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    • 2. 发明授权
    • External diffusion amplifier
    • 外部扩散放大器
    • US09160136B1
    • 2015-10-13
    • US14292546
    • 2014-05-30
    • LEE LASER, INC.
    • Donald BishopDwight Kimberlin
    • H01S3/00H01S3/23H01S3/0941
    • H01S3/2333H01S3/005H01S3/0064H01S3/025H01S3/061H01S3/0612H01S3/0615H01S3/0617H01S3/0621H01S3/0623H01S3/0941H01S3/09415H01S3/1611H01S3/1673H01S3/2341
    • A first amplification structure uses a single pass external diffusion amplifier wherein the picosecond beam cross-sectional area is matched to the cross-sectional area of the gain medium. A half waveplate between the gain medium and the incoming beam optimizes the polarization of the beam diameter to the polarization of the gain medium. A second amplification structure uses a double pass external diffusion amplifier wherein the beam cross-sectional area is matched to the cross-sectional area of the gain medium and passed twice therethrough. A half waveplate and a rotator create a right circular polarized beam through the gain medium and a maximum “R” coated reflector resides beyond the external diffusion amplifier and reflects a left circular polarized beam back through the gain medium, the rotator and the half waveplate where it becomes horizontally polarized and is then transmitted out of the amplification structure by the polarization sensitive beam splitter.
    • 第一放大结构使用单通道外部扩散放大器,其中皮秒波束横截面面积与增益介质的横截面面积相匹配。 增益介质和入射光束之间的半波片将光束直径的极化优化为增益介质的极化。 第二放大结构使用双通道外部扩散放大器,其中光束横截面积与增益介质的横截面面积相匹配并通过两次。 半波片和旋转器通过增益介质产生右圆偏振光束,并且最大“R”涂层反射器位于外扩散放大器之外,并将左圆偏振光束反射回增益介质,旋转器和半波片 它变得水平偏振,然后通过偏振敏感分束器被发射出放大结构。
    • 5. 发明授权
    • Multipath laser apparatus using a solid-state slab laser rod
    • 使用固态板激光棒的多径激光设备
    • US07515625B2
    • 2009-04-07
    • US11471493
    • 2006-06-21
    • Mitsuo Ishizu
    • Mitsuo Ishizu
    • H01S3/06
    • H01S3/0606H01S3/0615H01S3/0623H01S3/0625H01S3/063H01S3/08095H01S3/093H01S3/1611H01S3/1643H01S3/1653H01S3/2325
    • A laser apparatus has a multipath solid-state slab laser rod and an excitation source that excites it, and uses a solid-state slab laser rod that has a trapezoid or parallelogram-shaped cross section along the optical path, that is provided with six or more faces and that has a light amplifying effect or a nonlinear optical effect. The light that is incident to the laser rod is totally reflected at the incident-light end face and exit end face of the laser rod, passes back through the interior of the laser rod a plurality of times, e.g., three times, and then exits. For light amplification, excitation light is irradiated from the side face. In addition, for nonlinear optical effects, the z-axis of a nonlinear optical crystal is disposed so as to be orthogonal to the plane of the optical path, and the temperature of the solid-state slab laser rod is kept at the phase-matching temperature. This laser apparatus of this configuration solves drawbacks of prior-art laser rods so that the high conversion rate from excitation light to laser light is obtained at a high laser gain.
    • 激光装置具有多径固态板激光棒和激发源,并且使用沿着光路具有梯形或平行四边形横截面的固态平板激光棒,其设有六个或 更多的面孔,具有光放大效果或非线性光学效果。 入射到激光棒的光在激光棒的入射光端面和出射端面处被全反射,多次反复穿过激光棒的内部,例如三次,然后退出 。 对于光放大,从侧面照射激发光。 此外,对于非线性光学效应,非线性光学晶体的z轴被布置成与光路的平面正交,并且固态平板激光棒的温度保持在相位匹配 温度。 这种配置的激光装置解决了现有技术的激光棒的缺点,从而在高激光增益下获得从激发光到激光的高转换率。
    • 7. 发明申请
    • Laser with narrow bandwidth antireflection filter for frequency selection
    • 用于频率选择的具有窄带宽抗反射滤波器的激光器
    • US20060176914A1
    • 2006-08-10
    • US11351682
    • 2006-02-10
    • Gerald BacherDavid Hargis
    • Gerald BacherDavid Hargis
    • H01S3/10
    • H01S3/08059H01S3/0623H01S3/08031H01S3/105H01S3/1062H01S3/109H01S3/1623H01S3/1648H01S3/1658
    • A laser includes a narrow bandwidth AR coating for defining a frequency range for laser emission within the laser cavity. Advantageously, the narrow-band AR coating has a very low loss, which can be particularly useful if the gain medium has low gain. The narrow-band AR coating can be used to narrow the laser emission from a broadband gain medium (e.g. Cr:LiSAF), or to select from among discrete transition lines (e.g. Nd:YAG) without the use of cumbersome tuning elements. An etalon, which may be substantially uncoated, may be utilized to further narrow the fundamental wavelength. For a solid state gain medium, the AR coating may be formed on one of the optical faces. A nonlinear element may be included for frequency-conversion, and the AR coating constrains the lasing frequency in the presence of this nonlinear loss and assists in maintaining single frequency operation to provide a stable frequency-converted output.
    • 激光器包括用于定义激光腔内的激光发射的频率范围的窄带宽AR涂层。 有利地,窄带AR涂层具有非常低的损耗,如果增益介质具有低增益,则其可以是特别有用的。 可以使用窄带AR涂层来缩小来自宽带增益介质(例如Cr:LiSAF)的激光发射,或者不使用繁琐的调谐元件从离散过渡线(例如Nd:YAG)中进行选择。 可以使用基本上未涂覆的标准具来进一步缩小基波长。 对于固态增益介质,可以在其中一个光学面上形成AR涂层。 可以包括用于频率转换的非线性元件,并且AR涂层在存在这种非线性损耗的情况下约束激光频率,并且有助于维持单频操作以提供稳定的频率转换输出。