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To reduce the absorbing non-homogeneration of the gain medium in a single-end high power pump, a double end-pumped fold cavity structure is applied.

为了减少单端高功率泵浦造成的增益介质吸收不均匀性,采用双端泵浦折叠腔结构。

Objective To assess the clinical efficiency of the trilumen single balloon catheter newly designed for percutaneous transvenous mitral commissurotomy.

目的 为评价三腔单球囊导管行经皮二尖瓣分离术的临床疗效。

980Nm VCSEL array was fabricated and the comparison of output power and spectrum of array device with single device of same active area was analyzed.

研制出980nm 垂直腔面发射激光列阵,测试了输出功率和光谱,并与相同出光面积的单管器件进行了比较。

The original two-photon JC model is generalized to the case of degenerate atomic level.

本文研究了双光子JC模型的耗散与退相干,得到了一些不同于单光子过程结论;发现双光子过程中场的相干性无论在质的方面及量的方面都受腔耗散的影响,这是与单光子过程明显不同的。

Hyperfine structures of the R(122) 35-0 and P(84) 33-0 transitions of 127I2 near 532 nm.

用单块激光器和环形外腔获得稳定的532 nm激光。

Diode pumped monolithic nonplanar ring laser has the advantages of compactness, reliability and high efficiency.

激光二极管抽运的单块非平面环形腔固体激光器具有结构稳固、效率高等优点,在一定的纵向磁场作用下,可形成单向行波振荡,纵向抽运时就可得到较高功率的单频输出,有广泛的应用前景。

Based on the ring-shaped laser-diode array side-pumped Nd:YLF high gain amplifier and the conventional plan-concave resonator, a simple structure single-longitudinal-mode single-pulse Q-switched oscillator is demonstrated by taking advantages of mode-selecting property of passive Q-switches (Cr4+:YAG crystal) and etalons (formed by two end of uncoated Nd:YLF rod).

以激光二极管环形阵列侧面抽运Nd:YLF棒高增益放大器模块为基础,在经典的平凹驻波腔中加入一片Cr4+:YAG晶体作为被动Q开关,利用被动Q开关本身所具有的振荡选模功能以及两端不镀膜的Nd:YLF棒所具有的标准具效应,简便地实现了稳定的单脉冲、单纵模调Q输出。

In view of the development about the certain airborne radar antenna array,considering the structural features of antenna array,analyse the cruces in manufacturing of feed cavity and radiant plate,and present the corresponding solution by mainly dealing with precise positioning style,delicate clamp design,error distribution and compensation method,high speed machining technology design,machining simulation and program optimizing.

某机载雷达平面裂缝阵列天线的单面阵如图1所示。该面阵布置多路裂缝线源,共分布384处长度各不相同的辐射裂缝,每一路线源均由脊型波导口单独馈电。面阵由辐射板和馈电腔两个零件组成,采用整体钎焊成形。线源结构为非对称单脊共线形式,即在普通单脊波导的两侧与辐射裂缝相对应的位置上布置不对称的凹台。

Path analysis of nine traits, which were highly correlated with tree volume, showed that the direct contribution of DBH and height on the variations of tree volume took up about 63% of the total variations. On the other hand, those traits, such as tree crown and wall/lumina, affected the volume strongly by indirect way of the genetic correlation with DBH and height.

通过对与材积性状紧密相关的胸径等9个性状的通径分析发现,胸径和树高两个性状对单木材积的直接作用占材积总变异的63%,其余性状的直接控制作用很小;冠幅、壁腔比等性状通过胸径对单木材积具有很大的间接遗传控制作用,这种控制是通过与胸径、树高的遗传相关实现的。

The results show that the increasing weight of tungsten oxide nanopowders and the color of tungsten nanomaterials turns light yellow from dark blue and black by increasing oxygen partial pressure in blown gas; the decreasing weight of tungsten oxide nanopowders and the color of tungsten oxide nanopowders becomes dark blue by the plasma that compares row increase including the hydrogen.The tungsten oxide nanomrods was increasing with chamber pressures. Urged nanoparticles to have the clavate fusion phenomenon in the development process with increasing plasma currents, and increased the nanorods distribution quantity along with the generated time to be more, 12 minutes later presents all nanorods. This system to prepare a monoclinic crystal W18O49 nanorods successfully, each hourly output approximately is 0.33 gram, and monoclinic crystal WO3 tungsten oxide nanoparticles, each hourly output approximately is 5.77 grams, its growth mechanism is Vapor-Solid solidly the physiognomy explanation.

研究结果显示,随著氧分压增加时,氧化钨材料呈现重量增加趋势,其颜色从黑色至深蓝色转为淡黄色;随著电浆气中含氢气比列的增加,氧化钨材料呈现重量减少,其颜色从淡黄色至深蓝色转为黑色;针对於氧化钨奈米棒而言随了腔体压力增加,奈米棒的数量也会随之增加,而电浆电流的提高,促使奈米颗粒在成长过程中有了棒状熔合现象,且随了生成时间的增加奈米棒分布数量越多,直到12分钟后呈现出多是奈米棒;本制程在适当制程条件下成功制备出单斜晶体W18O49奈米棒,每小时产量约为0.33 公克,与单斜晶体WO3氧化钨奈米颗粒,每小时产量约为5.77公克,其成长机制可透过气-固(Vapor-Solid, VS)相法解释。

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