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    • 1. 发明授权
    • High brightness solid-state laser with zig-zag amplifier
    • 具有锯齿形放大器的高亮度固态激光器
    • US5555254A
    • 1996-09-10
    • US148758
    • 1993-11-05
    • Hagop InjeyanRandall J. St. PierreRodger C. HilyardGeorge M. HarpoleCarolyn S. Hoefer
    • Hagop InjeyanRandall J. St. PierreRodger C. HilyardGeorge M. HarpoleCarolyn S. Hoefer
    • G02F1/35H01S3/04H01S3/042H01S3/06H01S3/08H01S3/0941H01S3/10H01S3/109H01S3/23
    • H01S3/2316H01S3/042H01S3/0606H01S3/0941H01S3/0407H01S3/0621H01S3/0625H01S3/08072H01S3/08095H01S3/10076H01S3/109
    • A solid-state laser architecture producing a beam of extremely high quality and brightness, including a master oscillator operating in conjunction with a zig-zag amplifier, an image relaying telescope and a phase conjugation cell. One embodiment of the laser architecture compensates for birefringence that is thermally induced in the amplifier, but injects linearly polarized light into the phase conjugation cell. Another embodiment injects circularly polarized light into the phase conjugation cell and includes optical components that eliminate birefringence effects arising in a first pass through the amplifier. Optional features permit the use of a frequency doubler assembly to provide output at twice optical frequencies, and an electro-optical switch or Faraday rotator to effect polarization angle rotation if the amplifier material can only be operated at one polarization. The zig-zag amplifier is cooled by flow of cooling liquid, preferably using longitudinal flow to minimize temperature gradients in a vertical direction, and has cooling channel seals disposed in dead zones that receive no light, to minimize optical damage to the seals. Light is input to the amplifier at a near normal angle of incidence, to minimize polarization by reflection and to permit a polarizer to be used to extract an output beam from the amplifier. Antireflective coatings on edges and on sides of the amplifier eliminate parasitic oscillations, and wedge-shaped windows provide uniform pumping by eliminating gaps between diode arrays.
    • 一种固态激光器架构,产生了极高质量和亮度的光束,包括与之前的Zig放大器,图像中继望远镜和相位共轭单元结合操作的主振荡器。 激光器结构的一个实施例补偿了在放大器中热感应的双折射,但是将线偏振光注入到相位共轭单元中。 另一实施例将圆偏振光注入到相位共轭单元中,并且包括消除在第一次通过放大器中产生的双折射效应的光学部件。 可选功能允许使用倍频器组件提供两倍光频率的输出,以及如果放大器材料只能在一个极化下操作,则电光开关或法拉第旋转器可实现偏振角旋转。 锯齿形放大器通过冷却液体的流动来冷却,优选地使用纵向流动以使垂直方向上的温度梯度最小化,并且具有设置在不受光的死区中的冷却通道密封件,以最小化对密封件的光学损伤。 光以接近的正常入射角输入到放大器,以通过反射使偏振最小化,并允许使用偏振器从放大器提取输出光束。 在放大器的边缘和侧面上的抗反射涂层消除了寄生振荡,楔形窗口通过消除二极管阵列之间的间隙来提供均匀的泵浦。
    • 2. 发明授权
    • Solid-state zig-zag slab optical amplifier
    • 固态曲折平板光学放大器
    • US5646773A
    • 1997-07-08
    • US541540
    • 1995-10-10
    • Hagop InjeyanRandall J. St. PierreRodger C. HilyardGeorge M. HarpoleCarolyn S. Hoefer
    • Hagop InjeyanRandall J. St. PierreRodger C. HilyardGeorge M. HarpoleCarolyn S. Hoefer
    • G02F1/35H01S3/04H01S3/042H01S3/06H01S3/08H01S3/0941H01S3/10H01S3/109H01S3/23H01S3/09
    • H01S3/2316H01S3/042H01S3/0606H01S3/0941H01S3/0407H01S3/0621H01S3/0625H01S3/08072H01S3/08095H01S3/10076H01S3/109
    • A solid-state laser architecture producing a beam of extremely high quality and brightness, including a master oscillator operating in conjunction with a zig-zag amplifier, an image relaying telescope and a phase conjugation cell. One embodiment of the laser architecture compensates for birefringence that is thermally induced in the amplifier, but injects linearly polarized light into the phase conjugation cell. Another embodiment injects circularly polarized light into the phase conjugation cell and includes optical components that eliminate birefringence effects arising in a first pass through the amplifier. Optional features permit the use of a frequency doubler assembly to provide output at twice optical frequencies, and an electro-optical switch or Faraday rotator to effect polarization angle rotation if the amplifier material can only be operated at one polarization. The zig-zag amplifier is cooled by flow of cooling liquid, preferably using longitudinal flow to minimize temperature gradients in a vertical direction, and has cooling channel seals disposed in dead zones that receive no light, to minimize optical damage to the seals. Light is input to the amplifier at a near normal angle of incidence, to minimize polarization by reflection and to permit a polarizer to be used to extract an output beam from the amplifier. Antireflective coatings on edges and on sides of the amplifier eliminate parasitic oscillations, and wedge-shaped windows provide uniform pumping by eliminating gaps between diode arrays.
    • 一种固态激光器架构,产生了极高质量和亮度的光束,包括与之前的Zig放大器,图像中继望远镜和相位共轭单元结合操作的主振荡器。 激光器结构的一个实施例补偿了在放大器中热感应的双折射,但是将线偏振光注入到相位共轭单元中。 另一实施例将圆偏振光注入到相位共轭单元中,并且包括消除在第一次通过放大器中产生的双折射效应的光学部件。 可选功能允许使用倍频器组件提供两倍光频率的输出,以及如果放大器材料只能在一个极化下操作,则电光开关或法拉第旋转器可实现偏振角旋转。 锯齿形放大器通过冷却液体的流动来冷却,优选地使用纵向流动以使垂直方向上的温度梯度最小化,并且具有设置在不受光照射的死区中的冷却通道密封件,以最小化对密封件的光学损伤。 光以接近的正常入射角输入到放大器,以通过反射使偏振最小化,并允许使用偏振器从放大器提取输出光束。 在放大器的边缘和侧面上的抗反射涂层消除了寄生振荡,楔形窗口通过消除二极管阵列之间的间隙来提供均匀的泵浦。
    • 4. 发明授权
    • Birefringence compensated laser architecture
    • 双折射补偿激光器架构
    • US5640406A
    • 1997-06-17
    • US415880
    • 1995-04-03
    • Hagop InjeyanRandall J. St. Pierre
    • Hagop InjeyanRandall J. St. Pierre
    • G02F1/35H01S3/04H01S3/042H01S3/06H01S3/08H01S3/0941H01S3/10H01S3/109H01S3/23H01S3/00
    • H01S3/2316H01S3/042H01S3/0606H01S3/0941H01S3/0407H01S3/0621H01S3/0625H01S3/08072H01S3/08095H01S3/10076H01S3/109
    • Apparatus, and a related method, for compensating for birefringence introduced in a birefringent medium, such as a solid-state amplifier. The invention includes the combination of a quarter-wave plate, a Faraday rotator and a mirror, which may be a phase conjugation cell. Light passing through the quarter-wave plate is substantially circularly polarized, which is advantageous if the mirror is a phase conjugation cell using stimulated Brillouin scattering (SBS). A second pass through the quarter-wave plate provides a linearly polarized beam of which the polarization angle is orthogonally related to that of the original beam, to facilitate out-coupling of energy from the apparatus. The Faraday rotator effects a total polarization angle rotation of 90.degree. in two passes and helps compensate for birefringence when the beam is passed through the birefringent medium again on the return pass. The combination of the quarter-wave plate and the Faraday rotator provides better birefringence cancellation than either element acting alone.
    • 用于补偿在双折射介质(例如固态放大器)中引入的双折射的装置和相关方法。 本发明包括四分之一波片,法拉第旋转器和反射镜的组合,其可以是相位共轭单元。 通过四分之一波片的光基本上是圆偏振的,如果反射镜是使用受激布里渊散射(SBS)的相位共轭单元,这是有利的。 通过四分之一波片的第二次通过提供线性偏振光束,其偏振角与原始光束正交相关,以促进来自该装置的能量的外耦合。 法拉第旋转器在两次通过中实现90°的总偏振角旋转,并且当光束在返回通道上再次通过双折射介质时有助于补偿双折射。 四分之一波片和法拉第旋转器的组合提供比单独作用的任一元件更好的双折射消除。
    • 5. 发明授权
    • Highly-efficient solid-state blue laser
    • 高效固态蓝光激光
    • US5216681A
    • 1993-06-01
    • US739974
    • 1991-08-05
    • Randall J. St. PierreHagop InjeyanLarry G. DeShazer
    • Randall J. St. PierreHagop InjeyanLarry G. DeShazer
    • H01S3/0941H01S3/16
    • H01S3/16H01S3/0941H01S3/1611H01S3/167
    • A highly-efficient solid-state blue laser that exploits a strong emission line provided by a solid-state laser medium of neodymium-doped scandium oxide (Nd:Sc.sub.2 O.sub.3) to produce a beam of coherent blue light at a wavelength matching the absorption line of cesium at 455.6 nm (0.4556 microns). The solid-state blue laser includes the laser medium of neodymium-doped scandium oxide, a semiconductor diode laser array for optically pumping the laser medium to produce a beam of coherent infrared radiation at a wavelength of approximately 1367 nm (1.367 microns), and optical means for tripling the frequency of the beam of coherent infrared radiation to produce a beam of coherent blue light at the wavelength of approximately 455.6 nm. The solid-state blue laser is simple, highly efficient and provides relatively high power outputs.
    • 利用由钕掺杂钪氧化物(Nd:Sc 2 O 3)的固体激光介质提供的强发射线的高效率固态蓝色激光器,以产生与吸收线的吸收线匹配的波长的相干蓝光 铯在455.6nm(0.4556微米)。 固态蓝色激光器包括钕掺杂钪氧化物的激光介质,用于光学泵浦激光介质以产生约1367nm(1.367微米)的波长的相干红外辐射束的半导体二极管激光器阵列,以及光学 用于使相干红外辐射光束的频率增加三倍的装置,以产生约455.6nm波长的相干蓝光光束。 固态蓝色激光器简单,高效,并提供相对较高的功率输出。
    • 6. 发明授权
    • Variable coherence length high brightness laser architecture
    • 可变相干长度高亮度激光器架构
    • US5825791A
    • 1998-10-20
    • US520349
    • 1995-08-28
    • Hagop InjeyanLawrence J. LemboRandall J. St. PierreMarcy M. Valley
    • Hagop InjeyanLawrence J. LemboRandall J. St. PierreMarcy M. Valley
    • H01S3/05G02F1/03H01S3/00H01S3/10H01S3/16H01S3/23
    • H01S3/0057H01S3/10076H01S3/2333
    • A high power laser source having a preselected broad bandwidth, including a master oscillator providing a single-mode laser beam, a resonant electro-optical modulator and a source of radio-frequency (rf) modulation voltage, to produce a modulator output beam having sidebands spaced on each side of the nominal frequency of the single-mode laser beam. The bandwidth and the number of modes may be varied by controlling the voltage applied to the modulator. At least one additional modulator in series with the first provides for the addition of other sidebands overlaying those generated with just one modulator. In another embodiment of the invention, the modulator is installed in a PC MOPA (phase conjugated master oscillator power amplifier) configuration to provide modulation only on the return path of the beam from a phase conjugation device having a stimulated Brillouin scattering (SBS) medium. Because the electro-optical modulator is sensitive to polarization direction, it can be oriented to be effective only for the return beam, which has a different direction of polarization from that of the single-mode laser beam, thus optimizing the performance of the SBS medium.
    • 具有预选宽带宽的高功率激光源,包括提供单模激光束的主振荡器,谐振电光调制器和射频(RF)调制电压源),以产生具有边带的调制器输出光束 在单模激光束的标称频率的每一侧隔开。 可以通过控制施加到调制器的电压来改变带宽和模式数量。 与第一个串联的至少一个附加调制器提供了与仅用一个调制器产生的边带重叠的其他边带的添加。 在本发明的另一个实施例中,调制器安装在PC MOPA(相位共轭主振荡器功率放大器)配置中,以仅提供来自具有受激布里渊散射(SBS)介质的相位共轭装置的波束的返回路径的调制。 因为电光调制器对极化方向敏感,所以它可以被定向为仅对于具有与单模激光束的偏振方向不同的返回光束有效,从而优化SBS介质的性能 。
    • 8. 发明授权
    • End pumped zig-zag slab laser gain medium
    • 末端抽取锯齿状平板激光增益介质
    • US06268956B1
    • 2001-07-31
    • US09580726
    • 2000-05-30
    • Hagop InjeyanCarolyn S. HoeferStephen P. Palese
    • Hagop InjeyanCarolyn S. HoeferStephen P. Palese
    • H01S300
    • H01S3/0602H01S3/042H01S3/0606H01S3/0612H01S3/0615H01S3/0623H01S3/0625H01S3/063H01S3/08095H01S3/094053H01S3/094057H01S3/09408H01S3/0941H01S3/09415H01S3/11H01S3/1603H01S3/1643H01S3/2308H01S3/2383
    • An optical amplifier (20, 100) includes an elongated slab (22, 102) of solid state lapsing material, such as a rare earth doped yttrium-aluminum-garnet (YAG) slab. In order to provide a relatively increased absorption length and thus a higher overall efficiency, the optical amplifier (20, 100) in accordance with the present invention incorporates end pumping in which the pumped light is coaligned with the amplified light resulting in relatively longer absorption lengths and higher overall efficiencies. The coaligned pumped sources are directed to lateral faces of the slab (22, 102) which include footprints (41, 43, 108) or windows. In order to cause internal reflection of the pump beam along the lapsing axis, the end faces (28, 30, 110) are formed at about a 45° angle relative to the longitudinal axis which causes the pumped light to be reflected within the slab co-axially with amplified light. In order to confine the absorption of the pumped light to the center portion of the slab (22, 102), the slab (22, 102) may be formed from a composite material with the opposing end portions of the slab formed from an undoped host material while the center portion of the slab along the longitudinal axis is formed from a doped host material. Such a configuration provides relatively low residual thermal lensing with virtually no birefringence. In one embodiment, the pumping light from the diode arrays is coupled to the slab (22, 102) by way of lenses (54) or lens ducts (FIG. 1). In an alternate embodiment, the pumping light is coupled to the slab (22, 102) by way of optical fibers (104, 106). In yet another embodiment (FIG. 8), the pumping light and laser beams are interchanged forming a low-loss straight through slab with end pumped architecture.
    • 光学放大器(20,100)包括固态收缩材料的细长板(22,102),例如稀土掺杂的钇 - 铝 - 石榴石(YAG)板。 为了提供相对增加的吸收长度并因此提供更高的总体效率,根据本发明的光放大器(20,100)包括端泵浦,其中泵浦的光与放大的光轴相结合,导致相对更长的吸收长度 并提高整体效率。 联合泵送源被引导到板坯(22,102)的侧面,其包括脚印(41,43,108)或窗口。 为了引起泵浦光束沿着折叠轴的内部反射,端面(28,30,110)相对于纵向轴线以大约45°的角度形成,这导致泵送的光在板坯co 用放大的光轴。 为了将抽吸光的吸收限制在板坯(22,102)的中心部分,板坯(22,102)可以由复合材料形成,其中板坯的相对端部由未掺杂的主体 而沿着纵向轴线的板坯的中心部分由掺杂的主体材料形成。 这种构造提供了相对较低的剩余热透镜,实际上没有双折射。 在一个实施例中,来自二极管阵列的泵浦光通过透镜(54)或透镜导管(图1)耦合到板坯(22,102)。 在替代实施例中,泵浦光通过光纤(104,106)耦合到板坯(22,102)。 在另一个实施例(图8)中,泵浦光和激光束互换形成具有末端泵浦结构的低损耗直通板。
    • 9. 发明授权
    • Laser with two orthogonal zig-zag slab gain media for optical phase distortion compensation
    • 激光器具有两个正交的Z形板式增益介质,用于光学相位失真补偿
    • US06178040B1
    • 2001-01-23
    • US09104477
    • 1998-06-25
    • Hagop InjeyanRandall J. St. PierreStephen P. Palese
    • Hagop InjeyanRandall J. St. PierreStephen P. Palese
    • H01S300
    • H01S3/08095H01S3/0606H01S3/07H01S3/08072H01S3/2316
    • An optical amplifier for use with a solid state laser which includes a pair of elongated slabs of a solid state lasing material, such as a rare earth doped yttrium-aluminum-garnet (YAG) crystal. Two embodiments of the invention are disclosed. In both embodiments of the invention, each of the elongated slabs is formed with a square or generally rectangular cross-section. The slabs are configured such that the longitudinal axes of the slabs are generally co-axial aligned and the slabs are orientated such that the major axis of the slabs are generally orthogonal. By configuring the two slabs to be orthogonal with respect to one another, the integrated thermal lens becomes azimuthally symmetric and can be compensated by a simple external lens. In addition, the negative lensing affect along the major axis of one slab is used to compensate for the positive lensing affect along the minor axis of the other slab and vice versa, thus minimizing the affects of the astigmatism. In an alternate embodiment of the invention, a dove prism is used to rotate the beam instead of rotation of the slabs.
    • 一种用于固态激光器的光放大器,其包括一对固体激光材料的细长板,例如稀土掺杂的钇铝石榴石(YAG)晶体。 公开了本发明的两个实施例。 在本发明的两个实施例中,每个细长板形成有方形或大致矩形的横截面。 板坯构造成使得板坯的纵向轴线大体上同轴对齐,并且板坯被定向成使得板坯的长轴线大致正交。 通过将这两个平板相互配合,集成的热透镜变为方位角对称的,并且可以通过简单的外部透镜进行补偿。 此外,沿着一个板坯的长轴的负透镜影响用于补偿沿着另一个板坯的短轴的正透镜影响,反之亦然,从而最小化散光的影响。 在本发明的替代实施例中,使用鸽子棱镜来旋转梁而不是板的旋转。
    • 10. 发明授权
    • Birefringence-compensated alignment-insensitive frequency doubler
    • 双折射补偿对准不敏感倍频器
    • US5467214A
    • 1995-11-14
    • US152647
    • 1993-11-12
    • Lee O. HeflingerWilliam W. SimmonsRandall J. St. PierreHagop Injeyan
    • Lee O. HeflingerWilliam W. SimmonsRandall J. St. PierreHagop Injeyan
    • G02F1/35G02F1/355G02F1/37H01S3/10H01S3/109G01J1/20
    • G02F1/37H01S3/109H01S3/10076
    • Apparatus and a related method for generating a second harmonic frequency optical output from a fundamental frequency input beam, without significant birefringence. The apparatus includes two Type II doubler crystals of equal length arranged with their corresponding axes parallel to each other, and a polarization rotator positioned between the doubler crystals, to rotate the polarization angle of a residual fundamental frequency component of an output beam from one of the crystals by 90.degree. or an odd multiple of 90.degree.. Random birefringence introduced into one of the doubler crystals is virtually canceled in the other, and the assembly of the two crystals and the polarization rotator may be angularly adjusted as needed for phase matching or tuning, without detracting from the birefringence compensation capability. The invention is also disclosed in the context of a phase conjugated master oscillator power amplifier (PC MOPA) system.
    • 用于从基频输入光束产生二次谐波频率光输出的装置和相关方法,没有显着的双折射。 该装置包括两个相等长度的II型倍频晶体,它们的对应的轴线彼此平行,并且偏振旋转器位于倍晶晶体之间,以使输出光束的剩余基频分量的偏振角从 晶体90°或90°的奇数倍。 引入到倍晶晶体之一中的随机双折射在另一个实际上被消除,并且两个晶体和偏振旋转器的组装可以根据需要进行角度调整,以进行相位匹配或调谐,而不会降低双折射补偿能力。 在相位共轭主振荡器功率放大器(PC MOPA)系统的上下文中也公开了本发明。