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稀土的发光和激光性能都是由其4f电子在不同能级之间的跃迁产生的。由于稀土离子的独特性能,使得稀土掺杂光功能玻璃无论作为主动还是被动元器件,均在高功率激光系统发挥着重要作用。掺钕磷酸盐激光玻璃和掺铒磷酸盐激光玻璃,具有高稀土离子掺杂浓度、大尺寸和高均匀制备特性,分别是1 um和1.5 um人眼安全波段重频-大能量激光器的重要增益介质材料;光致热折变玻璃及体光栅器件,可实现波长选择和模式选择功能,具有衍射效率高、热稳定性好和抗损伤阈值高等特点,是高功率激光系统中重要的、多功能元器件。文中主要介绍了上海光机所最近几年在掺钕磷酸盐激光玻璃,掺铒磷酸盐激光玻璃以及掺铈的光致热折变玻璃及体光栅器件的研究进展。 相似文献
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N/A 《激光与光电子学进展》1970,7(5):33
美帝休斯飞机公司的研究实验室最近研制了一种叫做氟化铒钙的新合成晶体,它使可见光转换为红外辐射的效率为100%。这种晶体的首要用途是作激光工作物质。据该公司的研究人员说,晶体在紫外光谱波段每吸收一个光子,便在晶体的2微米红外萤光中探测到光子,数目多达五个。由于五个红外光子的能量各为激励萤光的紫外光子的五分之一,所以保存了全部电磁能。效率之所以这样高,是因为晶体的主要成分铒离子与另外两种稀土离子钙和钬(它们取代小部分 铒离子)发生电磁相互作用。红外萤光由钬离子获得,而三种离子的复合吸收光谱则起激励萤光的作用。该公司已在他们最近的激光研究计划中制备了几吋长的氟化铒钙化合物单晶。 相似文献
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本发明涉及一种新型铈激活稀土卤磷酸盐荧光粉及其制备方法;以及使用该材料记录和再现辐射图象的方法和用该材料制做辐射图象存储屏。众所周知,在铈激活稀土卤化物荧光粉中有一种铈激活稀土卤氧化物荧光粉 LnOX 相似文献
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稀土掺杂光子晶体光纤是制作高功率光纤激光器、光纤放大器的理想材料,对稀土掺杂光子晶体光纤的研究尤为重要。提出了一种新型的空气孔八边形双排排列的光子晶体光纤,并对其部分特性进行分析。研究了该种光纤的掺杂纤芯直径、掺杂折射率和波长的变化对有效模场面积和有效折射率的影响,并计算了该稀土掺杂光纤作为光纤放大器时的重叠因子的特性。为以后更好的制作光纤放大器等光器件产生了一定的理论基础。 相似文献
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为了解决铈掺杂稀土卤化物单晶中内部热应力大、难于加工的技术难题,该文提供了一种针对铈掺杂稀土卤化物单晶的原位退火处理方法。利用该方法对尺寸为?25.4 mm×25.4 mm和?76.2 mm×76.2 mm的Ce∶LaBr_3晶体进行退火处理,晶体经过切割、滚圆、研磨、抛光、封装等工艺过程后,均未出现开裂的现象。通过测试以上两种Ce∶LaBr_3器件能量谱图,其能量分辨率分别为2.92%和3.02%,该工艺未对晶体的闪烁性能造成影响。实验结果表明,该文提出的铈掺杂稀土卤化物单晶原位退火处理方法,可有效地消除晶体内部的热应力,并改善其机械性能,这对提高晶体加工成品率具有重要意义。 相似文献
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本文深入研究了KTP晶体在不同磷酸盐助熔剂中的溶解过程、溶解度和晶体生长亚稳区的变化情况.结合溶液成份分析,讨论了各种变化规律和不同磷酸盐助熔剂对KTP晶体生长习性的影响. 相似文献
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研究了预群聚电子束团沿周期性理想金属光栅表面平行移动时产生的史密斯-帕塞尔辐射(SPR).详细分析了电子束团能量、束团群聚长度、具有不同电流密度分布的电子束团以及光栅结构对辐射特性的影响,同时研究了多个群聚束团的辐射.分析发现,电子束团能量增加、束团群聚尺寸变小以及光栅周期变短,辐射能量角分布峰值所对应的频率明显向高频方向移动;光栅周期与电子束团参量相同的条件下,三角形光栅辐射能量角分布峰值所对应的频率明显高于正弦光栅;群聚束团尺寸越小辐射能量越大,并且束团的纵向群聚长度对辐射能量与辐射频率起主要作用.研究结果表明,通过合理选择光栅尺寸与束团参量,可获得工作频率锁定的太赫兹(THz)波段辐射. 相似文献
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Ho3+在氟氧化物玻璃陶瓷中的光谱性质 总被引:5,自引:0,他引:5
根据 Ho掺杂的氟氧化物玻璃陶瓷的吸收光谱,用 Judd-Ofelt理论计算了强度参量,并由此计算了激发能级的自发辐射跃迁速率、辐射寿命、荧光分支比和积分发射截面等光谱参量. 相似文献
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An algorithm based on hyperspectral infrared cloudy radiative transfer model (HIRTM) is introduced and a simulation method for infrared image of the generation geostationary meteorological satellite is proposed. Based on the parameters from weather research and forecast (WRF), such as the water content, atmospheric temperature, and humidity profile, the simulation data for the advanced Himawari imager (AHI) infrared radiative (IR) channels of Himawari-8 are obtained. Simulated results based on HIRTM agree well with the observed data. Further, the movement, development, and change of the cloud are well predicated. And the simulation of IR cloud image for the weather forecast has been obtained. This paper provides an improved method for evaluation and improvement of regional numerical model for weather forecast. 相似文献
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A comparison of clear-air brightness temperatures is performed between radiometric measurements and atmospheric radiative transfer calculations. The measurements were made using the NASA Goddard Space Flight Center's Millimeter-wave Imaging Radiometer (MIR) in a series of airborne and ground-based atmospheric experiments at six millimeter-wave frequencies: 89; 150; 183.3±1, ±3, ±7; and 220 GHz. With the inclusion of the 220 GHz channel, these measurements are the first passive observations of the atmosphere made simultaneously at the six frequencies. The MIR was operated concurrently with supporting meteorological instruments (radiosonde and Raman lidar) to construct a paired set of both spatially and temporally coincident calibrated brightness temperatures and atmospheric profile parameters. Calculated brightness temperatures based on the measured atmospheric profile parameters were obtained using a numerical radiative transfer model. Incremental water-vapor weighting functions were used to study the impact of radiosonde hygrometer errors on the radiative transfer calculations. The aircraft-based brightness temperature comparisons are generally within 3 K for the channels sensitive to the lower atmospheric levels (89, 150, 183.3±7, and 220 GHz), but show discrepancies of up to 11 K for the opaque channels (183.3±1 and ±3 GHz) caused primarily by radiosonde bias. The ground-based calculations are similarly found to be sensitive to hygrometer errors in the lower atmosphere. Ground-based comparisons between MIR observations and lidar-based calculations are typically within ±6 K 相似文献
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基于VLIDORT矢量辐射传输模型,应用灰霾型气溶胶的物理参量,计算了不同条件下的灰霾气溶胶偏振辐射特性,并与常用气溶胶模式下计算的偏振辐射进行分析对比,得到了灰霾气溶胶条件下偏振辐射对于几何位置、气溶胶光学厚度、气溶胶复折射指数、单次反照率、地表参数的敏感性。对于利用偏振辐射实现灰霾气溶胶监测以及气溶胶复折射指数与光学厚度反演提供了理论依据。 相似文献
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Asryan L.V. Grundmann M. Ledentsov N.N. Stier O. Suris R.A. Bimberg D. 《Quantum Electronics, IEEE Journal of》2001,37(3):418-425
The general relationship between the gain and spontaneous emission spectra of a quantum dot (QD) laser is shown to hold for an arbitrary number of radiative transitions and an arbitrary QD-size distribution. The effect of microscopic parameters (the degeneracy factor and the overlap integral for a transition) on the gain is discussed. We calculate the threshold current density and lasing wavelength as a function of losses. The conditions for a smooth or step-like change in the lasing wavelength are described. We have simulated the threshold characteristics of a laser based on self-assembled pyramidal InAs QDs in the GaAs matrix and obtained; a small overlap integral for transitions in the QDs and a large spontaneous radiative lifetime. These are shown to be a possible reason for the low single-layer modal gain, which limits lasing via the ground-state transition for short (several hundreds of micrometers) cavity lengths 相似文献
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Detailed theoretical analysis of the temperature dependence of threshold current density of a semiconductor quantum dot (QD) laser is given. Temperature dependences of the threshold current density components associated with the radiative recombination in QDs and in the optical confinement layer (OCL) are calculated. Violation of the charge neutrality in QDs is shown to give rise to the slight temperature dependence of the current density component associated with the recombination in QD's. The temperature is calculated (as a function of the parameters of the structure) at which the components of threshold current density become equal to each other. Temperature dependences of the optimum surface density of QD's and the optimum thickness of the OCL, minimizing the threshold current density, are obtained. The characteristic temperature of QD laser To is calculated for the first time considering carrier recombination in the OCL (barrier regions) and violation of the charge neutrality in QDs. The inclusion of violation of the charge neutrality is shown to be critical for the correct calculation of To. The characteristic temperature is shown to fall off profoundly with increasing temperature. A drastic decrease in To is shown to occur in passing from temperature conditions wherein the threshold current density is controlled by radiative recombination in QD's to temperature conditions wherein the threshold current density is controlled by radiative recombination in the OCL. The dependences of To on the root mean square of relative QD size fluctuations, total losses, and surface density of QDs are obtained 相似文献