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    • 1. 发明申请
    • REGENERATIVE LASER AMPLIFIER
    • 再生激光放大器
    • US20090174930A1
    • 2009-07-09
    • US11970916
    • 2008-01-08
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • H01S3/30
    • H01S3/235H01S3/06754H01S3/094003H01S3/094015H01S3/094084H01S3/10084H01S3/302H01S3/305
    • A laser amplifier system is presented including a pump regenerative amplifier. The amplifier generally has a cavity defined by a pair of end cavity mirrors between which an amplified pump pulse oscillates. The amplifier also includes an interaction cell with a tunable gain medium amplifies laser pulses (e.g., Raman gain). The interaction cell may be positioned within the pump amplifier cavity and an input pulse may be injected into the cavity of the amplifier to transit through the tunable gain medium of the interaction cell. A pump pulse transfers energy via interaction with the input pulse (e.g., Raman interaction) as the pulses counter-propagate through the gain medium of the interaction cell. Amplification of output laser pulses, however, is generally achieved according to the wavelength of the pump laser pulses thereby providing a wavelength dependent, or “tunable”, means for amplifying laser pulses.
    • 提出了一种包括泵再生放大器的激光放大器系统。 放大器通常具有由一对端腔反射镜限定的空腔,放大的泵浦脉冲在其之间振荡。 放大器还包括具有可调增益介质的相互作用单元放大激光脉冲(例如,拉曼增益)。 相互作用单元可以位于泵浦放大器空腔内,并且输入脉冲可以被注入到放大器的空腔中,以便穿过相互作用单元的可调增益介质。 当脉冲通过相互作用单元的增益介质反向传播时,泵浦脉冲通过与输入脉冲(例如,拉曼相互作用)的相互作用传递能量。 然而,输出激光脉冲的放大通常根据泵浦激光脉冲的波长来实现,从而提供用于放大激光脉冲的波长依赖性或“可调谐”装置。
    • 3. 发明授权
    • Regenerative laser amplifier
    • 再生激光放大器
    • US08891162B2
    • 2014-11-18
    • US13164506
    • 2011-06-20
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • H01S3/30H01S3/10H01S3/23H01S3/067H01S3/094
    • H01S3/235H01S3/06754H01S3/094003H01S3/094015H01S3/094084H01S3/10084H01S3/302H01S3/305
    • A laser amplifier system is presented including a pump regenerative amplifier. The amplifier generally has a cavity defined by a pair of end cavity mirrors between which an amplified pump pulse oscillates. The amplifier also includes an interaction cell with a tunable gain medium amplifies laser pulses (e.g., Raman gain). The interaction cell may be positioned within the pump amplifier cavity and an input pulse may be injected into the cavity of the amplifier to transit through the tunable gain medium of the interaction cell. A pump pulse transfers energy via interaction with the input pulse (e.g., Raman interaction) as the pulses counter-propagate through the gain medium of the interaction cell. Amplification of output laser pulses, however, is generally achieved according to the wavelength of the pump laser pulses thereby providing a wavelength dependent, or “tunable”, means for amplifying laser pulses.
    • 提出了一种包括泵再生放大器的激光放大器系统。 放大器通常具有由一对端腔反射镜限定的空腔,放大的泵浦脉冲在其之间振荡。 放大器还包括具有可调增益介质的相互作用单元放大激光脉冲(例如,拉曼增益)。 相互作用单元可以位于泵浦放大器空腔内,并且输入脉冲可以被注入到放大器的空腔中,以便穿过相互作用单元的可调增益介质。 当脉冲通过相互作用单元的增益介质反向传播时,泵浦脉冲通过与输入脉冲(例如,拉曼相互作用)的相互作用传递能量。 然而,输出激光脉冲的放大通常根据泵浦激光脉冲的波长来实现,从而提供用于放大激光脉冲的波长依赖性或“可调谐”装置。
    • 9. 发明申请
    • REGENERATIVE LASER AMPLIFIER
    • 再生激光放大器
    • US20110249318A1
    • 2011-10-13
    • US13164506
    • 2011-06-20
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • H01S3/30H01S3/00
    • H01S3/235H01S3/06754H01S3/094003H01S3/094015H01S3/094084H01S3/10084H01S3/302H01S3/305
    • A laser amplifier system is presented including a pump regenerative amplifier. The amplifier generally has a cavity defined by a pair of end cavity mirrors between which an amplified pump pulse oscillates. The amplifier also includes an interaction cell with a tunable gain medium amplifies laser pulses (e.g., Raman gain). The interaction cell may be positioned within the pump amplifier cavity and an input pulse may be injected into the cavity of the amplifier to transit through the tunable gain medium of the interaction cell. A pump pulse transfers energy via interaction with the input pulse (e.g., Raman interaction) as the pulses counter-propagate through the gain medium of the interaction cell. Amplification of output laser pulses, however, is generally achieved according to the wavelength of the pump laser pulses thereby providing a wavelength dependent, or “tunable”, means for amplifying laser pulses.
    • 提出了一种包括泵再生放大器的激光放大器系统。 放大器通常具有由一对端腔反射镜限定的空腔,放大的泵浦脉冲在其之间振荡。 放大器还包括具有可调增益介质的相互作用单元放大激光脉冲(例如,拉曼增益)。 相互作用单元可以位于泵浦放大器空腔内,并且输入脉冲可以被注入到放大器的空腔中,以便穿过相互作用单元的可调增益介质。 当脉冲通过相互作用单元的增益介质反向传播时,泵浦脉冲通过与输入脉冲(例如,拉曼相互作用)的相互作用传递能量。 然而,输出激光脉冲的放大通常根据泵激光脉冲的波长来实现,从而提供用于放大激光脉冲的波长依赖性或“可调谐”装置。
    • 10. 发明授权
    • Regenerative laser amplifier
    • 再生激光放大器
    • US07982947B2
    • 2011-07-19
    • US11970916
    • 2008-01-08
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • Stephen W. McCahonSamvel SarkisyanPaul B. Lundquist
    • H01S4/00H01S3/00
    • H01S3/235H01S3/06754H01S3/094003H01S3/094015H01S3/094084H01S3/10084H01S3/302H01S3/305
    • A laser amplifier system is presented including a pump regenerative amplifier. The amplifier generally has a cavity defined by a pair of end cavity mirrors between which an amplified pump pulse oscillates. The amplifier also includes an interaction cell with a tunable gain medium amplifies laser pulses (e.g., Raman gain). The interaction cell may be positioned within the pump amplifier cavity and an input pulse may be injected into the cavity of the amplifier to transit through the tunable gain medium of the interaction cell. A pump pulse transfers energy via interaction with the input pulse (e.g., Raman interaction) as the pulses counter-propagate through the gain medium of the interaction cell. Amplification of output laser pulses, however, is generally achieved according to the wavelength of the pump laser pulses thereby providing a wavelength dependent, or “tunable”, means for amplifying laser pulses.
    • 提出了一种包括泵再生放大器的激光放大器系统。 放大器通常具有由一对端腔反射镜限定的空腔,放大的泵浦脉冲在其之间振荡。 放大器还包括具有可调增益介质的相互作用单元放大激光脉冲(例如,拉曼增益)。 相互作用单元可以位于泵浦放大器空腔内,并且输入脉冲可以被注入到放大器的空腔中,以便穿过相互作用单元的可调增益介质。 当脉冲通过相互作用单元的增益介质反向传播时,泵浦脉冲通过与输入脉冲(例如,拉曼相互作用)的相互作用传递能量。 然而,输出激光脉冲的放大通常根据泵激光脉冲的波长来实现,从而提供用于放大激光脉冲的波长依赖性或“可调谐”装置。