端面抽运,end-pumped
1)end-pumped端面抽运
1.Optical bistability performance of laser-diodeend-pumped Tm,Ho:YLF laser;激光二极管端面抽运Tm,Ho:YLF激光器双稳特性研究
2.Research of End-pumped 4-mirror Folded Cavity Nd∶YVO_4 Laser;端面抽运四镜折叠腔Nd:YVO_4激光器的研究
3.Cavity mode matching analyses ofend-pumped solid-state lasers;端面抽运固体激光器的腔模匹配分析
英文短句/例句
1.Direct Heat Dissipation from Pumped End in Laser Diode End-Pumped Solid-State Lasers端面抽运固体激光器中抽运端面的直接散热
2.An investigation on temperature field and thermal induced distortion of laser diode end pumped Nd:YVO_4;LD端面抽运Nd:YVO_4温度场及热形变分析
3.Study of Temperature Distribution and Deformation of the End-face in End-Pumped DPL端面抽运激光晶体热形变及温度场分布研究
4.A Method for Measuring Thermal Lens Focal Length of End-Pumped Nd:GdVO_4 Crystals一种测量端面抽运Nd-GdVO_4晶体热透镜焦距的方法
5.High-Power Laser Diode End-Pumped Yb:YAG Repeat Frequency Laser高功率激光二极管端面抽运重复频率Yb:YAG激光器
6.High Power Laser Diode Arrays End-Pumped Efficient Coupling System高效大功率激光二极管阵列端面抽运耦合系统
7.Research on Stability of LD Dual-end-pumped Folded Resonator Nd:YVO_4 Master OscillatorLD双端端面抽运Nd：YVO_4折叠腔主振荡器的稳定性研究
8.Simplified Method for Thermal Distortion of End-Pumped Laser Crystal with Circular Cross-Section端面抽运圆截面激光晶体热变形量的简便求解方法
9.Parameter Optimization and Thermal Effect in End-pumped Continuous Wave Tm, Ho: YLF Lasers;端面抽运Tm，Ho：YLF连续激光器参数优化及热效应研究
10.Theoretical Research of an End Pumped Double-clad Fiber Lasers Doped with Quasi Two-energy-level Ions;端面抽运准二能级双包层光纤激光器的理论探讨
11.Output Characteristics of LD End-pumping Nd∶YVO_4 Laser with Pulse Repetition Rates up to 1 kHzLD端面抽运1KHz电光调Q Nd∶YVO_4激光器输出功率特性研究
12.Thermal Effect of LD End-pumped Nd∶KGW LaserLD端面抽运Nd∶KGW激光器热效应的理论与实验研究
pact LD end-pumped Nd:YAG intracavity frequency-tripled quasi-continuous 355 nm laser紧凑型LD端面抽运Nd:YAG内腔三倍频准连续355nm紫外激光器
14.Room Temperature Efficient Continuous Wave Laser Diode-End-Pumped Tm:YAP Laser室温下高效率连续波激光二极管端面抽运Tm:YAP激光器
15.Thermal Effect of LD End-Pumped Laser Crystal Rods Based on Convective Heat-Transfer about Side Surface基于边界对流传热的LD端面抽运圆柱形晶体的热效应
16.Theoretical Analysis of Temperature and Stress Distribution in End-Pumped Composite Ceramic Nd:YAG Laser Slab端面抽运复合Nd:YAG陶瓷板条激光介质温度和应力分布的理论分析
pact LD End-Pumped Nd:YVO_4 Intracavity Frequency-Tripled 355 nm Laser紧凑型激光二极管端面抽运Nd:YVO_4内腔三倍频355nm紫外激光器
18.Theoretical and experimental investigation of optical bistability in end-pumped Tm,Ho:YLF lasers端面抽运Tm,Ho:YLF激光器双稳特性的理论分析与实验研究
相关短句/例句
end pumped端面抽运
1.A high power high efficiency Nd∶YVO 4 solid state laserend pumped by a fiber coupled diode laser was reported in this paper.报道了一种光纤耦合半导体激光器端面抽运高功率高效Nd:YVO4固体激光器。
2.A few critical rules concerning the design of resonators used for high power laser diodeend pumped CW solid state lasers were presented in this paper.提出了设计高功率半导体激光器（ＬＤ）端面抽运连续固体激光器谐振腔的基本原则。
3.A high power quasi CW diode laser arraysend pumped Nd∶YVO 4 laser is experimentally studied.对高功率准连续激光二极管端面抽运的 Nd:YVO4 固体激光器进行了实验研究。
3)end pump端面抽运
1.A simple Nd∶YVO 4 microchip laser with a plano/plano cavityend pumped by LD is reported.用一种简单方法实现了 LD端面抽运 Nd:YVO4 的平 -平腔微片激光器 ,获得波长为 1。
2.By using a continuous wave, LDend pumped Nd∶YAG laser as a model of the experiment, the noises including intensity noise, frequency noise and field distributing noise of the laser are studied.以连续激光二极管端面抽运NdYAG激光器为实验模型,研究了该激光器中输出激光强度噪声、频率噪声和场分布噪声的特性,并根据实验数据推算出NdYAG晶体的粒子上能级寿命随温度变化为1。
4)LD end-pumpedLD端面抽运
pactLD end-pumped Nd:YAG intracavity frequency-tripled quasi-continuous 355 nm laser紧凑型LD端面抽运Nd:YAG内腔三倍频准连续355nm紫外激光器
5)dual-end-pumped双端端面抽运
1.The design of adual-end-pumped Nd:YVO_4 Z-folded-resonator master oscillator is simulated and the effect of each cavity parameter on the stability of the resonator is analyzed in detail according to the ABCD transfer matrix theory.对双端端面抽运的Nd:YV_4Z型折叠腔主振荡器的设计进行了模拟,采用ABCD传输矩阵理论详细分析了各腔参量对谐振腔稳定性的影响。
6)partially end-pumped部分端面抽运
1.Experimental study ofpartially end-pumped Nd∶YVO_4 slab laser with hybrid resonator operation;部分端面抽运混合腔Nd∶YVO_4板条激光器实验研究
延伸阅读
光学抽运光学抽运Optical pumping光学抽运(optieal pumping)在原子和分子系统中，利用称为抽运辐射的光辐射(即光波波长在可见光谱或近可见光谱内的辐射)使不同能量的选定量子态的热平衡粒子数发生强烈偏差，这种过程称为光学抽运。在温度为TK的热平衡下，分别处在量子化能级E:和El的原子的相对数目NZ/N;可以表示为N:/N，一。一叽一凡’/kT(设E:是较高能级)，式中k是玻耳兹曼常量。热平衡时，处在高能级的原子数目通常要少于处在低能级的原子数目，而且当两能级间的能量差增大时，处在高能级的原子数目实际上将变得非常少。但是，当一个适当的系统受到光辐射的照射时，可以把原子从低能态抽运到高能态，从而使处在高能态的原子数目大大增加，超过平衡时的数值。参阅“能级，，(energy level)条。早期应用这一原理时，能级EZ和E，相隔不远，因此热平衡下这两个能级上的原子数目相差不大。曾选择有第三个能级E3的系统，当系统吸收单色可见光时可从能级El升到能级E3，而不是从能级凡升到能级E3(所涉及的能态是原子能态的顺磁塞曼分量，适当选择单色可见光的偏振态便可保证这种光激发的跃迁所需的选择性)。单色可见光把原子从能级凡激发到E3，随着自发发射，原子再从凡以大约相等的概率返回低能态E:和El。在一个时间周期之后，如果系统受到可见光足够强烈的激发，大多数原子便都处在能态及，而只有少数原子处在低能态E、，亦即原子通过高激发态E3从El抽运到了刃2。参阅“原子结构和光谱”(atomie strueture and、peetra)、“塞曼效应”(Zeeman effeet)条。有一类重要的激光器，是利用受激发射来实现光放大的，在这里光学抽运是不可缺少的。例如，红宝石激光器的作用涉及从激发能级E:跃迁到基能级E，的红光荧光发射。在这种情况下.E:相对来说比E:高，E:的平衡粒子数实际上为零。利用激光器来实现红光的放大要求N:超过N:(粒子数反转)。这种反转可以利用发自一个外部光源的强烈的绿光和紫光把红宝石中的铬离子激发到E:上面的一个能级它:而得到实现。离子无辐射地从E3迅速落到E:，对于激发态来说，在E:上它的寿命是较长的。因此，足够强的抽运便可使发光离子经由能级E3落在E:的数目多于留在基态E，的数目，这样便可利用受激发射实现红宝石红光发射的放大。参阅“激光器”(loser)条。匡韦斯特(W.West)撰]
