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    • 4. 发明申请
    • Optical Coherence Tomography Control Systems and Methods
    • 光学相干断层扫描控制系统与方法
    • US20140218742A1
    • 2014-08-07
    • US14160939
    • 2014-01-22
    • Desmond Adler
    • Desmond Adler
    • G01B9/02
    • G01B9/02091A61B5/0066A61B5/0084G01B9/02004G01B9/02067H01S3/0092H01S3/1062H01S3/1396H01S5/183
    • In part, the invention relates to methods, devices, and systems suitable for controlling a light source. The light source is configured for use in a data collection system such as an optical coherence tomography system. The light source can be controlled with a drive waveform. Linearizing and symmetrizing parameters of the light source such as forward and backward scan durations is achieved using a suitable drive waveform. Phase, amplitude, and other parameters for different harmonics of a fundamental wave can be identified that improve operating parameters such as the duty cycle and peak frequency matching between scans. The fundamental wave and one or more of such harmonics can be combined to generate the suitable drive wave form. The light source can include a tunable light source that includes or is in optical communication with a tunable filter.
    • 部分地,本发明涉及适于控制光源的方法,装置和系统。 光源被配置用于诸如光学相干断层摄影系统的数据采集系统中。 光源可以用驱动波形控制。 使用合适的驱动波形实现光源的线性化和对称性参数,如前进和后退扫描持续时间。 可以确定基波不同谐波的相位,幅度和其他参数,以提高扫描之间的占空比和峰值频率匹配等工作参数。 基波和这些谐波中的一个或多个可以组合以产生合适的驱动波形。 光源可以包括可调谐光源,其包括或者与可调谐滤光器光学通信。
    • 5. 发明授权
    • Frequency stabilized laser system
    • 频率稳定的激光系统
    • US06434176B1
    • 2002-08-13
    • US09245170
    • 1999-02-05
    • Leslie Ludwig Deck
    • Leslie Ludwig Deck
    • H01S313
    • H01S3/1396G01B9/02007G01B2290/70H01S3/139H01S3/2222
    • The invention features a frequency stabilized laser system including a laser source, a first detector, a second detectors, and a circuit. The laser source has an adjustable cavity length and, during operation, produces a control beam including two frequency components having different polarizations. The first detector absorbs a portion of the control beam, reflects the remaining portion of the control beam, and generates a first signal proportional to the intensity of the absorbed portion of the control beam. The second detector absorbs a portion of the reflected beam and generates a second signal proportional to the intensity of the absorbed portion of the reflected beam. The circuit receives the first and second signals from the detectors and generates a control signal based on the first and second signals that controls the adjustable cavity length of the laser source. The frequency stabilized laser system can be used in interferometry applications or any other application in which frequency stability is beneficial.
    • 本发明的特征在于包括激光源,第一检测器,第二检测器和电路的频率稳定的激光系统。 激光源具有可调节的腔长度,并且在操作期间产生包括具有不同偏振的两个频率分量的控制波束。 第一检测器吸收控制光束的一部分,反射控制光束的剩余部分,并产生与控制光束的吸收部分的强度成比例的第一信号。 第二检测器吸收反射光束的一部分并产生与反射光束的吸收部分的强度成比例的第二信号。 电路从检测器接收第一和第二信号,并且基于控制激光源的可调节腔长度的第一和第二信号产生控制信号。 频率稳定的激光系统可用于干涉测量应用或频率稳定性有益的任何其他应用中。
    • 6. 发明授权
    • Harmonically mode-locked laser
    • 谐振锁模激光
    • US5274659A
    • 1993-12-28
    • US860526
    • 1992-03-30
    • George T. HarveyLinn F. Mollenauer
    • George T. HarveyLinn F. Mollenauer
    • H01S3/07H01S3/06H01S3/067H01S3/083H01S3/098H01S3/106H01S3/139H01S3/10
    • H01S3/06791H01S3/082H01S3/1396H01S3/1062H01S3/1109H01S3/1121H01S3/1305
    • In a harmonically mode-locked laser, first (33) and second (34) optical beams are derived from the laser optical path which are directed, respectively, through first and second optical filters (37) having optical pass-bands (40, 41) that are displaced in frequency but which intersect at approximately the center frequency (f.sub.c) of operation of the laser. The free spectral range of a Fabry-Perot optical resonator (24) in the laser ring is deviated from a frequency exactly equal to the pulse repetition rate of the laser by a frequency (df) sufficient to permit changes in the length of the optical path to be manifested as changes in the wavelength of light transmitted along the optical path. Apparatus (39, 40, 42) for detecting the difference of intensity of light passing through the first and second filters can then be used to generate a signal proportional to the difference of intensity of such light for the purpose of adjusting, by length adjusting apparatus (43), the length of the optical path to compensate for spurious temperature-induced length variations.
    • 在谐振锁模激光器中,第一(33)和第二(34)光束从激光光路导出,分别通过具有光通带(40,41)的第一和第二滤光器(37) ),其在频率上移位,但是在激光器的操作的近似中心频率(fc)处相交。 激光环中的法布里 - 珀罗光学谐振器(24)的自由光谱范围偏离与激光器的脉冲重复频率完全相同的频率,频率(df)足以允许光路长度的变化 被表现为沿着光路传输的光的波长的变化。 用于检测通过第一和第二滤波器的光的强度差的装置(39,40,42)可用于产生与这种光的强度差成比例的信号,以便通过长度调节装置 (43),光路的长度以补偿杂散温度引起的长度变化。
    • 7. 发明授权
    • Frequency stabilized gas laser
    • 频率稳定气体激光器
    • US3889207A
    • 1975-06-10
    • US35775273
    • 1973-05-07
    • HEWLETT PACKARD CO
    • GLENN M BURGWALDWILLIAM P KRUGERDONALD L HAMMOND
    • H01S3/032H01S3/034H01S3/038H01S3/139H01S3/10H01S3/22
    • H01S3/139H01S3/0323H01S3/034H01S3/038H01S3/1396
    • A rod made of an insulating material having a thermal coefficient of expansion in the range from +1 to -1 part in 107 per degree centigrade is mounted between a pair of mirrors and hermetically sealed either within a glass or a stainless steel enclosure containing a gas discharge medium. The stainless steel enclosure may be clamped to and fixedly spaced from the rod by projections formed on the enclosure and symmetrically disposed around the rod toward the ends of the rod. The mirrors and an annular piezoelectric disc positioned within the enclosure between one of the mirrors and one end of the rod are axially mechanically biased against the ends of the rod either by a spring loading structure or by a gas pressure differential. An anode and an annular cathode electrically insulated from one another for operation at different potentials are mounted toward the opposite ends of the rod. A discharge path communicating with the gas discharge medium and including a portion of a bore axially extending through the rod is provided in the rod between and in communication with the anode and the cathode to provide a gas discharge for excitation of the gas discharge medium to produce a laser beam. This discharge path may be placed in a magnetic field having a component in the direction of the laser beam to Zeeman split the atomic transition line at which the laser action occurs so that the laser oscillates at two different frequencies and thereby produces an output beam with two components of different frequency and polarization. In response to a portion of the laser beam a feedback control circuit changes the thickness of the piezoelectric disc to maintain the spacing between the mirrors as required, for example, to stablize the frequency, or frequencies, of oscillation of the laser at or in a known relationship to the center of the atomic transition line at which the laser action occurs.
    • 由绝缘材料制成的棒材,其热膨胀系数从+1到-1部分在107度/摄氏度之间安装在一对反射镜之间,并被密封在玻璃或含有气体的不锈钢外壳内 放电介质。 不锈钢外壳可以通过形成在外壳上的突起夹紧并与杆固定隔开,并且朝向杆的端部对称地设置在杆周围。 反射镜和位于其中一个反射镜和杆的一端之间的壳体内的环形压电盘通过弹簧加载结构或通过气体压力差轴向机械地偏置抵靠杆的端部。 将电极彼此电绝缘以在不同电位下操作的阳极和环形阴极朝向杆的相对端安装。 与气体放电介质连通并且包括轴向延伸通过杆的孔的一部分的排放路径设置在杆中并且与阳极和阴极连通并提供气体放电,用于激发气体放电介质以产生 激光束。 该放电路径可以被放置在具有激光束方向上的分量的磁场中,塞曼分裂发生激光作用的原子转移线,使得激光器以两个不同的频率振荡,从而产生具有两个的输出光束 不同频率和极化的分量。 响应于激光束的一部分,反馈控制电路根据需要改变压电盘的厚度以保持反射镜之间的间隔,例如,以稳定激光器的振荡或频率的频率或频率 与发生激光作用的原子跃迁线的中心的已知关系。
    • 9. 发明授权
    • Optical coherence tomography control systems and methods
    • 光学相干断层扫描控制系统和方法
    • US09417052B2
    • 2016-08-16
    • US14160939
    • 2014-01-22
    • Desmond Adler
    • Desmond Adler
    • G01B11/02G01B9/02A61B5/00H01S3/106H01S3/139H01S5/183H01S3/00
    • G01B9/02091A61B5/0066A61B5/0084G01B9/02004G01B9/02067H01S3/0092H01S3/1062H01S3/1396H01S5/183
    • In part, the invention relates to methods, devices, and systems suitable for controlling a light source. The light source is configured for use in a data collection system such as an optical coherence tomography system. The light source can be controlled with a drive waveform. Linearizing and symmetrizing parameters of the light source such as forward and backward scan durations is achieved using a suitable drive waveform. Phase, amplitude, and other parameters for different harmonics of a fundamental wave can be identified that improve operating parameters such as the duty cycle and peak frequency matching between scans. The fundamental wave and one or more of such harmonics can be combined to generate the suitable drive wave form. The light source can include a tunable light source that includes or is in optical communication with a tunable filter.
    • 部分地,本发明涉及适于控制光源的方法,装置和系统。 光源被配置用于诸如光学相干断层摄影系统的数据采集系统中。 光源可以用驱动波形控制。 使用合适的驱动波形实现光源的线性化和对称性参数,如前进和后退扫描持续时间。 可以确定基波不同谐波的相位,幅度和其他参数,以提高扫描之间的占空比和峰值频率匹配等工作参数。 基波和这些谐波中的一个或多个可以组合以产生合适的驱动波形。 光源可以包括可调谐光源,其包括或者与可调谐滤光器光学通信。