960 resultados para Nd-Yag Laser


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橘黄色波段固体激光器在基于荧光探测的生物医学诊断和显示等众多方面有着广泛的实际应用.报道了利用532nm的Nd:YAG倍频激光抽运外置喇曼腔内的硝酸钡晶体,获得高效率的599nm橘黄色喇曼激光的实验结果.对外置喇曼腔实验装置和运转参量进行了优化,喇曼振荡腔由对二阶斯托克斯光有最优化反射率的腔镜构成,对实验中所得到的二阶斯托克斯喇曼激光脉宽压缩及出现双尖峰的现象进行了分析.当抽运光功率达到4.1W时,获得二阶斯托克斯喇曼激光功率为710mW,输出光中心波长为599.38nm,半峰全宽(FWHM)为1.1nm

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利用激光诱导等离子体开关技术,在1064nm的Nd:YAG固体激光器上获得了脉宽4.4~6.4ns的短脉冲激光输出。激光电离空气产生的等离子体开关控制脉冲宽度时,聚焦透镜焦距越短,压缩后的脉宽越窄,但激光能量损耗越大。压缩后的激光脉宽与激光能量近似成双曲线关系。在控制脉宽光路的焦点处放置带孔的Cu薄片可抑制等离子体的扩散,得到了脉宽最短可达4.4ns的激光输出。

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Multi-mode rate equations have been developed to investigate mode competition in high-power acousto-optically Q-switched planar waveguide lasers. The mode competition arises from coupling effects and temporal losses in the transform between guided modes and free-space propagation. Pulse-to-pulse instability and temporal beam distortions are enlarged by mode competition when the laser works in the multi-mode regime. The influence of parasitic oscillation is also discussed. A Nd:YAG planar waveguide laser has been established with a folded hybrid/unstable resonator. A maximum average power of 83 W with a beam propagation factor M-x(2) x M-y(2) = 1.2 x 1.4 is obtained. The theoretical simulation agrees well with the experimental observation. (c) 2006 Elsevier Ltd. All rights reserved.

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我们报道了一种以二极管泵浦的 1.94 μm Tm:YAP激光器为泵浦源,常温下在2.1 μm连续运行的Ho:YAG激光器。最大输出功率1.5 W,相应斜率效率为17.9%,二极管到的转换效率为5.6%。

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The spectroscopic properties of (Y0.92-xLa0.08Ndx)(2)O-3 transparent ceramics were investigated. According to three intensity parameters (Omega(2),Omega(4),Omega(6)) fitted by the Judd-Ofelt theory, the spectroscopic quality parameter (X-Nd), branching ratio (beta(J,J')), and quantum efficiency (eta) of Nd3+ were determined. It was found that X-Nd of the host, owing to the additive La2O3, was decreased from 1.6 to 0.46; thus beta(J,11/2) was increased from 46% to 56.82%. A figure of merit of the specimens was discussed and compared with Nd:YAG transparent ceramic. (c) 2007 Optical Society of America.

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YAG单晶是高功率激光的重要材料,近年来高透明度多晶陶瓷作为激光介质引起人们广泛的注意。YAG陶瓷相对单晶具有易制造大尺寸、掺杂浓度高、易批量生产等优点。在Nd:YAG陶瓷获得长足发展的同时,Yb掺杂的陶瓷也得到了越来越多的关注。Yb:YAG陶瓷与Nd:YAG陶瓷相比具有许多优点:Yb掺杂的激光介质无交叉弛豫振荡和激发态吸收,有较宽的吸收带,较长的荧光寿命及较高的量子效率等。因此,高质量的Yb:YAG陶瓷将是非常理想的高功率激光材料。

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使用脉宽12ns,频率10Hz的1064nm调Q Nd:YAG激光器,研究了高反射膜在重复率激光作用下的损伤的累积效应。实验发现,高反射膜的损伤阈值随辐照脉冲数增加而降低,表现出明显的累积效应。通过对损伤阈值和损伤概率以及辐照次数的统计性研究.并结合单脉冲辐照的结果,说明了存在于薄膜中微小的缺陷参与了多脉冲激光对薄膜的损伤过程。可用预损伤机制解释实验结果。得到了关于IBS制备的高反射膜的损伤阈值和照射次数的关系式,并用实验结果进行验证.发现具有很好的一致性。实验过程中样品的损伤形貌通过Nomarski偏光

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研究了高反射膜在多脉冲激光作用下损伤的累积效应.实验中使用1064nm调Q的Nd:YAG激光器,脉宽是12ns,频率为10Hz.实验发现:高反射膜的损伤阈值随辐照脉冲数增加而降低,表现出明显的累积效应.通过对损伤阈值和损伤概率以及辐照次数的统计性研究,并结合单脉冲辐照的结果,说明了存在于薄膜中微小的缺陷参与了多脉冲激光对薄膜的损伤过程,得到了制备IBS高反射膜的损伤闽值和照射次数的关系式,用Nomarski偏光显微镜观察了实验过程中样品的损伤形貌,发现是典型的缺陷损伤.

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以1030nm高反.940。980nm高透的波长分离膜作为实例,为提高该薄膜元件的波长分离效果,从膜系的优化方面做了一系列的研究。诸如采用带通滤光片的设计思想,在膜堆两侧加入了匹配层,调整膜堆的周期厚度,并用膜系设计软件对通带作进一步的优化。通过这一系列的优化设计后.利用RF双离子柬溅射工艺在BK7玻璃基底上沉积样品薄膜,并在基底背面加镀通带增透膜。结果显示,透射带在940和980nm处的透过率分别为97.73%和93.63%.反射带在1030nm的反射率为99.99%。对所制备的样品薄膜进行了激光损伤阈

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利用Nd:YAG调Q单脉冲激光和自由脉冲激光对硬膜窄带干涉滤光片进行激光损伤阈值的测试,并且采用表面热透镜技术测量了滤光片的吸收率。实验发现:窄带干涉滤光片的吸收率和激光损伤阈值强烈依赖于辐照激光波长与窄带干涉滤光片通带的相对位置;在调Q单脉冲激光作用下,不同中心波长的滤光片损伤形貌存在明显的差别,而在自由脉冲激光作用下,各滤光片的损伤形貌则趋于相同.均表现为典型的热熔烧蚀破坏。根据实验结果,结合损伤形貌,通过驻波场理论对激光作用下滤光片内电场分布的分析与模拟.探讨了两种激光模式作用下滤光片的损伤特征和损

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The transient optical nonlinearity of a nematic liquid crystal doped with azo-dye DR19 is examined. The optical reorientation threshold of a 25-mu m-thick planar-aligned sample of 5CB using a 50 ns pulse duration 532 nm YAG laser pulse is observed to decrease from 800 mJ/mm(2) to 0.6 mJ/mm(2) after the addition of 1 vol% azo dopant, a reduction of three orders of magnitude. When using a laser pulse duration of 10 ns, no such effect is observed. Experimental results indicate that the azo dopant molecules undergo photoisomerization from trans-isomer to cis-isomer under exposure to light, and this conformation change reorients the 5CB molecules via intermolecular coupling between guest and host. This guest-host coupling also affects the azo photoisomerization process.

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A low-threshold passively continuous-wave (CW) mode-locked Nd:YVO4 solid-state laser was demonstrated by use of a semiconductor saturable absorber mirror (SESAM). The threshold for continuous-wave mode-locked is relatively low, about 2.15 W. The maximum average output power was 2.12 W and the optical to optical conversion efficiency was about 32%. The pulse width was about 15 ps with the repetition rate of 105 MHz. (C) 2008 Elsevier GmbH. All rights reserved.

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Experimental investigations of nondegenerate ultrabroadband chirped pulse optical parametric amplification have been carried out. The general mathematical expressions for evaluating parametric bandwidth, gain and gain bandwidth for arbitrary three-wave mixing parametric amplifiers are presented. In our experiments, a type-I noncollinear phase-matched optical parametric amplifier based on lithium triborate, which was pumped by a 5-ns second harmonic pulses from a Q-switched Nd:YAG operating at 10 Hz, seeded by a 14-fs Ti:sapphire laser at 800 nm, was presented. The 0.85 nJ energy of input chirped signal pulse with 57-FWHM has been amplified to 3.1 muJ at pump intensity 3 GW/cm(2), the corresponding parametric gain reached 3.6 x 10(3), the 53 nm-FWHM gain spectrum bandwidth of output signal has been obtained. The large gain and broad gain bandwidth, which have been confirmed experimentally, provide great potentials to amplify efficiently the broad bandwidth femtosecond light pulses to generate new extremes in power, intensity, and pulse duration using optical parametric chirped pulse amplifiers pumped by powerful nanosecond systems.

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Stacking chirped pulse optical parametric amplification based on a home-built Yb(3+)-doped mode-locked fiber laser and an all-fiber pulse stacker has been demonstrated. Energic 11 mJ shaped pulses with pulse duration of 2.3 ns and a net total gain of higher than 1.1 x 10(7) at fluctuation less than 2% rms are achieved by optical parametric amplification pumped by a Q-switched Nd:YAG frequency-doubled laser, which provides a simple and efficient amplification scheme for temporally shaped pulses by stacking chirped pulse. (C) 2009 Elsevier B.V. All rights reserved.

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42CrMo合金钢C含量高、合金元素含量多、淬硬倾向大,焊接性能差。激光焊接具有功率密度高、焊接变形小等优点,适合焊接传统工艺难焊的同种或异种金属。通过额定功率为3kW的Nd∶YAG固体激光器焊接42CrMo,采用光学显微镜(OM)、扫描电镜(SEM)、X衍射、硬度仪分析了焊缝区域组织、成分和硬度变化。研究结果表明:焊缝区域组织为马氏体,热影响完全淬火区的组织为马氏体+贝氏体组织,热影响不完全淬火区的组织为贝氏体。从焊缝正面到焊缝背面的硬度分布表明:由于焊缝正面有保护气体的作用提高了焊缝正面熔池的冷却速度,使焊缝背面的硬度低于焊缝正面的硬度。