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    • 1. 发明授权
    • Optical isolator employing multipass faraday rotation
    • 采用多径法拉第旋转的光隔离器
    • US4909612A
    • 1990-03-20
    • US885249
    • 1986-07-14
    • David G. ScerbakJohn DutcherRobert L. MortensenRichard W. WallaceWilliam M. Grossman
    • David G. ScerbakJohn DutcherRobert L. MortensenRichard W. WallaceWilliam M. Grossman
    • G02F1/09
    • G02F1/093
    • An optical Faraday isolator includes a slab of Faraday rotator medium coated to define input and output faces and internal reflective surfaces for causing the beam to travel between the input and output faces along a zig-zag path. Permanent magnets polarized in a direction normal to the plane defined by the zig-zag beam path are disposed on opposite sides of the beam path. The magnets are paired on each side with serially alternating polarity and the like poles are in transverse registration on opposite sides of the beam path to produce an intense, unidirectional magnetic field parallel to the beam path within the rotator slab. A quarterwave plate introduces a compensating amount of elliptical polarization to cancel unwanted elliptical polarization effects of the slab and its coatings. A beam shaving aperture at the exit of the slab shaves off divergent backward travelling rays.
    • 光学法拉第隔离器包括法拉第转子介质的平板,其被涂覆以限定输入和输出面以及内部反射表面,用于使光束沿着之字形路径在输入和输出面之间行进。 在垂直于由锯齿形光束路径限定的平面的方向上极化的永磁体设置在光束路径的相对侧上。 磁体在每一侧配对,具有串联交替的极性,并且类似的磁极在光束路径的相对侧上横向配准,以产生平行于旋转板内的光束路径的强烈的单向磁场。 四分之一波片引入补偿量的椭圆极化以消除板坯及其涂层的不需要的椭圆偏振效应。 在平板出口处的光束剃须孔可以消除发散的反向行进光线。
    • 4. 发明授权
    • Intracavity resonantly enhanced fourth-harmonic generation using uncoated brewster surfaces
    • 使用未涂布的布鲁斯特表面进行腔内共振增强的四次谐波生成
    • US06697391B2
    • 2004-02-24
    • US10113921
    • 2002-03-28
    • William M. GrossmanJeffrey D. Kmetec
    • William M. GrossmanJeffrey D. Kmetec
    • H01S310
    • H01S3/109
    • An optical fourth-harmonic generation system includes a resonant cavity configured to support electromagnetic radiation of a fundamental frequency and a fourth-harmonic generator disposed within the resonant cavity produces electromagnetic radiation of a fourth-harmonic frequency by an interaction with radiation of the fundamental frequency. The fundamental radiation is characterized by a p polarization that is complementary to an s polarization that characterizes the fourth-harmonic radiation. The fourth-harmonic generator has an output facet oriented substantially at a Brewster's angle with respect to the fundamental radiation to separate the fundamental radiation from the fourth-harmonic radiation as they emerge from the output facet.
    • 光学四次谐波发生系统包括构造成支持基频的电磁辐射的谐振腔,并且设置在谐振腔内的第四谐波发生器通过与基频辐射的相互作用产生四次谐波频率的电磁辐射。 基本辐射的特征在于与表征四次谐波辐射的s偏振互补的p偏振。 第四谐波发生器具有相对于基本辐射基本上以布鲁斯特角度定向的输出小面,当基本辐射从输出小面出现时将基本辐射与第四谐波辐射分离。
    • 6. 发明授权
    • Multi-pass light amplifier
    • US5546222A
    • 1996-08-13
    • US79640
    • 1993-06-18
    • Henry PlaessmannWilliam M. GrossmanTodd E. Olson
    • Henry PlaessmannWilliam M. GrossmanTodd E. Olson
    • H01S3/23H01S5/40H01S5/50H01S3/091H01S3/08
    • H01S3/2325H01S3/005H01S3/08068H01S3/09415H01S5/4025H01S5/5018
    • A multiple-pass laser amplifier that uses optical focusing between subsequent passes through a single gain medium so that a reproducibly stable beam size is achieved within the gain region. A resonator or a White Cell cavity is provided, including two or more mirrors (planar or curvilinearly shaped) facing each other along a resonator axis and an optical gain medium positioned on a resonator axis between the mirrors or adjacent to one of the mirrors. In a first embodiment, two curvilinear mirrors, which may include adjacent lenses, are configured so that a light beam passing through the gain medium and incident on the first mirror is reflected by that mirror toward the second mirror in a direction approximately parallel to the resonator axis. A light beam translator, such as an optical flat of transparent material, is positioned to translate this light beam by a controllable amount toward or away from the resonator axis for each pass of the light beam through the translator. A second embodiment uses two curvilinear mirrors and one planar mirror, with a gain medium positioned in the optical path between each curvilinear mirror and the planar mirror. A third embodiment uses two curvilinear mirrors and two planar mirrors, with a gain medium positioned adjacent to a planar mirror. A fourth embodiment uses a curvilinear mirror and three planar mirrors, with a gain medium positioned adjacent to a planar mirror. A fourth embodiment uses four planar mirrors and a focusing lens system, with a gain medium positioned between the four mirrors. A fifth embodiment uses first and second planar mirrors, a focusing lens system and a third mirror that may be planar or curvilinear, with a gain medium positioned adjacent to the third mirror. A sixth embodiment uses two planar mirrors and a curvilinear mirror and a fourth mirror that may be planar or curvilinear, with a gain medium positioned adjacent to the fourth mirror. In a seventh embodiment, first and second mirrors face a third mirror, all curvilinear, in a White Cell configuration, and a gain medium is positioned adjacent to one of the mirrors.
    • 8. 发明授权
    • Multi-pass light amplifier
    • 多通道光放大器
    • US5615043A
    • 1997-03-25
    • US979576
    • 1993-05-07
    • Henry PlaessmannWilliam M. Grossman
    • Henry PlaessmannWilliam M. Grossman
    • H01S3/0941H01S3/23H01S3/081H01S3/0933
    • H01S3/2325H01S3/005H01S3/08068H01S3/09415
    • A multiple-pass laser amplifier that uses optical focusing between subsequent passes through a single gain medium so that a reproducibly stable beam size is achieved within the gain region. A confocal resonator or White Cell resonator is provided, including two or three curvilinearly shaped mirrors facing each other along a resonator axis and an optical gain medium positioned on the resonator axis between the mirrors (confocal resonator) or adjacent to one of the mirrors (White Cell). In a first embodiment, two mirrors, which may include adjacent lenses, are configured so that a light beam passing through the gain medium and incident on the first mirror is reflected by that mirror toward the second mirror in a direction approximately parallel to the resonator axis. A light beam translator, such as an optical flat of transparent material, is positioned to translate this light beam by a controllable amount toward or away from the resonator axis for each pass of the light beam through the translator. The optical gain medium may be solid-state, liquid or gaseous medium and may be pumped longitudinally or transversely. In a second embodiment, first and second mirrors face a third mirror in a White Cell configuration, and the optical gain medium is positioned at or adjacent to one of the mirrors. Defocusing means and optical gain medium cooling means are optionally provided with either embodiment, to controllably defocus the light beam, to cool the optical gain medium and to suppress thermal lensing in the gain medium.
    • 一种多遍激光放大器,其在后续通过单个增益介质之间使用光学聚焦,使得在增益区域内实现可再现的稳定的光束尺寸。 提供共焦共振器或白电池谐振器,包括沿着谐振器轴线彼此面对的两个或三个曲线形状的反射镜和位于反射镜之间的谐振器轴上的光学增益介质(共焦共振器)或与其中一个反射镜相邻(白色 细胞)。 在第一实施例中,可以包括相邻透镜的两个反射镜被配置为使得通过增益介质并且入射在第一反射镜上的入射到第一反射镜的光束被反射镜朝向第二反射镜在大致平行于谐振器轴的方向上反射 。 定位光束平移器,例如透明材料的光学平面,以使光束通过可调量量朝向或远离谐振器轴线移动,以使光束通过翻译器的每次通过。 光学增益介质可以是固态,液态或气态介质,并且可以纵向或横向泵送。 在第二实施例中,第一和第二反射镜面对白色单元配置中的第三反射镜,并且光学增益介质位于或邻近其中一个反射镜。 散焦装置和光学增益介质冷却装置可选地设置有任一实施例,以可控地散焦光束,冷却光学增益介质并抑制增益介质中的热透镜。
    • 9. 发明授权
    • Laser pump control for output power stabilization
    • 激光泵控制输出功率稳定
    • US5226051A
    • 1993-07-06
    • US710288
    • 1991-06-04
    • Melvin ChanHenry G. PlaessmanFrank AdamsWilliam M. Grossman
    • Melvin ChanHenry G. PlaessmanFrank AdamsWilliam M. Grossman
    • H01S3/0941H01S3/11H01S3/131H01S5/042
    • H01S3/115H01S3/0941H01S3/117H01S3/1312H01S5/042
    • Method and apparatus for stabilization of pulse energies produced by a continuously pumped, Q-switched, solid-state or gas laser, through control of the optical power delivered by an optical pump to the laser, in order to limit the energy emitted in any single laser pulse as a result of Q-switching. The laser pump is driven at full strength for a selected initial refresh time t.sub.r. If a Q-switch trigger signal is received by the laser before the elapsed time .DELTA.t has reached the refresh time t.sub.r, the laser emits a pulse with the reduced energy stored in the laser at that time. If the elapsed time reaches or exceeds the refresh time t.sub.r, the optical pump power subsequently delivered to the laser is reduced to a lower level, which may be time-dependent, that is sufficient to maintain the net energy stored in the laser at a predetermined value so that the energy in a subsequently emitted laser pulse does not exceed a selected limit. Numerous techniques for controlling the optical pump power delivered are disclosed.
    • 通过控制由光泵向激光器传递的光功率,通过连续泵浦,Q开关,固态或气体激光器产生的脉冲能量的稳定化方法和装置,以限制在任何单个 激光脉冲作为Q开关的结果。 激光泵以全强度驱动以选择初始刷新时间tr。 如果在经过时间DELTA t达到刷新时间tr之前由激光器接收到Q开关触发信号,那么激光器在那时发射存储在激光器中的能量减少的脉冲。 如果经过的时间达到或超过刷新时间tr,则随后输送到激光器的光泵浦功率被降低到较低的水平,其可能是时间依赖性的,其足以将存储在激光器中的净能量保持在预定的 使得随后发射的激光脉冲中的能量不超过选定的极限。 公开了用于控制递送的光泵功率的许多技术。