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    • 5. 发明授权
    • Apparatus and method for mode control in a semi-guiding amplifier medium
    • 半导体放大器介质中模式控制的装置和方法
    • US08594476B2
    • 2013-11-26
    • US12358983
    • 2009-01-23
    • Vladimir V. ShkunovDavid A. RockwellRobin A. Reeder
    • Vladimir V. ShkunovDavid A. RockwellRobin A. Reeder
    • G02B6/02
    • H01S3/06708H01S3/06704H01S3/0672H01S3/06729H01S3/08045
    • 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.
    • 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。
    • 7. 发明授权
    • Multi-media raman resonators and related system and method
    • 多媒体拉曼共振器及相关系统及方法
    • US08675694B2
    • 2014-03-18
    • US13397987
    • 2012-02-16
    • Vladimir V. ShkunovDavid A. Rockwell
    • Vladimir V. ShkunovDavid A. Rockwell
    • H01S3/30
    • H01S3/30F41H13/005F41H13/0056F41J2/02H01S3/07H01S3/08027H01S3/0815H01S3/082H01S3/094038H01S3/23
    • 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.
    • 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。
    • 8. 发明授权
    • Optical device and method of controlling a refractive index profile in the optical device
    • 控制光学元件折射率分布的光学元件及方法
    • US08014426B2
    • 2011-09-06
    • US12358608
    • 2009-01-23
    • Vladimir V. ShkunovDavid A. RockwellScott T. Johnson
    • Vladimir V. ShkunovDavid A. RockwellScott T. Johnson
    • H01S3/30G02B6/02G02B6/36
    • H01S3/04H01S3/06704H01S3/06708H01S3/06716H01S3/0672H01S3/094003
    • 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.
    • 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。
    • 9. 发明授权
    • Apparatus and method for mode control in a semi-guiding amplifier medium
    • 半导体放大器介质中模式控制的装置和方法
    • US08606062B2
    • 2013-12-10
    • US13616758
    • 2012-09-14
    • Vladimir V. ShkunovDavid A. RockwellRobin A. Reeder
    • Vladimir V. ShkunovDavid A. RockwellRobin A. Reeder
    • G02B6/02
    • H01S3/06708H01S3/06704H01S3/0672H01S3/06729H01S3/08045
    • In various examples, a semi-guiding optical fiber includes a core having a high aspect ratio including first and second wide surface interfaces, and first and second narrow edge interfaces. The core has a slow axis parallel to the first and second wide surface interfaces, and a refractive index. The fiber also includes first and second signal claddings positioned in contact with the first and second wide surfaces of the core, respectively. The first and second signal claddings have a spatial refractive index profile having: i) a minimum value at a longitudinal axis of the core, ii) a maximum value substantially equal to the refractive index of the core at the first and second narrow edge interfaces of the core, and iii) intermediate values gradually increasing from the minimum value to the maximum value as distance from the longitudinal axis increases along the slow axis of the fiber.
    • 在各种示例中,半导光纤包括具有包括第一和第二宽面接口的高纵横比的芯以及第一和第二窄边界面。 芯具有平行于第一和第二宽表面界面的慢轴和折射率。 光纤还包括分别与芯的第一和第二宽表面接触定位的第一和第二信号包层。 第一和第二信号包层具有空间折射率分布,其具有:i)芯的纵向轴线处的最小值,ii)基本上等于芯部在第一和第二窄边缘界面处的折射率的最大值 并且iii)随着距离纵轴的距离沿着光纤的慢轴增加,中间值从最小值逐渐增加到最大值。