a closed hall current in crossed electric and magnetic fields

A dc glow discharge with a closed Hall current in crossed electric and magnetic fields in helium is investigated. It is shown that the main features of an unmagnetized dc discharge [1] (such as the separation of the discharge into a space charge sheath and a quasineutral plasma, the formation of a cathode fall region and a negative glow, the appearance of a region with a reversed electric field producing a potential well for low-energy electrons and resulting in the formation of a Faraday dark space, and the formation of three pronounced groups of electrons in the electron distribution function) are also retained in a discharge in crossed fields. It is found that the sheath length is almost independent of the magnetic field, while the length of the negative glow region decreases appreciably with increasing magnetic field. The measured electron distribution function agrees well with the nonlocal theory, according to which the current in the Faraday dark space is carried by the intermediate electrons that are not trapped in the potential well and the energies of which are lower than the first excitation energy.     

Experimental study of the effect of a longitudinal magnetic field on the cathode parts of a glow discharge in helium

The effect of a longitudinal magnetic field on the electrical and optical properties of negative glow and the Faraday dark space of a glow discharge in helium is experimentally studied at a discharge current J_d=11 mA and a pressure of 100–150 Pa in the discharge chamber. An experimental setup is designed and described. A longitudinal electric field is found to be absent in the region of negative glow and the Faraday dark space in both the presence and the absence of the magnetic field. The magnetic field is shown to decrease the voltage of the glow discharge and to increase the total discharge luminosity and the intensities of some spectral lines by a factor of 10–12. The experimental results are explained.     

应用于光刻领域中的固态紫外激光源的制作

以半导体侧泵钇铝石榴石激光器为泵浦源,采用腔内泵浦两块三硼酸铯晶体,产生满足高功率与高光束质量要求的三倍频355 nm紫外激光.通过使用法拉第旋转器谐振腔优化设计与热效应补偿提高输出光的光束质量,并且使用体光栅作为输出镜,在实现线宽窄化同时保持准相位匹配的高效性能.该光刻用紫外激光源成功地替代准分子激光器,使用在一套大面积亚纳米级投影式光刻系统上,工作时紫外光输出功率为4.37 W,光束质量因子为2.27.     

应用于光刻领域中的固态紫外激光源的制作

以半导体侧泵钇铝石榴石激光器为泵浦源,采用腔内泵浦两块三硼酸铯晶体,产生满足高功率与高光束质量要求的三倍频355 nm紫外激光.通过使用法拉第旋转器谐振腔优化设计与热效应补偿提高输出光的光束质量,并且使用体光栅作为输出镜,在实现线宽窄化同时保持准相位匹配的高效性能.该光刻用紫外激光源成功地替代准分子激光器,使用在一套大面积亚纳米级投影式光刻系统上,工作时紫外光输出功率为4.37W,光束质量因子为2.27.     

高性能大口径顺磁旋光玻璃

旋光玻璃广泛用于激光的调制、偏转、开关和高功率激光系统的隔离器.旋光玻璃的主要性质为费尔德常数.含高顺磁离子的旋光玻璃具有大的费尔德常数,可见区高透过等优点.具有较大磁矩和较低f-d跃迁能隙的顺磁离子铽应具有大的费尔德常数.本工作以高Tb2O3含量的Tb2 O3-B2O3-Al2O3-SiO2为基本系统.研究玻璃的形成;测定了不同Tb3+离子浓度时的费尔德常数,符合线性关系;调整玻璃组成以避免析晶,发展了波长632 nm的费尔德常数为75.1～116.4 rad/(T·m)的TG20,TG28,TG32旋光玻璃系列.建立了10升规模铂坩埚高温熔炉,成形和退火设备.形成口径30 cm旋光玻璃的生产能力.产品的1054 nm光吸收小于0.008 cm-1,1 ns的激光破坏阈值大于8 J/cm2,透过波前畸变小于五分之一波长.所制造的旋光玻璃已用于美国Lawrence Livermore国家实验室,中国"神光Ⅱ"升级,英国Rutherford实验室的Vulcan Laser System和CNRS CEA Luli等高功率激光系统.     

半导体激光器混沌法拉第效应控制方法

提出了外腔延时反馈半导体激光器法拉第效应控制下的新激光系统, 构造出两种类型结构光路, 建立了法拉第效应控制下的延时负反馈、延时正反馈激光动力学物理模型, 研究了激光混沌控制与反控制等. 利用法拉第效应原理及磁致旋光性和系统特点, 调节控制光路中的光旋转角度和光延时间可实现双参数控制激光器, 控制激光到双周期、三周期及多周期, 使激光产生拍动等现象, 反控制激光周期到混沌等. 发现了以磁致旋光角分布的激光混沌控制与反控制区域. 并研究了激光混沌控制与周期控制的动态情况, 演示讨论了激光态的转化演变过程等.     

Faraday laser at Rb 1529 nm transition for optical communication systems

We experimentally demonstrate a Faraday laser at Rb 1529 nm transition by using a performance-improved Rb electrodeless-discharge-lamp-based excited-state Faraday anomalous dispersion optical filter as the frequencyselective element. Neither the electrical locking scheme nor the additional frequency-stabilized pump laser are used. The frequency of the external-cavity diode laser is stabilized to the Rb 1529 nm transition, and the Allan deviation of the Faraday laser is measured by converting the optical intensity into frequency. The Faraday laser can be used as a frequency standard in the telecom C band for further research on metrology, microwave photonics, and optical communication systems.     

CO2激光调Q技术

调Q技术是实现小型CO₂激光器短脉冲输出的重要手段,近年来随着短脉冲CO₂激光器在激光测距、测速、成像雷达、环境探测、空间通讯及激光与物质相互作用等领域应用需求的不断增长,激光调Q技术越来越受到国内外专家的关注而成为红外激光技术的研究热点之一。本文就目前用于CO₂激光器中实现短脉冲输出的5种主要调Q技术（机械调Q技术、电光调Q技术、声光调Q技术、被动调Q技术、复合调Q技术）的国内外发展历程和现状进行了综合评述,总结分析了各种方法的关键技术和存在的问题,并简要分析了该技术的未来发展趋势。     

Optical limitation in resonant Faraday media

Optical limitation in resonant Faraday media sandwiched between crossed polarizers is analyzed both theoretically and experimentally. In this technique resonant Faraday rotation permits a net transmission at low intensity levels, whereas the setup transmission is quenched at higher intensities when the active transition is completely saturated. This technique offers many advantages, such as a very low fluence threshold (~12 nJ/cm(2) in cesium vapor), a high intensity range (more than 4 orders of magnitude for polarizer losses of 10(-5)), and quasi invulnerability to optical damage, which make this technique attractive for the protection of fixed-wavelength operated detectors.     

Magnetic Faraday modulation spectroscopy of the 1–0 band of 14NO and 15NO

Magnetic rotation spectroscopy signals of the nitric oxide (NO) fundamental band near 5 μm have been observed and compared with calculated signals. This spectroscopic approach exploits magnetic field modulation in the Faraday configuration for very sensitive detection of NO. Line shapes and strengths of the Faraday signals depend on molecular parameters, like J and Ω quantum numbers of the transitions involved, and on experimental parameters, like pressure of the gas sample and applied external magnetic field strength. In this study we implemented a software model which provides a simulation of the complete v=1–0 Faraday spectrum of NO. The algorithm considers the magnetic field modulation, the collisional and Doppler broadening of the line shapes, and the line intensities of ¹⁴NO and ¹⁵NO fundamental band lines. Optimum values for pressure and magnetic field modulation for maximum sensitivity are given. Suitable spectral windows for simultaneous detection of ¹⁴NO and ¹⁵NO are discussed. Experimental data were obtained in the wavenumber region from 1840 to 1900 cm^?1 by means of a CO sideband laser and a quantum cascade laser. Comparison between calculated and observed signals shows excellent agreement.