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水晶类型: AgGaS2 (Silver Gallium Sulfide) 相位测量类型: Type I 安装: Unmounted 宽度: 5mm 高度: 5mm
AgGaS2(AGS)晶体在0.50-13.2μm范围内是透明的。在Nd:YAG激光泵浦的OPO中,利用AGS晶体在550nm处的高短波长透过率边缘;在大量的DIOD差频混频实验中;覆盖3-12um范围的钛宝石、Nd:YAG和红外染料激光器;用于直接红外对抗系统;AGS晶体也是CO2激光器SHG的一种选择。薄的AgGaS2(AGS)晶体板在通过使用近红外波长脉冲的差频产生中红外范围的超短脉冲产生中很受欢迎。AGS尺寸:标准外尺寸:8x8mm和5x5mm,厚度为1.0-30.0mm
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水晶类型: Cr:YAG AR 涂层: Both sides
Cr4+:YAG在0.9-1.2微米光谱范围内提供了大的吸收截面,这使其成为掺钕激光器被动调Q开关的一个有吸引力的选择。所得到的器件是固态的、紧凑的和低成本的。Cr:YAG具有高损伤阈值、良好的导热性、良好的化学稳定性、抗紫外线辐射,并且易于加工。它正在取代更传统的Q开关材料,比如氟化物和有机染料。所使用的掺杂剂水平在0.5%和3%(摩尔)之间。Cr:YAG可用于工作波长在1000和1200nm之间的激光器的被动调Q,例如基于Nd:YAG、Nd:YLF、Nd:YVO4和Yb:YAG的激光器。Cr:YAG本身也可用作激光增益介质,产生输出在1350和1550nm之间可调的可调谐激光器。Cr:YAG激光器在Nd:YAG激光器的1064nm泵浦下,可以产生飞秒量级的超短脉冲。
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水晶类型: Nd:YAG 水晶直径: 5mm 水晶长度: 50mm AR 涂层: Both sides
Nd:YAG激光晶体L(掺钕钇铝石榴石;Nd:Y3Al5O12)用作固体激光器的激射介质。掺杂物通常约为1%。使用闪光灯或激光二极管对Nd:YAG激光晶体进行光学泵浦。它们是较常见的激光器类型之一,用于许多不同的应用。Nd:YAG激光器通常发射波长为1064 nm的红外光。然而,在940、1120、1320和1440nm附近也存在跃迁。Nd:YAG激光器有脉冲和连续两种工作模式,Nd:YAG主要在730-760nm和790-820nm波段吸收。在低电流密度下,氪闪光灯在这些波段比更常见的氙气灯具有更高的输出,氙气灯在900nm左右产生更多的光。因此,前者对于泵浦Nd:YAG激光器更有效。材料中钕掺杂剂的量根据其用途而变化。对于连续波输出,掺杂显著低于脉冲激光器。轻掺杂的CW棒可以通过较少的颜色(几乎是白色)来光学区分,而较高掺杂的棒是粉红色-紫色的。
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材料: BK7, FS, UVFS, Ge 直径: 25.4mm 高度: 19.0mm 厚度: 10mm 安装: Unmounted
回复反射器是三面体棱镜,通常称为角隅棱镜,该棱镜有三种不同的尺寸(Ø10.0 mm、Ø25.4 mm或Ø50.0 mm)。回射器通过三次全内反射(TIR)将图像或光束反射回其原始方向。即使入射角不为零,光束或图像也将被反转并反射180°。棱镜对准的不敏感性使其成为理想的回射光学器件。对于这些回射棱镜,入射光束和反射光束将按要求在2弧秒至6弧分的范围内平行,然而,除非入射光束和反射光束正好撞击光学元件的中心,否则它们将不会重叠,而是相对于彼此偏移。例如,如果入射光束在中心右侧3mm处撞击光学器件,则回射光束将在中心左侧3mm处射出。此外,回射光束在通过固体回射器传播时,其偏振状态将发生变化。这些棱镜由N-BK7、UV熔融石英、Ge等制成它们可以在入射面上涂有AR涂层,在三个反射面上涂有黑色涂层的金属。
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材料: Calcite, a-BBO 传输波长范围: 400 - 700 nm 最大消光比: Not Available 波前失真: <= Lambda/4 表面质量: 20-10 scratch-dig
Glan Taylor偏振器由两个相同的双折射材料棱镜制成,这两个棱镜由空气间隔隔开。具有侧面逸出窗口的偏振器适用于低到中等功率的应用。Glan Taylor偏振器将入射的非偏振光束分成两束光线,一束是通过另一侧透射的非寻常光,另一束是被全内反射吸收的寻常光。Glan-Taylor偏振器被设计为去除光束的反射普通偏振分量的偏振器元件,大量的反射光通过侧端口离开偏振器,包括所有的普通光线和一些特殊光线。因此,逃逸光束不是完全偏振的,并且只有透射的非常光线应该用于需要高质量偏振光束的应用。它们仅被设计为与良好准直的光束一起工作;会聚和发散的输入光束将不会在内部界面处表现出适当的偏振和入射角。
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镜头类型: Positive 材料: H-K9L 尺寸: 20mm 焦距: 50mm
平凸柱面透镜非常适合需要一维放大的应用。当球面透镜在两个维度上对称地作用于入射光线时,柱面透镜以相同的方式作用,但仅在一个维度上作用。典型的应用是使用一对柱面透镜来提供光束的变形整形。一对正柱面透镜可用于准直和圆化激光二极管的输出。另一种可能的应用是使用单个透镜将发散光束聚焦到检测器阵列上。为了较大限度地减少球面像差的引入,当将准直光聚焦成线时,准直光应入射在曲面上,而当准直时,来自线光源的光应入射在普莱诺表面上。F=R/(n-1),其中n是折射率,R1,R2是透镜每个表面的曲率半径。它们也可以涂有MgF2以保护表面,或者涂有AR涂层以增加透射率。