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    • 21. 发明授权
    • High gain laser amplifier
    • 高增益激光放大器
    • US06646793B2
    • 2003-11-11
    • US09736997
    • 2000-12-14
    • Hans W. BruesselbachAlexander A. BetinDavid S. Sumida
    • Hans W. BruesselbachAlexander A. BetinDavid S. Sumida
    • H01S300
    • H01S3/063H01S3/0602H01S3/0612H01S3/0617H01S3/1618H01S3/1643
    • A high gain optical amplifier and method. Generally, the inventive amplifier includes a first crystal having an axis and a first index of refraction and a second crystal bonded to the first crystal about the axis and having a second index of refraction. The first index is higher than the second index such that light through the first crystal is totally internally reflected. In the illustrative embodiment, the first crystal is Yb:YAG with an index of approximately 1.82, the second crystal is Sapphire with an index of approximately 1.78, and the axis is the propagation axis. The invention is, in its preferred embodiment, a light guide fabricated out of crystalline materials, diffusion bonded together. If the core of the light guide is doped with laser ions, high gain amplifiers made be designed and operable over a large étendue. With a judicious choice of the laser crystal and cladding materials, shape, and bonding technique, the guided amplifier is much less susceptible to parasitic oscillation than amplifiers constructed in accordance with conventional teachings. The clad core is also able to handle larger thermal load without breakage than can an unclad core.
    • 高增益光放大器和方法。 通常,本发明的放大器包括具有轴和第一折射率的第一晶体,以及围绕轴线键合到第一晶体并具有第二折射率的第二晶体。 第一指数高于第二指数,使得通过第一晶体的光完全内部反射。 在说明性实施例中,第一晶体为Yb:YAG,折射率约为1.82,第二晶体为蓝宝石,折射率约为1.78,轴为传播轴。 在其优选实施例中,本发明是由结晶材料制成的光导,扩散结合在一起。 如果光导的核心掺杂有激光离子,则高增益放大器可以在大的衰减范围内设计和操作。 通过明智地选择激光晶体和包层材料,形状和结合技术,与根据常规教导构建的放大器相比,引导放大器不太容易发生寄生振荡。 包芯可以处理较大的热负载,而不会破损。
    • 23. 发明授权
    • Laser pump cavity apparatus with improved thermal lensing control,
cooling, and fracture strength and method
    • 激光泵腔设备具有改进的热透镜控制,冷却和断裂强度和方法
    • US5974061A
    • 1999-10-26
    • US994423
    • 1997-12-19
    • Robert W. ByrenDavid S. SumidaHans W. Bruesselbach
    • Robert W. ByrenDavid S. SumidaHans W. Bruesselbach
    • H01S3/042H01S3/06H01S3/08H01S3/094H01S3/0941H01S3/04
    • H01S3/094H01S3/0941H01S3/042H01S3/0606H01S3/0612H01S3/08072H01S3/08095H01S3/094084
    • A laser pump cavity apparatus with integral concentrator provides improved thermal lensing control, cooling and fracture strength. The concentrator is formed around a doped solid-state laser medium by diffusion bonding, using a material different than the doped laser medium and with a substantially lower index of refraction, higher thermal conductivity and higher stress fracture strength than the doped laser crystal. The concentrator has a top cladding layer with a cylindrical focusing surface and a bottom cladding layer with a cylindrical focusing surface and may have edge cladding layers. Cold plates, each of which also has one cylindrical surface, are placed in thermal contact with the cylindrical surfaces of the top and bottom cladding layers. The cylindrical surfaces preferably have hyperbolic or quasi-hyperbolic shape. The laser pump cavity apparatus is preferably pumped with several laser diode arrays in directions transverse to a laser beam axis. The pumplight is injected from the laser diode arrays through the edge cladding layers in directions toward line foci of the cylindrical surfaces. The concentrator top and bottom cladding material is preferably sapphire and the doped solid-state laser medium is preferably Yb:YAG. The edge cladding layers are preferably thermally insulating to maintain a one-dimensional heat flow condition within the doped laser medium, by forming them of a material that has lower thermal conductivity than the material used for the top and bottom cladding layers. The edge cladding layers are preferably made of undoped YAG material
    • 具有整体浓缩器的激光泵腔设备提供改进的热透镜控制,冷却和断裂强度。 集中器通过扩散接合形成在掺杂的固态激光介质周围,使用与掺杂的激光介质不同的材料,并且具有比掺杂的激光晶体低得多的折射率,更高的热导率和更高的应力断裂强度。 集中器具有具有圆柱形聚焦表面的顶部包层和具有圆柱形聚焦表面的底部包层,并且可以具有边缘包覆层。 它们中的每一个也具有一个圆柱形表面,与顶部和底部包层的圆柱形表面热接触。 圆柱形表面优选具有双曲线或准双曲线形状。 激光泵腔装置优选地在与激光束轴线横切的方向上用几个激光二极管阵列泵送。 该激光二极管阵列沿着朝向圆柱形表面的线焦点的方向通过边缘包覆层注入。 集中器顶部和底部包层材料优选是蓝宝石,并且掺杂的固态激光介质优选为Yb:YAG。 边缘覆层优选是隔热的,以通过形成具有比用于顶部和底部包层的材料低的导热性的材料来保持掺杂的激光介质内的一维热流条件。 边缘覆层优选由未掺杂的YAG材料制成
    • 24. 发明授权
    • Efficient phase conjugate laser
    • 高效相位共轭激光器
    • US4734911A
    • 1988-03-29
    • US839475
    • 1986-03-14
    • Hans W. Bruesselbach
    • Hans W. Bruesselbach
    • H01S3/10H01S3/23H01S3/30H01S3/13
    • H01S3/2333H01S3/10076
    • A laser apparatus (10) utilizing a master oscillator power amplifier configuration wherein a master oscillator (12) provides a source of low energy, high phase front quality, and high spectral purity radiation, injected into at least one lasing medium gain element (14) disposed along an optical path. Coupling means (16) is positioned to selectively couple a predetermined percentage of the master oscillator (12) radiation into the gain element (14) medium while preventing all but a predetermined percentage of any amplified radiation exiting the gain element (14) from re-entering the master oscillator (12). Phase conjugation means (20) is disposed along the optical path on the opposite side of the gain element (14) as the coupling means (16), for reflecting the phase conjugate of laser radiation incident thereon. Delay means (26) positioned between the gain element (14) and the phase conjugation means (16) assures that radiation pulses coupled along the optical path traverse and substantially exit from the gain element (14), toward the phase conjugation means (20), before any reflected radiation from the phase conjugation means (20) enters the gain element (14). In a further aspect of the invention the laser apparatus (100) further comprises imaging means (132) disposed along the optical path between said phase conjugation means (120) and said gain element (114) so as to provide maximum transfer of phase information from the lasing medium of said gain element (114) to said phase conjugate reflector (120) and back.
    • 一种利用主振荡器功率放大器配置的激光装置(10),其中主振荡器(12)提供注入到至少一个激光介质增益元件(14)中的低能量,高相位前质量和高光谱纯度辐射源, 沿光路设置。 耦合装置(16)被定位成选择性地将预定百分比的主振荡器(12)辐射耦合到增益元件(14)介质中,同时防止离开增益元件(14)的任何放大的放射线的预定百分比除以重新 进入主振荡器(12)。 相位共轭装置(20)沿着作为耦合装置(16)的增益元件(14)的相反侧的光路布置,用于反射入射在其上的激光辐射的相位共轭。 位于增益元件(14)和相位共轭装置(16)之间的延迟装置(26)确保沿着光路耦合的辐射脉冲朝向相位共轭装置(20)大体上从增益元件(14)退出, 在来自相位共轭装置(20)的反射辐射进入增益元件(14)之前。 在本发明的另一方面,激光装置(100)还包括沿着所述相位共轭装置(120)和所述增益元件(114)之间的光路布置的成像装置(132),以便提供相位信息从 所述增益元件(114)的激光介质到达所述相位共轭反射器(120)并返回。
    • 27. 发明授权
    • Method for fabricating and using a light waveguide
    • 制造和使用光波导的方法
    • US07217585B1
    • 2007-05-15
    • US11395702
    • 2006-03-31
    • David S. SumidaAuthi A. NarayananHans W. Bruesselbach
    • David S. SumidaAuthi A. NarayananHans W. Bruesselbach
    • H01L21/20
    • G02B6/1342
    • A waveguide is fabricated by first preparing two waveguide precursor pieces. Each waveguide precursor piece includes a single-crystal substrate, and an epitaxial coating layer of an oxide coating material on the substrate. The oxide substrate material preferably comprises yttrium as a substrate-material cation, and the oxide coating material preferably comprises a coating-material cation selected from the group consisting of ytterbium, thulium, erbium, and holmium. The two substrates are placed together with the coating layers in contact to form a precursor structure. The precursor structure is heated to an elevated diffusion temperature so that the coating layers bond together and the coating materials and the respective substrate materials interdiffuse to form the waveguide having an interdiffused region. A laser beam may be directed through the interdiffused region, while the interdiffused region is optionally optically pumped through one or both of the substrates.
    • 通过首先制备两个波导前体件来制造波导。 每个波导前体件包括单晶衬底和在衬底上的氧化物涂层材料的外延涂层。 氧化物基材优选包含作为基材材料阳离子的钇,氧化物涂层材料优选包含选自镱,ium,铒和钬的涂料阳离子。 将两个基板与涂层接触放置在一起以形成前体结构。 将前体结构加热到升高的扩散温度,使得涂层结合在一起,并且涂层材料和相应的衬底材料相互扩散以形成具有相互扩散区​​域的波导。 激光束可以被引导穿过相互扩散的区域,而相互扩散的区域可选地被光泵浦通过一个或两个基底。
    • 30. 发明授权
    • Single mirror integral raman laser
    • 单镜组合拉曼激光
    • US4821272A
    • 1989-04-11
    • US924108
    • 1986-10-31
    • Hans W. BruesselbachDonald R. Dewhirst
    • Hans W. BruesselbachDonald R. Dewhirst
    • H01S3/30
    • H01S3/305
    • A Raman laser (10) is provided using a pump laser (22) as a source of radiation at a first wavelength and a Raman cell (30) for converting the first wavelength radiation to a second wavelength. The pump laser (20) provides polarized radiation at a predetermined first wavelength which is focused by a focusing means (40) into a Raman medium (32) which converts radiation at the first wavelength to a predetermined second wavelength by Raman scattering processes. A reflection means (50) which is aligned normal to the first wavelength radiation is disposed between the pump laser (20) and focusing means (40). The reflection means is substantially 100% reflective of radiation at the second wavelength and substantially non-reflective of radiation at the first wavelength. A polarizing means (70) and quarter-wave plate (60) are disposed along the optical path between the Raman medium (32) and the pump laser (20) for allowing propagation of the first wavelength to the Raman medium (32) but preventing SBS radiation from entering the pump laser (20) from the Raman medium.Alternatively, the pump laser includes an output reflection means (124) that is substantially 100% reflective of radiation at the second wavelength and partially reflective of radiation at the first wavelength. This embodiment achieves automatic alignment of the pump laser and the Raman medium (32) and does not use additional reflection means, polarization means, or a quarter-wave plate.
    • 使用泵浦激光器(22)作为第一波长的辐射源和用于将第一波长辐射转换为第二波长的拉曼单元(30)提供拉曼激光器(10)。 泵浦激光器(20)以预定的第一波长提供偏振辐射,该预定的第一波长由聚焦装置(40)聚焦成通过拉曼散射方法将第一波长的辐射转换成预定的第二波长的拉曼介质(32)。 与泵浦激光器(20)和聚焦装置(40)之间设置与第一波长辐射垂直对准的反射装置(50)。 反射装置基本上100%反射第二波长处的辐射,并且基本上不反射第一波长处的辐射。 沿着拉曼介质(32)和泵浦激光器(20)之间的光路设置偏振装置(70)和四分之一波片(60),用于允许第一波长传播到拉曼介质(32),但防止 SBS辐射从拉曼介质进入泵激光器(20)。 或者,泵浦激光器包括输出反射装置(124),其基本上100%反射第二波长处的辐射并部分地反射第一波长的辐射。 该实施例实现了泵浦激光器和拉曼介质(32)的自动对准,并且不使用附加的反射装置,偏振装置或四分之一波片。