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1.发明授权Optical device and method of controlling a refractive index profile in the optical device 有权控制光学元件折射率分布的光学元件及方法公开(公告)号：US08014426B2
公开(公告)日：2011-09-06
申请号：US12358608
申请日：2009-01-23
CPC分类号： H01S3/04 , H01S3/06704 , H01S3/06708 , H01S3/06716 , H01S3/0672 , H01S3/094003
摘要： An optical device includes an optical material comprising active dopant ions and absorber dopant ions spaced apart from the active dopant ions. The active dopant ions are provided to absorb a first radiation and convert a portion of the first radiation into sensible heat. A concentration profile of the absorber dopant ions is selected to absorb a second radiation different from the first radiation and optionally the first radiation in at least one direction of the optical material so as to control a refractive index profile in the at least one direction of the optical material. In another embodiment, a method of controlling a refractive index profile in an optical material includes exciting active dopant ions in the optical material with a first radiation, the active dopant ions converting at least a portion of the first radiation into sensible heat; and exciting absorber dopant ions in the optical material with a second radiation to control a refractive index profile in at least one direction of the optical material.
摘要翻译： 光学装置包括光学材料，其包括与活性掺杂剂离子间隔开的活性掺杂剂离子和吸收剂掺杂剂离子。 提供活性掺杂剂离子以吸收第一辐射并将第一辐射的一部分转换成显热。 选择吸收剂掺杂剂离子的浓度分布以吸收与光学材料的至少一个方向上的第一辐射和任选的第一辐射不同的第二辐射，以便控制光学材料的至少一个方向上的折射率分布 光学材料。 在另一个实施例中，控制光学材料中的折射率分布的方法包括用第一辐射激发光学材料中的活性掺杂剂离子，活性掺杂剂离子将第一辐射的至少一部分转化为显热; 和具有第二辐射的光学材料中激发的吸收剂掺杂剂离子，以控制光学材料的至少一个方向上的折射率分布。
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2.发明申请OPTICAL DEVICE AND METHOD OF CONTROLLING A REFRACTIVE INDEX PROFILE IN THE OPTICAL DEVICE 有权光学装置和控制光学装置中的折射率折射率剖面的方法公开(公告)号：US20100189137A1
公开(公告)日：2010-07-29
申请号：US12358608
申请日：2009-01-23
CPC分类号： H01S3/04 , H01S3/06704 , H01S3/06708 , H01S3/06716 , H01S3/0672 , H01S3/094003
摘要： An optical device includes an optical material comprising active dopant ions and absorber dopant ions spaced apart from the active dopant ions. The active dopant ions are provided to absorb a first radiation and convert a portion of the first radiation into sensible heat. A concentration profile of the absorber dopant ions is selected to absorb a second radiation different from the first radiation and optionally the first radiation in at least one direction of the optical material so as to control a refractive index profile in the at least one direction of the optical material. In another embodiment, a method of controlling a refractive index profile in an optical material includes exciting active dopant ions in the optical material with a first radiation, the active dopant ions converting at least a portion of the first radiation into sensible heat; and exciting absorber dopant ions in the optical material with a second radiation to control a refractive index profile in at least one direction of the optical material.
摘要翻译： 光学装置包括光学材料，其包括与活性掺杂剂离子间隔开的活性掺杂剂离子和吸收剂掺杂剂离子。 提供活性掺杂剂离子以吸收第一辐射并将第一辐射的一部分转换成显热。 选择吸收剂掺杂剂离子的浓度分布以吸收与光学材料的至少一个方向上的第一辐射和任选的第一辐射不同的第二辐射，以便控制光学材料的至少一个方向上的折射率分布 光学材料。 在另一个实施例中，控制光学材料中的折射率分布的方法包括用第一辐射激发光学材料中的活性掺杂剂离子，活性掺杂剂离子将第一辐射的至少一部分转化为显热; 和具有第二辐射的光学材料中激发的吸收剂掺杂剂离子，以控制光学材料的至少一个方向上的折射率分布。
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公开(公告)号：US08675694B2
公开(公告)日：2014-03-18
申请号：US13397987
申请日：2012-02-16
IPC分类号： H01S3/30
CPC分类号： H01S3/30 , F41H13/005 , F41H13/0056 , F41J2/02 , H01S3/07 , H01S3/08027 , H01S3/0815 , H01S3/082 , H01S3/094038 , H01S3/23
摘要： A system includes a laser configured to generate a pump beam at a pump wavelength. The system also includes a multi-media Raman resonator configured to receive the pump beam and generate an output beam. The multi-media Raman resonator includes multiple mirrors and multiple Raman media optically located between the minors. Output power in the output beam is spectrally concentrated around a single dominant wavelength that is longer than a pump wavelength. The longer wavelength of the output beam is associated with a combination of at least one Stokes shift associated with each of the individual Raman media. A filter could be configured to absorb light at a wavelength that is absorbed by one of the Raman media or to redirect light at the wavelength absorbed by one of the Raman media away from that Raman medium.
摘要翻译： 一种系统包括配置成产生泵浦波长的泵浦光束的激光器。 该系统还包括配置成接收泵浦光束并产生输出光束的多介质拉曼共振器。 多介质拉曼谐振器包括多个反射镜和光学地位于未成体之间的多个拉曼介质。 输出光束中的输出功率被光谱集中在比泵波长长的单个主波长上。 输出光束的较长波长与与每个单独拉曼介质相关联的至少一个斯托克斯波动的组合相关联。 滤光器可以被配置为吸收由拉曼介质之一吸收的波长的光，或者以从拉曼介质中的一个拉曼介质吸收的波长重定向光。
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4.发明申请Method and apparatus for generation and amplification of light in a semi-guiding high aspect ratio core fiber 有权用于在半导向高纵横比芯纤维中产生和放大光的方法和装置公开(公告)号：US20090041061A1
公开(公告)日：2009-02-12
申请号：US11891328
申请日：2007-08-09
CPC分类号： H01S3/06704 , H01S3/06708 , H01S3/06729 , H01S3/094019
摘要： A planar laser gain medium and laser system. The novel laser gain medium includes an active core having a high aspect ratio cross-section with a fast-axis dimension and a slow-axis dimension, signal claddings adapted to form reflective boundaries at fast-axis boundaries of the core, and a material adapted to minimize reflections at slow-axis boundaries of the core. In an illustrative embodiment, the laser gain medium is an optical fiber. The core and claddings form a waveguide adapted to control modes propagating in the fast-axis direction. When the laser gain medium is employed as a laser oscillator, a high reflectivity mirror and an outcoupler are positioned at opposite ends of the core to form a laser resonator adapted to control modes in the slow-axis direction.
摘要翻译： 平面激光增益介质和激光系统。 新颖的激光增益介质包括具有快轴尺寸和慢轴尺寸的高纵横比横截面的活性芯，适于在芯的快轴边界处形成反射边界的信号包层，以及适于 以使芯的慢轴边界处的反射最小化。 在说明性实施例中，激光增益介质是光纤。 芯和包层形成适于控制在快轴方向上传播的模式的波导。 当激光增益介质用作激光振荡器时，高反射镜和外耦合器位于芯的相对端，以形成适于控制慢轴方向的激光谐振器。
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公开(公告)号：US09438006B2
公开(公告)日：2016-09-06
申请号：US13476687
申请日：2012-05-21
CPC分类号： H01S3/30 , H01S3/083 , H01S3/094026 , H01S3/2325
摘要： According to an embodiment of the disclosure, a Raman generator includes a Raman medium and one or more optical elements. The Raman medium is configured to receive a pump pulse at a first wavelength and shift at least a portion of the pump pulse energy or power into a Stokes-shifted pulse at a second wavelength. The one or more optical elements are configured to pass the pump pulse and the Stokes-shifted pulse multiple times through the Raman medium. Each pass of the pulses through the Raman medium follows a path. Each path is parallel or anti-parallel to the other paths.
摘要翻译： 根据本发明的实施例，拉曼发生器包括拉曼介质和一个或多个光学元件。 所述拉曼介质被配置为接收第一波长的泵浦脉冲并将所述泵浦脉冲能量或功率的至少一部分移动到第二波长的斯托克斯脉冲。 一个或多个光学元件被配置为通过拉曼介质多次通过泵浦脉冲和斯托克斯位移脉冲。 通过拉曼介质的脉冲的每次通过一条路径。 每个路径与其他路径平行或反平行。
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公开(公告)号：US08705918B2
公开(公告)日：2014-04-22
申请号：US13308400
申请日：2011-11-30
CPC分类号： H01S3/06704 , H01S3/06708 , H01S3/06729 , H01S3/094019
摘要： A planar laser gain medium and laser system. The novel laser gain medium includes an active core having a high aspect ratio cross-section with a fast-axis dimension and a slow-axis dimension, signal claddings adapted to form reflective boundaries at fast-axis boundaries of the core, and a material adapted to minimize reflections at slow-axis boundaries of the core. In an illustrative embodiment, the laser gain medium is an optical fiber. The core and claddings for a waveguide adapted to control modes propagating in the fast-axis direction. When the laser gain medium is employed as a laser oscillator, a high reflectivity mirror and an outcoupler are positioned at opposite ends of the core to form a laser resonator adapted to control modes in the slow-axis direction.
摘要翻译： 平面激光增益介质和激光系统。 新颖的激光增益介质包括具有快轴尺寸和慢轴尺寸的高纵横比横截面的活性芯，适于在芯的快轴边界处形成反射边界的信号包层，以及适于 以使芯的慢轴边界处的反射最小化。 在说明性实施例中，激光增益介质是光纤。 适用于控制在快轴方向传播的模式的波导的核心和包层。 当激光增益介质用作激光振荡器时，高反射镜和外耦合器位于芯的相对端，以形成适于控制慢轴方向的激光谐振器。
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7.发明授权公开(公告)号：US08594476B2
公开(公告)日：2013-11-26
申请号：US12358983
申请日：2009-01-23
IPC分类号： G02B6/02
CPC分类号： H01S3/06708 , H01S3/06704 , H01S3/0672 , H01S3/06729 , H01S3/08045
摘要： In various embodiments, a semi-guiding optical fiber includes a core having a first refractive index and a high aspect ratio elongated cross-section along a slow axis direction. First and second signal claddings having a second refractive index sandwich the core. A third cladding having a third refractive index substantially surrounds at least side edges of the core. The first refractive index of the core, the third refractive index of the third cladding, and/or the second refractive index of the first and second signal claddings, are selected so as to maximize a differential loss between a lowest order mode propagating in the optical fiber and next order modes so as to discriminate in favor of the lowest order mode and against the next order modes. In another embodiment, a method for mode control in a semi-guiding medium includes controlling either the first refractive index of the core, the second refractive index of the first and second signal claddings, and/or the third refractive index of the third cladding, to maximize a differential loss between a lowest order mode propagating in the optical fiber and next order modes so as to discriminate in favor of the lowest order mode and against the next order modes.
摘要翻译： 在各种实施例中，半导向光纤包括沿着慢轴方向具有第一折射率和高纵横比细长横截面的芯。 具有第二折射率的第一和第二信号包层夹着芯。 具有第三折射率的第三包层基本上围绕芯的至少侧边缘。 选择芯的第一折射率，第三包层的第三折射率和/或第一和第二信号包层的第二折射率，以使在光学传播的最低阶模之间的差分损耗最大化 光纤和下一个订单模式，以便有利于最低阶模式和下一个订单模式。 在另一个实施例中，用于半导向介质中的模式控制的方法包括控制芯的第一折射率，第一和第二信号包层的第二折射率和/或第三包层的第三折射率， 以最大化在光纤中传播的最低阶模式与下一阶模式之间的差分损耗，以便有利于最低阶模式和下一阶模式。
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公开(公告)号：US09535211B2
公开(公告)日：2017-01-03
申请号：US13308789
申请日：2011-12-01
CPC分类号： G02B6/02009 , G02B6/02138 , G02B6/32 , G02B6/4208 , G02B2006/02161
摘要： In various embodiments, an optical fiber includes a core having a relatively large area selected so as to raise a threshold of stimulated Raman scattering or stimulated Brillouin scattering, or both, the core having a high aspect ratio elongated cross-section and having a first refractive index. The core is narrower in a fast-axis direction and wider in a slow-axis direction, such that the fiber is mechanically flexible in the fast-axis direction and is mechanically rigid in the slow-axis direction.
摘要翻译： 在各种实施例中，光纤包括具有选择相对较大面积的芯，以便提高受激拉曼散射或受激布里渊散射的阈值，或两者具有高纵横比细长横截面的芯并具有第一折射率 指数。 芯在快轴方向上较窄，在慢轴方向上较宽，使得光纤在快轴方向上机械地柔性并且在慢轴方向上机械地刚性。
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公开(公告)号：US08896910B2
公开(公告)日：2014-11-25
申请号：US13476652
申请日：2012-05-21
IPC分类号： G02F1/35
CPC分类号： H01S3/30 , H01S3/08027 , H01S3/08059 , H01S3/094026 , H01S3/094076 , H01S3/094084
摘要： According to an embodiment of the disclosure, a Raman generator includes a Raman medium and one or more optical elements. The Raman medium is configured to receive a pump pulse at a first wavelength and shift at least a portion of the pump pulse energy or power into a Stokes-shifted pulse at a second wavelength. The one or more optical elements are configured to synchronize one or more subsequent passages of the Stokes-shifted pulse through the Raman medium with one or more subsequent pump pulses at the first wavelength. The synchronized passage of the Stokes-shifted pulse and one or more subsequent pump pulses through the Raman medium increases a power of the Stoke-shifted pulse.
摘要翻译： 根据本公开的实施例，拉曼发生器包括拉曼介质和一个或多个光学元件。 所述拉曼介质被配置为接收第一波长的泵浦脉冲并将所述泵浦脉冲能量或功率的至少一部分移动到第二波长的斯托克斯脉冲。 所述一个或多个光学元件被配置为使经过拉曼介质的斯托克斯位移脉冲的一个或多个后续通道与第一波长的一个或多个后续泵浦脉冲同步。 斯托克斯移位脉冲和一个或多个后续泵浦脉冲通过拉曼介质的同步通过增加了斯托克斯脉冲的功率。
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公开(公告)号：US08643942B2
公开(公告)日：2014-02-04
申请号：US12915737
申请日：2010-10-29
CPC分类号： G02B6/02 , H01S3/06708 , H01S3/0672 , H01S3/08072 , H01S3/094003
摘要： In various embodiments, an optical element, e.g., an optical fiber, may be configured to compensate for thermal lensing. For example, thermal lensing may be caused by light power dissipation within an optical fiber, which may include a fiber core that guides amplified light along the longitudinal dimension of the fiber core. Thermal lensing from a thermally induced change in material refractive index as a function of position along dimensions perpendicular to the fiber's longitudinal dimension may be at least partially compensated or offset when light is guided by the fiber core by a designed-in effective refractive index profile selected such that the designed-in material refractive index of the fiber core changes as a function of transverse position within the fiber core, or by selection of a favorable cross-sectional core shape in a plane perpendicular to the longitudinal dimension of the fiber core.
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