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    • 23. 发明授权
    • Method and apparatus for optical beam combination and cleanup using
stimulated scattering
    • 用于光束组合和使用受激散射的清理的方法和装置
    • US5208881A
    • 1993-05-04
    • US810980
    • 1991-12-20
    • Hans W. Bruesselbach
    • Hans W. Bruesselbach
    • G02B6/34H01S3/00H01S3/30
    • H01S3/302H01S3/005
    • An optical beam is made closer to diffraction limited by coupling it into a multi-mode guide, such as an optical fiber, of sufficient length to generate a stimulated Brillouin scattering (SBS) return beam with improved divergence. For this purpose the term .DELTA.kL is made substantially greater than .pi., where .DELTA.k is the difference in propagation vectors between the input and SBS beams, and L is the mutual interaction length of the input and SBS beams within the fiber. Beam amplification can also be provided by coupling a plurality of low power input beams that have respective wavelengths within the fiber's SBS linewidth into the fiber so that each of the input beams transfers energy into the SBS beam, which emerges with a power greater than that of any of its inputs. The beam cleanup and amplification functions are capable of operating with continuous wave or pulsed inputs.
    • 通过将光束耦合到具有足够长度的多模引导件(例如光纤)中,使光束更接近衍射,以产生具有改善的发散的受激布里渊散射(SBS)返回光束。 为此,术语DELTA kL基本上大于pi,其中ΔTAk是输入和SBS波束之间的传播矢量的差,L是光纤内的输入和SBS波束的相互作用长度。 光束放大还可以通过将具有光纤SBS线宽内的各个波长的多个低功率输入光束耦合到光纤中来提供,使得每个输入光束将能量传递到SBS光束中,SBS光束的功率大于 其任何投入。 光束清除和放大功能能够连续波或脉冲输入。
    • 26. 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。
    • 29. 发明授权
    • Hermetically sealed apparatus and method for maintaining crystals at a
controlled operating temperature
    • 密封装置和在受控工作温度下保持晶体的方法
    • US4968121A
    • 1990-11-06
    • US281134
    • 1988-12-07
    • Hans W. BruesselbachRobert H. Sipman
    • Hans W. BruesselbachRobert H. Sipman
    • G02F1/35G02F1/37G05D23/20
    • G02F1/3501G05D23/1919G05D23/20G02F1/37G02F2001/3505
    • An apparatus for maintaining a crystal at a precisely controlled operating temperature over extended periods of time without significant thermal degradation of the crystal. The apparatus has thermally conducting walls. The walls define an inner hermetically sealed chamber for the crystal. Input and output windows are hermetically sealed to the input and output ends of the chamber. The inner surfaces of these windows are maintained at the operating temperature of the crystal to prevent fogging of the windows. Flexible thermal conducting layers are used between the crystal surfaces and the walls of the chamber to achieve uniform and continuous thermal contact therebetween, without mechanical stress to the crystal. The structure provides fast thermal response, controlled temperature in the crystal interaction region and stability of operation over extended periods of time. In one preferred embodiment, the crystal is held in suspended position within the chamber between a pair of spring-loaded plungers. Other embodiments and options are also disclosed.
    • 一种用于在晶体长时间内将晶体保持在精确控制的工作温度下而不会明显的热降解的装置。 该装置具有导热壁。 这些墙壁为水晶界定了一个内部密封的室。 输入和输出窗口密封到腔室的输入和输出端。 这些窗口的内表面保持在晶体的工作温度,以防止窗户起雾。 在晶体表面和室壁之间使用柔性导热层,以在其间实现均匀且连续的热接触,而不会对晶体造成机械应力。 该结构提供快速的热响应,晶体相互作用区域中的受控温度和长时间的操作稳定性。 在一个优选实施例中,晶体在一对弹簧加载柱塞之间的室内被保持在悬挂位置。 还公开了其它实施例和选项。
    • 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。