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1.
 利用OMA光学多道分析谱仪,分别在激光镜反方向和接近靶面法线方向测量了2倍频谐波的精细结构。在激光功率密度为5×1017 W/cm2的条件下,通过散射光2倍频谐波谱的精细结构,回推出激光与等离子体相互作用中产生的自生磁场达100T量级。  相似文献   

2.
林金龙  王国文 《光子学报》2002,31(4):385-388
报道了Na2+离子的三个低激发态1Σu、2Σg、2Σu在二个光脉冲作用下的解离动量谱,激光波长为680nm,各脉冲功率为1×1012W/cm2,脉宽50fs,从研究结果可见,其单光子、双光子、三光子激发的对应的解离峰及峰值随相对相位而变,并且这种影响随延时增大而减小.  相似文献   

3.
 利用脉冲Nd:YAG激光作用在铝、铜靶上,研究了不同入射激光能量下冲量耦合系数和离焦量之间的关系,以及不同功率密度情况下冲量耦合系数和光斑直径的关系。实验表明铝靶在入射激光脉冲能量由75.8 mJ增加到382.3 mJ时,冲量耦合系数峰值对应的最佳离焦量由-10 mm处远离焦点向透镜方向移到-18 mm,而对应的激光功率密度仅由2.0×109 W/cm2增加到3.9×109 W/cm2;铜靶实验规律和铝靶类似。等离子体屏蔽的吸收作用导致了冲量耦合系数达到最大值后迅速降低。铝靶在入射激光功率密度由0.7×109 W/cm2增大到1.0×1010W/cm2时,冲量耦合系数随光斑直径增大而增大,对应变化斜率由5.2×10-5N·s/(mm·J)增大到49.2×10-5N·s/(mm·J),表明了稀疏波对冲量耦合系数的削弱作用随入射激光功率密度增加而增加,随光斑直径增大而减小。  相似文献   

4.
实验研究了CO2分子在飞秒强激光脉冲作用下的动力学过程,包括分子取向,隧穿电离和库仑爆炸,激光强度从1×1013W/cm2变化到6×1014W/cm2. 当激光强度小于分子的电离阈值时,CO2分子的非绝热转动激发形成一个相干转动波包,波包演化导致分子沿激光电场方向取向. 激光脉冲结束后,分子取向可以周期性地再现,利用另一束激光可以对取向结构进一步进行修饰. 当激光强度大于分子  相似文献   

5.
1 053,527,351 nm倍频分离膜的制备与性能研究   总被引:2,自引:0,他引:2       下载免费PDF全文
 用电子束蒸发及光电极值监控技术在石英基底上沉积了三倍频分离膜,将部分样品置空气中于250 ℃温度下进行3 h热退火处理。然后用Lambda900分光光度计测量了样品的光谱性能;用表面热透镜技术测量了样品的弱吸收值;用调Q脉冲激光装置测试了样品分别在355 nm和1 064 nm的抗激光损伤阈值。实验结果发现,样品的实验光谱性能良好,退火前后其光谱性能几乎没有发生温漂,说明薄膜的温度稳定性好;同时弱吸收平均值从退火前的1.07×10-4下降到退火后的6.2×10-5,从而使对基频的抗激光损伤阈值提高,从14.6 J/cm2上升到18.8 J/cm2,但是三倍频阈值在退火后有显著降低,从7.5 J/cm2下降到2.5 J/cm2。  相似文献   

6.
报道在脉宽50fs—22ps,波长800nm脉冲激光作用下的空气电离阈值的研究结果.利用探测等离子体发光信号的方法,实验测量了激发空气电离所需的阈值激光强度.结果表明,当激光脉冲宽度从50fs增加到22ps时,阈值光强Ith从8.7×1014W/cm2下降到2.7×1013W/cm2Ith经历了由迅速降低逐渐发展为缓慢降低的过程.在50fs—1p  相似文献   

7.
实验研究了1.0×1011—1.0×1017p/cm2通量范围内110keV质子辐照引起的温控涂层热光性能的变化. 实验表明, 在1.0×1011p/cm2通量辐照下6种温控涂层材料的相对光反射率基本没有变化,当辐射通量在1.0×1012—1.0×1016p/cm2范围变化时,某些低吸收率的温控涂层的太阳吸收率随着辐射通量增加先变小而后又增大.这一特性对于制备更低太阳吸收率的温控涂层具有应用价值.  相似文献   

8.
利用侧向阴影照相技术探测靶的飞行速度   总被引:1,自引:0,他引:1       下载免费PDF全文
 建立起一套侧向阴影照相的光学系统,利用可见光作为探测光,在状态方程实验中对靶的飞行速度进行探测。在天光KrF准分子激光装置上进行激光打靶实验,激光波长为248.4 nm。在激光功率密度为8.3×1011 W/cm2的条件下,测得50 μm厚铝靶的飞行速度为3.28 km/s;在激光功率密度为4.7×101011 W/cm2的条件下,测得带100 μm厚烧蚀层的13 μm厚铝靶的飞行速度为2.52 km/s。最后进行了误差分析计算,实验中探测激光与靶表面偏离角度最大不会超过2.06°,偏离角对实验精度产生的影响可以被忽略。  相似文献   

9.
利用兰州重离子加速器(HIRFL)提供的2.79MeV/u Ar离子,在50K以下的低温辐照了Fe47Ni29V2Si6B16等4种非晶态合金样品,室温下使用光学显微镜对辐照前、后的同一样品拍照,对比测量了样品的宏观尺寸. 结果表明:在辐照剂量为1.5×1014离子/cm2时,非晶态合金形变不明显,测量到的样品宽度相对增长Δb/b0均小于1.0%;当辐照剂量增加到1.6×1015离子/cm2时,所有非晶态合金样品都发生了显著的形变,其宽度相对增长分布在4.3%—12.0%之间,对此结果进行了定性的分析.  相似文献   

10.
段国平  陈俊领  韩俊鹤  黄明举 《光子学报》2014,40(11):1657-1661
利用等离子增强化学气相沉积系统制备了本征非晶硅薄膜,并选用488 nm波长的连续激光进行晶化.采用喇曼测试技术对本征非晶硅薄膜在不同激光功率密度和扫描时间下的晶化状态进行了表征,并用514 nm波长与488 nm波长对样品的晶化效果进行了比较.测试结果显示:激光照射时间60 s, 激光功率密度在1.57×105 W/cm2时,能实现非晶硅向多晶硅的转变,在功率密度达到2.7 56×105 W/cm2时,有非晶开始向单晶转变,随着激光功率密度的继续增加,晶化结果仍为单晶;在功率密度为2.362×105 W/cm2下,60 s照射时间晶化效果较好;在功率密度为2.756×105 W/cm2和照射时间为60 s的条件下,用488 nm波长比514 nm波长的激光晶化本征非晶硅薄膜效果较好,并均为单晶态.  相似文献   

11.
We measured the nonlinear susceptibilities of Kr up to fifth order via nonresonant third-harmonic generation (THG) of a frequency-doubled dye laser at 3648 Å. In agreement with theory the optimum intensity conversion efficiency saturates at 10-5 in pure Kr. The phase matching of the third harmonic and fundamental wave breaks up owing to intensity-dependent changes of refractive indices. Phase matching in high-density Kr/Ar mixtures raised the 3648 Å to 1216 Å third harmonic conversion obtained in pure Kr by more than two orders of magnitude, as predicted by theory but hitherto never experimentally confirmed. With laser intensities of 5 × 109 W/cm2 at 3648 Å we measured conversion efficiencies of 1.4 × 10-4 limited by gas breakdown. Taking into account the Lyman alpha absorption of Kr2 and KrAr molecules in the high-density regime, a conversion efficiency of 10-3 is expected from extrapolating the experimental results to Kr/Ar mixtures of up to 3 × 103 torr. It is limited by self-focusing, assuming the minimum threshold intensity of gas breakdown is 1011 W/cm2, as predicted by theory.  相似文献   

12.
Spectral, temporal, and spatial characteristics of harmonics generated at solid surfaces interacting with laser radiation (t=27 ps and I≤1.5×1015 W/cm2) are studied. Spectral broadening and a long-wavelength shift of the second harmonic were observed for laser radiation intensities exceeding 5×1014 W/cm2. Results of the study of the conversion of spectral parameters and polarization features for the generation of second and third harmonics are presented. Conversion efficiencies for the second, third, and fourth harmonic are 2×10?8, 10?10, and 5×10?12, respectively. The results obtained are compared with data of analogous studies utilizing shorter pulses.  相似文献   

13.
We simulate the response of He+ exposed simultaneously to fundamental and 27th harmonic pulses from an intense Ti:sapphire laser. High-order harmonic emission from He+ is enhanced by 17 orders of magnitude compared with the case of the fundamental pulse alone. Moreover, while an individual 10 fs laser with a fundamental wavelength of 800 nm and a peak intensity of 3×1014 W/cm2, or its 27th harmonic pulse with a peak intensity of 1013 W/cm2, ionizes no more than 5×10-6 of He+, their combined pulses lead to a surprisingly high He2+ yield of 17%. The underlying mechanism is either harmonic generation from a coherent superposition of states or two-color frequency mixing, depending on the laser wavelength. PACS 32.80.Rm; 42.50.Hz; 42.65.Ky  相似文献   

14.
The phase-matched collinear third harmonic generation of picosecond laser pulses in a 0.0825 molar hexafluoroisopropanol solution of a pyrimidonecarbocyanine dye is studied. The fundamental pulses are generated in a passively mode-locked Nd-phosphate glass laser. The saturation of third harmonic generation at high intensities is investigated. The influences of two-photon absorption, excited-state absorption, and amplified spontaneous emission are discussed. For input peak intensities above 1011 W/cm2 a third harmonic energy conversion of about 2×10–4 is achieved.  相似文献   

15.
High harmonic generation is compared in the dependence on the ellipticity of the fundamental laser radiation for an atomic and a molecular system. In particular argon and nitrogen are compared employing molecular beams and intense ( 3×1014 W/cm2) and ultrashort (80 fs) 800 nm laser pulses. It turns out that for all the harmonics under investigation (H5, H13 and H21) the harmonic yield decreases slower with the ellipticity for the molecule than for the atom. This indicates differences in atomic and molecular high harmonic generation. Received 24 April 2002 Published online 24 September 2002  相似文献   

16.
The nonequilibrium plasma generated by nanosecond laser pulse is characterized using a SiC detector connected in time-of-flight configuration to measure the radiations emitted from the plasma. Different metallic targets were irradiated by the pulsed laser at an intensity of 1010 W/cm2 and 200 mJ pulse energy. The SiC allows detecting ultraviolet radiations and soft X-rays, electrons, and ions. The obtained plasma has a temperature of the order of tens to hundreds eV depending on the atomic number of the irradiated target and ion accelerations of the order of 100 eV per charge state.  相似文献   

17.
Flux of X-ray radiation emitted from the Ta plasma, produced by the fundamental (1ω) and the third harmonic (3ω) frequencies of the high-power iodine laser PALS, was studied in dependence on the laser focus position. One or two (three) maxima, corresponding to the hard or soft component of the emitted spectrum, can appear, according to the experimental conditions. These dependencies are compared with those published by other authors, and also with our results concerning the highly charged ion generation. At laser intensities above I L~ 1014 W/cm2, the participation of non-linear processes in the pre-formed plasma was confirmed.  相似文献   

18.
The generation of the third harmonic of femtosecond laser radiation with a wavelength of 1.24 μm tightly focused into the bulk of fused silica was simulated numerically for the regime with light intensity of 3 × 1013 W/cm2, which is extreme for solid bodies. The efficiency of third harmonic generation (THG) was found to be restricted to 0.1% in the regime of plasma formation. This is determined by two competitive processes: a decrease of THG efficiency due to an increase of wave detuning and an increase of THG efficiency due to a growth of focusing asymmetry. In an isotropic medium, determination of the threshold of plasma formation by use of the third harmonic signal is shown to be a more sensitive method as compared with the standard scheme of nonlinear transmittance detection.  相似文献   

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