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    • 4. 发明公开
    • CONCENTRIC CYLINDRICAL CIRCUMFERENTIAL LASER
    • US20230275391A1
    • 2023-08-31
    • US18310580
    • 2023-05-02
    • Ronald LaCombKevin LaComb
    • Ronald LaCombKevin LaComb
    • H01S3/083H01S3/067H01S3/0941H01S5/10H01S5/40H01S3/06
    • H01S3/083H01S3/0627H01S3/0675H01S3/0941H01S5/1075H01S5/4056H01S5/42
    • The present disclosure relates to a three-dimensional cylindrical cavity-type laser system capable of supporting circumferential radial emission. A cylindrical ring waveguide provides optical confinement in the radial and axial dimensions thereby supporting a plurality of radial modes, one of a plurality of axial modes and a plurality of degenerate azimuthal modes. These modes constitute a set of traveling wave modes which propagate around the cylindrical ring waveguide possessing various degrees of optical confinement as quantified by their respective Q-factors. Index tailoring is used to tailor the radial refractive index profile and geometry of the waveguide to support radial modes possessing Q-factors capable of producing efficient radial emission, while gain tailoring is used to define a gain confining region which offsets modal gain factors of the modal constituency to favor a preferred set of modes supporting efficient radial emission out of the total modal constituency supported by the resonator.. Under appropriate pump actuation the selected modes produce circumferential laser radiation with the output surface comprising of the entire outer perimeter of the cylindrical ring waveguide. The design is applicable toward both micro-resonators and resonators much larger than the optical wavelength, enabling high output powers and scalability. The circumferential radial laser emission can be concentrated by positioning the cylindrical ring laser inside a three-dimensional conical mirror thereby forming a laser ring of light propagating in the axial dimension away from the surface of the laser, which can be subsequently collimated for focused using conventional optics.
    • 7. 发明授权
    • Mode tailored spherical laser
    • 模式定制球形激光器
    • US09246300B2
    • 2016-01-26
    • US13486785
    • 2012-06-01
    • Ronald LaComb
    • Ronald LaComb
    • H01S3/08H01S3/0941H01S3/00H01S3/04H01S3/22
    • H01S3/08H01S3/0071H01S3/0407H01S3/08081H01S3/0941H01S3/2222H01S2301/02
    • A spherical laser includes a transparent or semi-transparent outer spherical vessel having an internal cavity, an amplifying medium in the cavity, and means to excite the amplifying medium. The sphere is provided with a partially reflective coating to act as a spherical optical resonator. The spherical resonator includes a plurality of optically different regions containing alternative optical media from the cavity medium differing in bulk optical parameters utilized for mode tailoring. The optically different regions work collectively to exclude the whispering gallery modes from those supported by the spherical cavity. Excitation of the amplifying medium produces an optical gain. When the gain exceeds cavity losses and threshold conditions are met, lasing is supported. This creates a three-dimensional, spherically radiating emission, emulating a point source. The sphere is enclosed within a mirrored ellipse to image the output to a point, or within a mirrored parabola to columinate the emission.
    • 球面激光器包括具有内腔的透明或半透明外球形容器,腔中的放大介质和激发放大介质的装置。 该球体设置有作为球面光学谐振器的部分反射涂层。 球面谐振器包括多个光学不同的区域,其包含来自空腔介质的替代光学介质,其不同于用于模式裁剪的体光学参数。 光学上不同的区域共同工作,将耳语画廊模式与由球形腔支撑的画廊模式排除在外。 放大介质的激励产生光学增益。 当增益超过腔体损耗和阈值条件时,支持激光。 这产生了一个三维的,辐射的辐射,模拟点源。 球体被包围在镜像椭圆内以将输出成像到一个点,或者在一个镜像抛物线内将该排放物逐渐变亮。
    • 8. 发明申请
    • MODE TAILORED SPHERICAL LASER
    • 模式定制球形激光
    • US20130322475A1
    • 2013-12-05
    • US13486785
    • 2012-06-01
    • Ronald LaComb
    • Ronald LaComb
    • H01S3/08H01S3/09H01S3/04
    • H01S3/08H01S3/0071H01S3/0407H01S3/08081H01S3/0941H01S3/2222H01S2301/02
    • A spherical laser includes a transparent or semi-transparent outer spherical vessel having an internal cavity, an amplifying medium in the cavity, and means to excite the amplifying medium. The sphere is provided with a partially reflective coating to act as a spherical optical resonator. The spherical resonator includes a plurality of optically different regions containing alternative optical media from the cavity medium differing in bulk optical parameters utilized for mode tailoring. The optically different regions work collectively to exclude the whispering gallery modes from those supported by the spherical cavity. Excitation of the amplifying medium produces an optical gain. When the gain exceeds cavity losses and threshold conditions are met, lasing is supported. This creates a three-dimensional, spherically radiating emission, emulating a point source. The sphere is enclosed within a mirrored ellipse to image the output to a point, or within a mirrored parabola to columinate the emission.
    • 球面激光器包括具有内腔的透明或半透明外球形容器,腔中的放大介质和激发放大介质的装置。 该球体设置有作为球面光学谐振器的部分反射涂层。 球面谐振器包括多个光学不同的区域,其包含来自空腔介质的替代光学介质,其不同于用于模式裁剪的体光学参数。 光学上不同的区域共同工作,将耳语画廊模式与由球形腔支撑的画廊模式排除在外。 放大介质的激励产生光学增益。 当增益超过腔体损耗和阈值条件时,支持激光。 这产生了一个三维的,辐射的辐射,模拟点源。 球体被包围在镜像椭圆内以将输出成像到一个点,或者在一个镜像抛物线内将该排放物逐渐变亮。
    • 10. 发明授权
    • Scalable spherical laser
    • 可扩展球形激光器
    • US07492805B2
    • 2009-02-17
    • US11401561
    • 2006-04-11
    • Ronald LaCombSallie S. Townsend
    • Ronald LaCombSallie S. Townsend
    • H01S3/06
    • H01S3/0602H01S3/005H01S3/03H01S3/0407H01S3/05H01S3/08
    • A spherical laser includes a transparent or semi-transparent outer spherical vessel having an internal cavity, an amplifying medium in the cavity, and means to excite the amplifying medium. The sphere is provided with a partially reflective coating to act as a spherical optical resonator. Excitation of the amplifying medium produces an optical gain. When the gain exceeds cavity losses and threshold conditions are met, lasing is supported. This creates a three-dimensional, spherically radiating emission, emulating a point source. The output is radially diverging, but is harnessed by enclosing the sphere within a mirrored ellipse to image the output to a point, or within a mirrored parabola to columinate the emission. A concentric, reflective inner sphere may be disposed in the cavity, with the amplifying medium lying between the two spheres. A voltage potential is applied between the spheres to excite the medium.
    • 球面激光器包括具有内腔的透明或半透明外球形容器,腔中的放大介质和激发放大介质的装置。 该球体设置有作为球面光学谐振器的部分反射涂层。 放大介质的激励产生光学增益。 当增益超过腔体损耗和阈值条件时,支持激光。 这产生了一个三维的,辐射的辐射,模拟点源。 输出是径向发散的,但是通过将球体包围在镜像椭圆内以将输出成像到一个点,或者在镜像抛物线内以使发射逐渐收敛。 同心的反射内球可以设置在空腔中,放大介质位于两个球体之间。 在球体之间施加电压以激发介质。