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    • 1. 发明申请
    • CRITICAL ANGLE OPTICAL SENSOR APPARATUS
    • 关键角度光学传感器装置
    • US20130214138A1
    • 2013-08-22
    • US13401765
    • 2012-02-21
    • Ronald ChiarelloShad PiersonChristopher WacinskiMark ArboreYevgeny Anoikin
    • Ronald ChiarelloShad PiersonChristopher WacinskiMark ArboreYevgeny Anoikin
    • G01J1/04G01J1/42
    • G01N21/431G01N21/553G01N2021/434G01N2021/437
    • An optical sensor apparatus includes an optically transmissive structure having planar first, second, and third faces, two or more light sources located outside the structure adjacent the first face, and a photodetector array located outside the prism adjacent the first face. The structure, light sources, and photodetector array are configured such that light from the light sources that is totally internally reflected at an optical interface between the prism and a sample outside the structure proximate the second face is reflected at the third face and incident on a portion of the photodetector array that depends on a refractive index of the sample. The light sources are positioned with respect to the structure and photodetector array such that the totally internally reflected light from each light source corresponds to a different range of refractive index of the sample and maps to a corresponding portion of the photodetector array.
    • 一种光学传感器装置包括具有平面的第一,第二和第三面的光学透射结构,位于与第一面相邻的结构外的两个或更多个光源,以及位于邻近第一面的棱镜外部的光电检测器阵列。 结构,光源和光电检测器阵列被配置为使得来自光源的光在棱镜和靠近第二面的结构外部的光学界面处被内部反射的光在第三面处被反射并且入射到 光电检测器阵列的部分取决于样品的折射率。 光源相对于结构和光电检测器阵列定位,使得来自每个光源的全内部反射光对应于样品的不同折射率范围并且映射到光电检测器阵列的相应部分。
    • 2. 发明授权
    • Optical sensor apparatus to detect light based on the refractive index of a sample
    • 基于样品的折射率检测光的光学传感器装置
    • US09024252B2
    • 2015-05-05
    • US13401765
    • 2012-02-21
    • Ronald ChiarelloShad PiersonChristopher WacinskiMark ArboreYevgeny Anoikin
    • Ronald ChiarelloShad PiersonChristopher WacinskiMark ArboreYevgeny Anoikin
    • H01J5/02G01N21/43
    • G01N21/431G01N21/553G01N2021/434G01N2021/437
    • An optical sensor apparatus includes an optically transmissive structure having planar first, second, and third faces, two or more light sources located outside the structure adjacent the first face, and a photodetector array located outside the prism adjacent the first face. The structure, light sources, and photodetector array are configured such that light from the light sources that is totally internally reflected at an optical interface between the prism and a sample outside the structure proximate the second face is reflected at the third face and incident on a portion of the photodetector array that depends on a refractive index of the sample. The light sources are positioned with respect to the structure and photodetector array such that the totally internally reflected light from each light source corresponds to a different range of refractive index of the sample and maps to a corresponding portion of the photodetector array.
    • 一种光学传感器装置包括具有平面的第一,第二和第三面的光学透射结构,位于与第一面相邻的结构外的两个或更多个光源,以及位于邻近第一面的棱镜外部的光电检测器阵列。 结构,光源和光电检测器阵列被配置为使得来自光源的光在棱镜和靠近第二面的结构外部的光学界面处被内部反射的光在第三面处被反射并且入射到 光电检测器阵列的部分取决于样品的折射率。 光源相对于结构和光电检测器阵列定位,使得来自每个光源的全内部反射光对应于样品的不同折射率范围并且映射到光电检测器阵列的相应部分。
    • 3. 发明申请
    • Wavelength combining using a arrayed waveguide grating having a switchable output
    • 使用具有可切换输出的阵列波导光栅的波长组合
    • US20080025350A1
    • 2008-01-31
    • US11904775
    • 2007-09-27
    • Mark ArboreGregory Miller
    • Mark ArboreGregory Miller
    • H01S3/10G02B6/26
    • G02B6/12033G02B6/12011G02B6/12019
    • Switchable power combining is provided using a tunable arrayed waveguide grating (AWG) as the combining element. The AWG has two or more inputs and two or more outputs. Each AWG input is bi-directionally coupled to a corresponding laser source, and each laser source has substantially the same gain spectrum. All sources are coupled to a selected one of the AWG outputs, without substantial coupling of the sources to any other AWG output. The AWG is tunable, such that any one of its outputs can be thus selected. The selected output provides optical feedback, thereby feedback stabilizing the emission wavelengths of the sources to values suitable for single-mode combining. According to a further aspect of the invention, a piezo-electrically tunable AWG is provided. The AWG has a piezo-electric transducer bonded to the waveguide array section of the AWG. Strain induced in the waveguide array by the transducer can alter optical path lengths of the waveguide, thereby tuning the AWG.
    • 使用可调阵列波导光栅(AWG)作为组合元件提供可切换功率组合。 AWG具有两个或更多个输入和两个或更多个输出。 每个AWG输入双向耦合到相应的激光源,并且每个激光源具有基本相同的增益光谱。 所有的源都耦合到选定的一个AWG输出,而不需要将源与任何其他AWG输出实质耦合。 AWG是可调谐的,使得可以选择其任一输出。 所选择的输出提供光学反馈,从而将源的发射波长的反馈稳定到适合于单模组合的值。 根据本发明的另一方面,提供了一种压电可调AWG。 AWG具有一个压电换能器,它连接到AWG的波导阵列部分。 通过传感器在波导阵列中感应的应变可以改变波导的光路长度,从而调谐AWG。
    • 5. 发明授权
    • Quasi-monolithic tunable optical resonator
    • 准单片可调谐光谐振器
    • US06654392B1
    • 2003-11-25
    • US09494747
    • 2000-01-31
    • Mark ArboreFrancisc Tapos
    • Mark ArboreFrancisc Tapos
    • H01S310
    • H01S3/025G02F2001/3542H01S3/0627H01S3/0816H01S3/083H01S3/105H01S3/131H01S3/1317
    • An optical resonator has a piezoelectric element attached to a quasi-monolithic structure. The quasi-monolithic structure defines an optical path. Mirrors attached to the structure deflect light along the optical path. The piezoelectric element controllably strains the quasi-monolithic structure to change a length of the optical path by about 1 micron. A first feedback loop coupled to the piezoelectric element provides fine control over the cavity length. The resonator may include a thermally actuated spacer attached to the cavity and a mirror attached to the spacer. The thermally actuated spacer adjusts the cavity length by up to about 20 microns. A second feedback loop coupled to the sensor and heater provides a “coarse” control over the cavity length. An alternative embodiment provides a quasi-monolithic optical parametric oscillator (OPO). This embodiment includes a non-linear optical element within the resonator cavity along the optical path. Such an OPO configuration is broadly tunable and capable of mode-hop free operation for periods of 24 hours or more.
    • 光学谐振器具有附接到准整体结构的压电元件。 准单片结构限定了光路。 附接到结构的镜子沿光路偏转光。 压电元件可控地应变准单片结构以将光路的长度改变约1微米。 耦合到压电元件的第一反馈环路提供对腔体长度的精细控制。 谐振器可以包括附接到空腔的热致动间隔件和附接到间隔件的反射镜。 热驱动间隔件将空腔长度调节高达约20微米。 耦合到传感器和加热器的第二反馈回路提供对腔长度的“粗略”控制。 另一实施例提供准单片光学参量振荡器(OPO)。 该实施例包括沿着光路在谐振腔内的非线性光学元件。 这样的OPO配置是广泛可调谐的,并且能够在24小时或更长时间内无模式跳跃操作。
    • 6. 发明申请
    • Laser burst boosting method and apparatus
    • 激光脉冲升压方法和装置
    • US20060018350A1
    • 2006-01-26
    • US10896641
    • 2004-07-20
    • Frank AdamsMark ArboreWerner Wiechmann
    • Frank AdamsMark ArboreWerner Wiechmann
    • H01S3/04
    • H01S3/109H01S3/08072H01S3/094076H01S3/0941H01S3/1024H01S3/1028H01S5/06216H01S5/0622
    • Methods and apparatus for managing thermal loads on a laser gain medium and for boosting the output power of a diode pumped laser are disclosed. The short-term average pumping power to the gain medium is increased, to provide a burst of pumping energy to the laser gain medium. A subsequent short-term reduction in the average pumping power then allows the gain medium to cool to a desired state steady level. The average pumping power is then increased to maintain this steady state level until the next burst is desired. For example, a pulse of current may be applied to a laser diode at a first current level I1 for a first time interval Δt1, where I1 exceeds a nominal current value Inom by an amount ΔI1. The current to the laser diode is reduced to a second current level I2 for a second time interval Δt2, where Inom exceeds I2 by an amount ΔI2. To balance the thermal load on the diode an integral of ΔI1 over the time Δt1 is approximately equal in magnitude to an integral of ΔI2 over the time Δt2. After applying the pulse of current at the first current level I1, and before or after reducing the current to the second level I2, the nominal current is applied to the laser diode for a third time interval Δt3.
    • 公开了用于管理激光增益介质上的热负荷并用于提高二极管泵浦激光器的输出功率的方法和装置。 对增益介质的短期平均泵送功率增加,以向激光增益介质提供脉冲泵浦能量。 随后的平均泵浦功率的短期减少然后允许增益介质冷却到期望的状态稳定水平。 然后增加平均泵浦功率以保持该稳定状态水平,直到需要下一个爆发。 例如,电流脉冲可以在第一时间间隔Deltat 1 <1> 1处以第一电流电平I 1 1施加到激光二极管,其中I 1 < / SUB>超过额定电流值I> nom 一个数量ΔI1 <1。 在第二时间间隔Deltat2 <2>中,到激光二极管的电流减小到第二电流电平I 2 2,其中I>超过I < SUB> 2 数量ΔI2 2。 为了平衡二极管上的热负载,在时间上的ΔI1&lt; 1&lt; 1&lt; 1&lt; 1&lt; 1&lt; 1&lt; 1&lt; 1&lt; 1&gt;之间的积分大致等于DeltaI 2& 当时Deltat 2 。 在将电流施加到第一电流I I 1之后,并且在将电流减小到第二电平I 2 2之前或之后,将标称电流施加到激光器 二极管第三时间间隔Deltat 3