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1.
A new approach for improving the efficiency of a copper bromide vapour laser with wavelengths of 510.6 and 578.2 nm is implemented. Multi-factor and regression analyses of a large amount of experimental data have outlined the parameters with highest impact on the laser efficiency. They are electric input power, inside diameter of the rings, distance between the electrodes, inside diameter of the laser tube, hydrogen pressure and electric input power per unit length.The results obtained allow discovery of the internal structure of dependences among parameters, to better account for the physical processes that influence efficiency, to improve the planning of further experiments and laser production technology.  相似文献   

2.
毛邦宁  陈钢  王煜博  陈立  潘佰良 《物理学报》2007,56(5):2652-2656
建立了一个描述纵向脉冲放电的Ne-CuBr紫外激光的动力学模型,数值计算了实验中主要参量对激光性能的影响.给出了激光输出特性随缓冲气压、工作温度和激光管口径之间的变化关系,定量解释了已有的实验结果,为进一步提高激光输出性能提供了依据. 关键词: Ne-CuBr紫外激光 脉冲放电 参量研究  相似文献   

3.
The operation of a CuBr and PbBr2 laser with a two-section gas-discharge tube with working media in different sections and an additional electrode between the sections was studied for the first time. Effective lasing was achieved in both media under control of time location of lasing pulses in different active media. The total mean lasing power equal to 1.5 W was distributed over wavelengths as follows: 1 W (510.6 nm), 0.3 W (578.2 nm), and 0.2 W (722.9 nm). The specific features of operation of the multicomponent laser and methods for its optimization are discussed. It is shown that the lasing power in a section is close to the power of an individual active element.  相似文献   

4.
冯贤平  徐至展 《光学学报》1991,11(9):76-780
本文是在复合泵浦类钠铜软X射线激光系统实验基础上,对该体系的等离子体参数、光谱结构进行测量和分析,给出了类钠铜离子粒子数反转,增益系数与等离子体参数及发射谱结构的内在联系。文中也给出了不同激光功率对各种等离子体参数、光谱结构的影响。  相似文献   

5.
CuBr自锁模激光器的实验研究   总被引:1,自引:1,他引:0  
耿纪宏  张桂燕 《光学学报》1992,12(10):73-878
首次报道在纵向放电的CuBr激光器中,通过抑制高阶横模的振荡,同时得到高度稳定完全调制的绿光和黄光自锁模脉冲串,并在实验上研究了高阶横模,泵浦功率和谐振腔腔长对CuBr激光自锁模脉冲串及其纵模频谱的影响.  相似文献   

6.
The spectral structure of spontaneous emission of copper atom at 510.6 nm and 578.2 nm was calculated considering the hyperfine structure of energy levels and the isotope shift. The spectral structure of the 510.6 nm and 578.2 nm laser lines was measured in a sealed-off CuBr laser tube with periodic refreshment of the neon buffer gas under different work temperature and excited voltage. The spectral structure of the spontaneous emission of copper atom was found to have similar outline with its laser lines. The spectrum of the 510.6 nm laser line maintains similar outline with three peaks at various discharging parameters while the spectrum of the 578.2 nm laser line is strongly dependent on the reservoir temperature and the discharge voltage.  相似文献   

7.
A cataphoresis discharge tube of 7 mm inner diameter and 38 cm active length was designed and made for the He–Sr+ laser. The cataphoretic input of uniform distribution of strontium vapor concentrations along the active region was realized by the cataphoresis effect and the slow flowing (0.5 nl/h) of helium buffer gas. The strontium ionic recombination laser at 430.5 nm and the R–M transition laser at 1.03 μm were obtained with the modified Blumlein circuit by high-frequency longitudinal pulsed discharge. The laser components are concentrated on the 430.5 nm wavelength. Dependences of working parameters such as the pulse frequency, the supply voltage, and the helium pressure on laser output characteristics were measured and discussed. The maximum laser output power of 819 mW and specific power of 56 mW/cm3 were obtained, respectively.  相似文献   

8.
用飞行时间质谱仪和超声速脉冲分子束技术研究了紫外激光对1-萘酚(1HN)团簇的电离质谱.观测到(1HN)_n~+系列的团簇离子,且离子强度随团簇尺寸的增大而减小.电离激光的强度(在5μJ/pulse~100μJ/pulse范围内)对团簇离子强度的相对分布影响较小,说明软电离为产生团簇离子的主要过程,团簇离子的强度分布反映出电离前中性团簇的分布特征.增大电离区的进样气压可以产生更大尺寸的团簇离子,同时在(1HN)_n~+后面观测到新系列的团簇离子.这些新生离子与(H_2O)_m有关,考虑到1-萘酚团簇可以通过OH形成H键,推测该新生团簇离子通过团簇内的反应而产生.  相似文献   

9.
A frequency comb in the UV region with a bandwidth greater than 100 MHz is generated by successive frequency shifts of a single mode laser by an acousto-optic modulator coupled to a passive ring cavity. The obtained spectrum is particularly suitable for laser cooling when a large velocity capture range is required as in the case, for example, of ions confined in a storage ring. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

10.
We show that when polystyrene is exposed (for 15–60 sec) to a UV laser light beam (λ = 248 nm), its absorption and luminescent properties change significantly. In the irradiated polymer, optical centers are formed with absorption bands in the 280–460 nm region and fluorescence bands in the 330–520 nm region. We have established the chemical structure of the optical centers for fluorescence of polystyrene. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 73, No. 1, pp. 54–58, January–February, 2006.  相似文献   

11.
We have established that exposure of polystyrene-based scintillator samples to UV laser radiation (248 nm) leads to a significant decrease in the fluorescence intensity. We have carried out a spectral analysis of the luminescent and absorption properties of the scintillator, which allowed us to determine the major factor in the decrease in luminescence intensity of the samples exposed to UV radiation. We propose a new hypothesis for the mechanism of the processes leading to the decrease in light output of the scintillator during operation. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 74, No. 6, pp. 744–749, November–December, 2007.  相似文献   

12.
 介绍了利用价格便宜的普通视频CCD来获取紫外激光和软X射线图像的方法和应用结果,以代替价格昂贵的紫外CCD、使用不方便的X光胶片或者昂贵的X光CCD,其关键点是:(1)去除CCD相机的自动增益校正;(2)将相机的校正系数γ值设置为1;(3)去除CCD相机前面的保护窗。作为一种简易的装置,可以用于紫外激光测量及激光与等离子体相互作用研究。结果表明,采用改造后的普通视频CCD测量紫外激光光斑,准确可靠,其灵敏度比科学级紫外CCD的低一个量级,它还可以测量软X射线的二维分布,作为X光针孔相机使用非常方便。  相似文献   

13.
本文分析了紫外准分子激光对有机材料的消融过程,用理论模型解释了每个激光脉冲对有机材料的消融量与入射激光能量密度之间的关系.对于有机玻璃.当入射激光能量密度较高时,双光子过程将起主要作用.最后讨论了消融率随有机材料吸收系数之间的关系,对吸收系数较小的材料,消融率随吸收系数改变有一个极大值.  相似文献   

14.
A mathematical model describing the discharge kinetics and lasing characteristics of copper bromide vapor laser with neon and hydrogen additives has been developed. The suggested model is based on a “zero-dimensional” model and offers simple mechanisms to explain discharge kinetics mechanisms, different physical processes and hydrogen additive effects on the copper bromide vapor laser.The model estimates the temporal evolution of discharge voltage and current, population densities, laser beam density, electron temperature and radial distribution of pressure and buffer gas temperature. The suggested mechanism assumes that the electron detachment from negative hydrogen ions does not contribute to the copper ionization process.Numerical solutions of a nonlinear rate equation system predict the generation of nanosecond pulses. The calculated maximum values of discharge voltage, current, average output laser power, electron temperature, etc. are in good agreement with other reported calculated and experimental data.  相似文献   

15.
Indium tin oxide (ITO) thin film is one of the most widely used as transparent conductive electrodes in all forms of flat panel display (FPD) and microelectronic devices. Suspension of already crystalline conductive ITO nanoparticles fully dispersed in alcohol was spun, after modifying with coupling agent, on glass substrates. The low cost, simple and versatile traditional photolithography process without complication of the photoresist layer was used for patterning ITO films. Using of UV light irradiation through mask and direct UV laser beam writing resulted in an accurate linear, sharp edge and very smooth patterns. Irradiated ITO film showed a high transparency (∼85%) in the visible region. The electrical sheet resistance decrease with increasing time of exposure to UV light and UV laser. Only 5 min UV light irradiation is enough to decrease the electrical sheet resistance down to 5 kΩ□.  相似文献   

16.
熔石英紫外激光初始损伤形态分析   总被引:3,自引:2,他引:1       下载免费PDF全文
 采取355 nm激光脉冲辐照熔石英样品,利用Nomarski微分干涉差显微镜、原子力显微镜和扫描电子显微镜观测手段对前后表面产生的损伤点进行了观察分析。对前后表面损伤形态做出详细的描述和分类,从理论上对每种损伤类型产生的条件与机理做出推测。实验结果表明:熔石英前表面存在小麻点群损伤和星状裂纹损伤两种损伤形态,横向尺寸分别为0.8~2.5和1.0~5.5 μm;后表面存在小麻点群损伤、壳状剥离损伤和火山口3种损伤形态,损伤横向尺寸分别为0.48~1.33,4~20和12~30 μm。实验证明了1 μm尺度损伤点的产生与再沉积层密切相关。  相似文献   

17.
An investigation of a He–SrCl2 vapor laser excited by Blumlein discharge circuit is performed. Dependences of laser output power on the working parameters are obtained by experiment. The optimal operating parameters for lasing on several strontium atom and ion lines are found. The multi-line average output power of 1.32 W and the power specific of 12.46 mW/cm3 are achieved, of which more than 78.1% is concentrated at the 6.45 μm laser line.  相似文献   

18.
Propagation of stress waves into polymer substrates undergoing UV laser ablation has been studied by means of laser Doppler vibrometry technique. The measurements acquired far from the ablation point demonstrate oscillations of high amplitude and low decay. For all the studied samples, realized in polystyrene and polymethylmethacrylate of two different molecular weights, ablation generates mechanical excitation of the structure, which propagates all over the bulk as vibrational modes and stress waves.  相似文献   

19.
激光器的打标速度、频率、填充间隔、电流、离焦量等工艺参数直接影响空气开关的打标效果。实验根据5因素4水平正交表L16(45)改变激光工艺参数,利用分光测色计和二维码扫描器对激光标记分别进行色差和读码率的测量,通过正交分析法和极差法研究激光工艺参数对打标效果的影响。研究表明:色差与读码率的数据趋于正比关系,并且存在一个阈值色差;当激光参数的速度为1 000 mm/s、频率为20~30 kHz、填充间隔为0.04 mm、电流为28 A、离焦量为-1 mm时,在空气开关上打标出点密度合适、色差对比度高、易于读取的二维码。  相似文献   

20.
The beam propagation factor, M2 of the master-oscillator power-amplifier (MOPA) CuBr laser emission compliant with ISO 11146 is studied methodically. Statistical parameters of 2D intensity profile of the near and far fields of MOPA laser radiation are measured by a beam analyzing technique as functions of timing delay between MO and PA. For first time the influence of the gas buffer (causing the radiation profile to change from annular to top-hat and Gaussian-like) and light polarization on CuBr laser beam focusability (M2) was under investigation. The MOPA gain curve is found and the influence of gain on the input signal (from MO into PA) due to the absorption/amplification in PA on the field profiles is shown. For annular radiation M2 range is from 13–14 (small delays) to 5–6 (large delays) and for filled-center radiation M2 is 6–7 (small delays) and at the end of gain curve is as much as 4. With polarized light, M2 drops to 3 at the end of gain curve. The brightness of laser emission with hydrogen goes up 3–5 times and the linearly-polarized beam is at least 40% brighter than that of partial or non-polarized beams.  相似文献   

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