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    • 1. 发明授权
    • Compact optical frequency comb systems
    • 紧凑型光频梳系统
    • US08792525B2
    • 2014-07-29
    • US13481211
    • 2012-05-25
    • Martin E. FermannThomas R. SchibliIngmar Hartl
    • Martin E. FermannThomas R. SchibliIngmar Hartl
    • H01S3/10
    • H01S3/1115H01S3/0092H01S3/06712H01S3/06725H01S3/08059H01S3/10046H01S3/105H01S3/1053H01S3/1118H01S3/1616H01S3/176
    • Compact optical frequency sources are described. The comb source may include an intra-cavity optical element having a multi-material integrated structure with an electrically controllable active region. The active region may comprise a thin film. By way of example, the thin film and an insulating dielectric material disposed between two electrodes can provide for rapid loss modulation. In some embodiments the thin film may comprise graphene. In various embodiments of a frequency comb laser, rapid modulation of the CEO frequency can be implemented via electric modulation of the transmission or reflection loss of an additional optical element, which can be the saturable absorber itself. In another embodiment, the thin film can also be used as a saturable absorber in order to facilitate passive modelocking. In some implementations the optical element may be formed on a cleaved or polished end of an optical fiber.
    • 描述了紧凑的光频源。 梳状光源可以包括具有电子可控有源区域的多材料集成结构的腔内光学元件。 有源区可以包括薄膜。 作为示例,设置在两个电极之间的薄膜和绝缘介电材料可以提供快速损耗调制。 在一些实施例中,薄膜可以包括石墨烯。 在频率梳状激光器的各种实施例中,CEO频率的快速调制可以通过附加光学元件的传输或反射损耗的电调制来实现,其可以是可饱和吸收体本身。 在另一个实施例中,薄膜也可以用作饱和吸收体,以便于被动锁模。 在一些实施方案中,光学元件可以形成在光纤的切割或抛光端上。
    • 7. 发明授权
    • Pulsed laser sources
    • 脉冲激光源
    • US08456735B2
    • 2013-06-04
    • US13526137
    • 2012-06-18
    • Martin E. FermannIngmar HartlGennady Imeshev
    • Martin E. FermannIngmar HartlGennady Imeshev
    • G02F1/35H01S3/098
    • H01S3/0057G02F1/3517G02F2001/3528H01S3/0078H01S3/0092H01S3/067H01S3/0675H01S3/06754H01S3/094042H01S3/10H01S3/105H01S3/1053H01S3/106H01S3/1067H01S3/109H01S3/1106H01S3/1118H01S3/1616
    • Modelocked fiber laser resonators may be coupled with optical amplifiers. An isolator optionally may separate the resonator from the amplifier. A reflective optical element on one end of the resonator having a relatively low reflectivity may be employed to couple light from the resonator to the amplifier. Enhanced pulse-width control may be provided with concatenated sections of both polarization-maintaining and non-polarization-maintaining fibers. Apodized fiber Bragg gratings and integrated fiber polarizers may also be included in the laser cavity to assist in linearly polarizing the output of the cavity. Very short pulses with a large optical bandwidth may be obtained by matching the dispersion value of the grating to the inverse of the dispersion of the intra-cavity fiber. Frequency comb sources may be constructed from such modelocked fiber oscillators. Low dispersion and an in-line interferometer that provides feedback may assist in controlling the frequency components output from the comb source.
    • 模式锁定光纤激光谐振器可以与光放大器耦合。 隔离器可选地可以将谐振器与放大器分离。 可以采用具有相对低的反射率的谐振器的一端上的反射光学元件来将来自谐振器的光耦合到放大器。 可以提供增强的脉冲宽度控制,其具有两个偏振保持和非偏振保持光纤的级联部分。 变形光纤布拉格光栅和集成光纤偏振器也可以包括在激光腔中,以帮助线性偏振空腔的输出。 可以通过将光栅的色散值与腔内光纤的色散相反来获得具有大的光学带宽的非常短的脉冲。 频率梳源可以由这种锁模光纤振荡器构成。 提供反馈的低色散和在线干涉仪可以有助于控制从梳状源输出的频率分量。
    • 8. 发明授权
    • Optical scanning and imaging systems based on dual pulsed laser systems
    • 基于双脉冲激光系统的光学扫描和成像系统
    • US08237122B2
    • 2012-08-07
    • US13399392
    • 2012-02-17
    • Martin E. FermannIngmar Hartl
    • Martin E. FermannIngmar Hartl
    • G01J5/02
    • H01S3/10046G01B9/02001G01N21/31G01N2021/317G02B6/02304H01S3/0675H01S3/06754H01S3/08054H01S3/1067H01S3/1068H01S3/11H01S3/1115H01S3/13H01S3/1307H01S3/1392H01S3/1394H01S3/2383
    • The invention relates to scanning pulsed laser systems for optical imaging. Coherent dual scanning laser systems (CDSL) are disclosed and some applications thereof. Various alternatives for implementation are illustrated, including highly integrated configurations. In at least one embodiment a coherent dual scanning laser system (CDSL) includes two passively modelocked fiber oscillators. The oscillators are configured to operate at slightly different repetition rates, such that a difference δfr in repetition rates is small compared to the values fr1 and fr2 of the repetition rates of the oscillators. The CDSL system also includes a non-linear frequency conversion section optically connected to each oscillator. The section includes a non-linear optical element generating a frequency converted spectral output having a spectral bandwidth and a frequency comb comprising harmonics of the oscillator repetition rates. A CDSL may be arranged in an imaging system for one or more of optical imaging, microscopy, micro-spectroscopy and/or THz imaging.
    • 本发明涉及用于光学成像的扫描脉冲激光系统。 公开了相干双扫描激光系统(CDSL)及其一些应用。 示出了用于实现的各种替代方案,包括高度集成的配置。 在至少一个实施例中,相干双扫描激光系统(CDSL)包括两个被动锁模光纤振荡器。 振荡器被配置为以稍微不同的重复率操作,使得与振荡器的重复率的值fr1和fr2相比,重复率的差δfr小。 CDSL系统还包括与每个振荡器光学连接的非线性频率转换部分。 该部分包括产生具有频谱带宽的频率转换频谱输出和包括振荡器重复频率的谐波的频率梳的非线性光学元件。 可以在成像系统中布置CDSL以用于光学成像,显微镜,微光谱和/或THz成像中的一种或多种。
    • 9. 发明授权
    • Pulsed laser sources
    • 脉冲激光源
    • US08208196B2
    • 2012-06-26
    • US12687807
    • 2010-01-14
    • Martin E. FermannIngmar HartlGennady Imeshev
    • Martin E. FermannIngmar HartlGennady Imeshev
    • G02F1/35H01S3/098
    • H01S3/0057G02F1/3517G02F2001/3528H01S3/0078H01S3/0092H01S3/067H01S3/0675H01S3/06754H01S3/094042H01S3/10H01S3/105H01S3/1053H01S3/106H01S3/1067H01S3/109H01S3/1106H01S3/1118H01S3/1616
    • Various embodiments include modelocked fiber laser resonators that may be coupled with optical amplifiers. An isolator may separate the laser resonator from the amplifier, although certain embodiments exclude such an isolator. A reflective optical element on one end of the resonator having a relatively low reflectivity may be employed to couple light from the laser resonator to the amplifier. Enhanced pulse-width control may be provided with concatenated sections of both polarization-maintaining and non-polarization-maintaining fibers. Apodized fiber Bragg gratings and integrated fiber polarizers may be also be included in the laser cavity to assist in linearly polarizing the output of the cavity. Very short pulses with a large optical bandwidth may be obtained by matching the dispersion value of the fiber Bragg grating to the inverse of the dispersion of the intra-cavity fiber. Frequency comb sources may be constructed from such modelocked fiber oscillators. In various exemplary embodiments, low dispersion and an in-line interferometer that provides feedback, assist in controlling the frequency components output from the comb source.
    • 各种实施例包括可与光放大器耦合的锁模光纤激光谐振器。 隔离器可以将激光谐振器与放大器分离,尽管某些实施例不包括这种隔离器。 可以使用具有相对较低反射率的谐振器的一端上的反射光学元件将来自激光谐振器的光耦合到放大器。 可以提供增强的脉冲宽度控制,其具有两个偏振保持和非偏振保持光纤的级联部分。 变形光纤布拉格光栅和集成光纤偏振器也可以包括在激光腔中,以帮助线性偏振空腔的输出。 可以通过将光纤布拉格光栅的色散值与腔内光纤的色散相反来获得具有大光学带宽的非常短的脉冲。 频率梳源可以由这种锁模光纤振荡器构成。 在各种示例性实施例中,提供反馈的低色散和在线干涉仪有助于控制从梳状源输出的频率分量。