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WANG Shan-Peng TAO Xu-Tang DONG Chun-Ming JIAO Zheng-Bo JIANG Min-Hua 《结构化学》2007,26(10):1184-1188
A Bridgman growth furnace was modified by adding adiabatic material between two furnace tubes. The appropriate temperature gradient of 10~30 ℃/cm at the growth interface was obtained by adjusting the distance between the two sections and controlling their temperature. The infrared nonlinear optical (NLO) crystal LiInS2 was successfully grown by the accelerated crucible rotation technique (ACRT). The crystal was characterized by using XRD and transmission microscopy. It is found that the UV-VIS-NIR and Mid-IR transmittances are about 40%. 相似文献
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借助抽运-探测技术研究了ZnTe晶体中光学整流产生的太赫兹(THz)辐射,利用ZnTe晶体的线性电光效应探测THz辐射场分布,观察到了较窄(约为0.2 ps)的THz场分布及相应较宽(响应超过4 THz,半峰宽约为2.4 THz)的THz频谱,并运用琼斯矩阵对实验结果进行了理论拟合. 研究了飞秒激光脉冲波长(750—850 nm)、脉冲宽度(56—225 fs)和晶体旋转与THz辐射产生的关系. 同时改变探测光偏振方向进行偏振调制,并从理论上分析了偏振调制对THz辐射探测的影响.
关键词:
THz辐射
光学整流
电光探测
ZnTe 相似文献
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The influence of nickel dopant on the microstructure and optical properties of SnO2 nano-powders 下载免费PDF全文
The microstructure and optical properties of Ni-doped SnO2 nano-powders are studied in detail. By Ni-doping, not only the grain size reduces, but also the grain shape changes from nano-rods to spherical particles. The crystallization becomes better with annealing temperature increasing. The band gap energy decreases as nickel doping level increases. The sp-d hybridization and alloying effect due to amorphous SnO2-x phase should be responsible for the band gap narrowing effect. Nickel dopant does not change the photoluminescence (PL) peak positions. 相似文献
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MoS2 是钼基加氢精制催化剂 [Co(Ni)Mo/γ Al2 O3]活性相的主要组份 ,其形态与结构对Co(Ni)Mo/γ Al2 O3的加氢脱硫 (HDS)、加氢脱氮 (HDN)活性的影响至关重要[1 ,2 ] .目前 ,人们通常使用的TPR方法虽可测定过渡金属硫化物的表面活性位 ,并可有效地区分位于催化剂活性相 (MoS2 slab)周边的硫物种 ,但对不同价态的钼尚无法鉴别[3] .本文制备了硫化态Mo/γ Al2 O3催化剂 ,以CO为探针分子 ,利用FTIR技术在液氮温度 (77K)下考察了催化剂的表面活性位 (钼物种 )及催化噻吩HDS的活性 .1 实… 相似文献
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硫化态三组元NiMoP/γ-Al2O3催化剂的TPR表征及噻吩HDS活性的研究 总被引:1,自引:0,他引:1
A series of sulfided tertiary NiMoP/γ-Al2O3 catalysts with different contents of MoO3 were prepared by using molybdophosphoric acid of Keggin structure(H3PMo12O40) and nickel nitrate as origins of active phase components of molybdenum, phosphorus and nickel, and characterized by TPR technique, with their HDS activity being investigated with thiophene as a model substrate. For the sulfided Mo-0 catalyst containing no nickel as promoter, the only hydrogen sulfide evolution peak Ⅰ is observed at 462 K and attributed to the hydrogenation of the so-called edge sulfur atoms chemisorbed on coordinatively unsaturated(cus) Mox+ sites on the MoS2 phase(MoS2 slab). With the introduction of nickel into the active phase of the sulfided Mo-0 catalyst and with the increase of the molybdenum loading, a new hydrogen sulfide evolution peak Ⅱ gradually develops at the low temperature side of the peak Ⅰ, at the same time accompanied by both the increase of the area ratio of the peak Ⅱ to the peak Ⅰ and the shift of the hydrogen sulfide evolution maximum rate to lower temperatures, which may imply the existence of two kinds of active centers related to molybdenum and nickel respectively and the synergic action between the two centers above. It should be noted that for the sulfided NiMoP/γ-Al2O3 catalysts, the thiophene HDS rate and the quantity of hydrogen sulfide evolved during TPR process increase monotonously with the atomic ratio of molybdenum to nickel in the form of [n(Ni)+n(Mo)]/n(Ni). On the basis of the results here, the conclusion may be reached that the two kinds of vacancies can be formed on the edge of Ni-Mo-S slab due to the loss of S during TPR process and vacancies or sites related to the H2S evolution peak II should be regarded as the mainly active reaction centers of thiophene HDS. 相似文献
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将多孔硅浸入含贵金属盐的HF溶液20 s, 制备了Ag, Au, Pd和Pt的沉积层. AFM形貌显示, 这4种贵金属都能在多孔硅上直接沉积, 但Pt的沉积量比其他3种少. SEM图及能谱(Energy dispersive X-ray spectrometer, EDS)分析显示, 沉积层优先生长在孔边上, 孔边上的沉积量约是孔底的4.6倍. 电化学方法分析显示, Pd和Pt, Ag和Au的沉积层分别具有类似的开路电位和交流阻抗特性, 其中Pd层的溶出电流比其他3种大1个数量级, 而阻抗比其他小1个数量级, 说明Pd层与硅基底的结合程度好, 结合界面导电性好. 相似文献
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In this paper, we study a two-dimensional piecewise smooth map arising in ecology. Such map, containing two parameters d and β, is derived from a model describing how masting of a mature forest happens and synchronizes. Here d is the energy depletion quantity and β is the coupling strength. Our main results are the following. First, we obtain a “weak” Sharkovskii ordering for the map on its nondiagonal invariant region for a certain set of parameters. In particular, we show that its Sharkovskii ordering is the natural number (resp., the positive even number) for β>1 (resp., 0<β<1). Second, we obtain a region of parameter space for which its corresponding global dynamics can be completely characterized. 相似文献