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We report a new way, i.e. double-end-pumping, to extend the stability range of a laser resonator, in advantage of making the thermal loading be effectively divided between the ends of the laser crystal to reduce the thermal effect, thus to extend the stability range. Using this new way, we experimentally obtained a 2.7-W cw laser source at 671 nm by intracavity frequency doubling of 1342nm ofa Nd:YVO4 laser based on the nonlinear crystal LIB3O5. The maximum pump power is 28 W, which is higher than 13 W of the single-end-pumping. 相似文献
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We demonstrate a passively Q-switched Nd:KLu W laser with a semiconductor sat urable absorber mirror (SESAM) at wavelength 1070 nm. At a pump power of 1.3 W, the pulse width is measured to be about 17ns with repetition rate of lOkHz and with the average output power of 260roW. To our knowledge, this is the first demonstration of Nd:KLuW used for passively Q-switched laser with an SESAM. 相似文献
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为提高聚合物太阳能电池的能量转换效率,将聚乙二醇(PEG)掺入PEDOT:PSS阳极缓冲层,研究了阳极缓冲层修饰对聚合物太阳能电池性能的影响。首先研究了聚乙二醇对PEDOT:PSS薄膜电导率的影响,发现PEG会与PEDOT和PSS相互作用,使得PEDOT链重新排布,有利于电荷载流子的传输,从而显著改善了PEDOT:PSS薄膜的电导率,当PEDOT:PSS中掺入体积分数为2%~4%的PEG时,可得到较大的电导率。然后,以PEG修饰的PEDOT:PSS薄膜作为阳极缓冲层制备了聚合物太阳能电池,研究了PEG的掺入对聚合物太阳能电池性能的影响。实验发现,PEG改善的PEDOT:PSS电导率有利于提高电池的短路电流密度和填充因子,从而改善了器件光伏性能。当PEDOT:PSS中掺入体积分数为2%的PEG时,聚合物太阳能电池的能量转换效率最高,比未掺杂的器件提高了24.4%。 相似文献
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AgX:I微晶的光电子衰减时间分辨谱测量 总被引:1,自引:0,他引:1
利用高时间分辨的微波吸收薄膜介电谱测量技术,采用自行设计的光电子时间分辨谱测量装置(时间分辨率达到1 ns),精确地测量了不同Agx:I材料在35 ps超短脉冲激光曝光后产生的自由光电子和浅俘获光电子随时间衰减的光电子衰减时间分辨谱,分析了不同的[I-]掺杂条件对材料光电子时间特性的影响关系,得到了影响Agx:I微晶光电子时间特性的最佳[I-]掺杂条件。对立方体AgCl乳剂来说,[I-]含量0.5%,掺杂位置80%Ag处时,乳剂的光电子寿命最长。而对T-颗粒AgBr乳剂而言,[I-]含量3%时,乳剂的光电子寿命最长。碘化物对光电子寿命增大的影响是由于碘化物离子可以作为缺陷电子陷阱,这就使得银簇上的反应减小,当碘化物大于3%时,这一效应由于碘化物团簇的形成而消失。 相似文献
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A high power continuous-wave (CW) diode-pumped Nd:YAG laser operated in heat capacity mode is demonstrated by use of two identical highly efficient diode-pumped laser heads placed in a plane-plane resonator.The laser heads are uniformly pumped with a five-fold symmetrical side-pumping configuration, and each head is able to output maximum output power of 2200 W at 808 nm.Under a total pump power of 4290 W,the output power of the laser at 1064 nm is up to 2277 W,corresponding to an optical-to-optical efficiency of 53.1%. 相似文献