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    • 2. 发明授权
    • Monolithic glass light shaping diffuser and method for its production
    • 单片玻璃光成型扩散器及其生产方法
    • US06446467B1
    • 2002-09-10
    • US08902415
    • 1997-07-29
    • Robert A. LiebermanEdgar A. MendozaDavid Mintzer
    • Robert A. LiebermanEdgar A. MendozaDavid Mintzer
    • C03B802
    • G02B5/0247C03B19/12C03C1/006C03C1/008C03C4/00C03C17/007C03C17/02C03C2204/08C03C2217/213C03C2218/113C03C2218/32G02B5/0252G02B5/0268G02B5/0278G02B5/32
    • A holographic light shaping diffuser (LSD) is formed from a monolithic glass material by recording light shaping structures (sometimes collectively known as “speckle”, particularly when the structures extend into the interior of the diffuser) in the glass material during its formation. A volume LSD may be produced by the photolithographic writing or other imaging of light shaping structures in a photosensitive glass material. Alternatively, a surface LSD may be produced by this imaging process or by embossing light shaping structures onto a high quality optical glass or by embossing a light shaping structures on a glass film layer coated onto a substrate. Both types of diffusers control the angular spread of transmitted light while homogenizing otherwise spatially noisy light sources such as LCDs and filamented light sources and while maintaining damage thresholds consistent with any glass optical element. The LSD has a transmission efficiency of over 90% from the Ultraviolet wavelengths through the physical spectrum and into the near-infrared. Moreover, because the LSD is a true glass, it is capable of withstanding temperatures well beyond glass transition temperatures of plastic LSDs, can be formed in a convex or concave surfaces through conventional molding, grinding, or polishing techniques, and can be coated by hot-coating techniques. The LSD also has a very high laser power threshold.
    • 通过记录光形成结构(有时统称为“斑点”,特别是当结构延伸到扩散器的内部时),通过记录光成形结构(玻璃材料)形成全息光成形扩散器(LSD)。 可以通过感光玻璃材料中的光成形结构的光刻书写或其他成像来产生体积LSD。 或者,可以通过该成像处理或通过将光成形结构压印到高质量光学玻璃上或通过在涂覆在基板上的玻璃膜层上压花光成形结构来制造表面LSD。 两种类型的扩散器控制透射光的角度扩展,同时均匀化否则为空间有噪声的光源,例如LCD和光纤光源,同时保持与任何玻璃光学元件一致的损伤阈值。 LSD的透射效率超过紫外线波长通过物理光谱和近红外光的90%以上。 此外,由于LSD是真正的玻璃,它能够承受超过塑料LSD的玻璃化转变温度的温度,可以通过常规的成型,研磨或抛光技术在凸面或凹面中形成,并可通过热涂层 涂层技术。 LSD还具有非常高的激光功率阈值。
    • 8. 发明授权
    • Modular fiber optic fluorometer and method of use thereof
    • 模块化光纤荧光计及其使用方法
    • US5994707A
    • 1999-11-30
    • US819050
    • 1997-03-18
    • Edgar A. MendozaJames E. SorensonRobert A. LiebermanThomas C. Forrester
    • Edgar A. MendozaJames E. SorensonRobert A. LiebermanThomas C. Forrester
    • G01N21/64
    • G01N21/645G01N2021/6419G01N2021/6421G01N2021/6484G01N2201/0221G01N2201/0245G01N2201/086
    • A low cost portable fiber optic fluorometer is packaged as a personal computer peripheral and is based on interchangeable modules. One embodiment of the fluorometer comprises an excitation source, a detector, a signal processor, frequency source, wavelength selector, and an optical interface. The optical interface is exclusively fiber optic-based, thereby simplifying optical alignment and reducing the cost of the fluorometer. In another embodiment, the excitation source is an inexpensive monochromatic excitation source. In this case, the monochromatic excitation source and the first wavelength selector are preferably removable and replaceable, so that the fluorometer is advantageously able to generate different excitation wavelengths and detect different emission wavelengths. A fluorescence measurement method comprises the steps of generating an excitation signal; transmitting the excitation signal to a system under study which, in response, generates an emission signal; and detecting both the excitation signal and the emission signal with the fluorometer, and then using the detected excitation signal as a reference signal to calibrate the fluorometer and to nullify distortion errors in the emission signal. The use of the excitation signal as a reference signal provides an advantageously simple way to calibrate the fluorometer and to nullify distortion errors in the emission signal. An alternative method allows the precise shapes of the emission signal and the excitation signal to be profiled. The fluorometry method and apparatus can both advantageously be used for performing both direct fluorescence lifetime measurements and for performing phase fluorometry.
    • 低成本便携式光纤荧光计作为个人计算机外围设备封装,并且基于可互换的模块。 荧光计的一个实施例包括激发源,检测器,信号处理器,频率源,波长选择器和光学接口。 光接口仅仅是基于光纤的,从而简化了光学对准并降低了荧光计的成本。 在另一个实施例中,激发源是便宜的单色激发源。 在这种情况下,单色激发源和第一波长选择器优选是可移除和可更换的,使得荧光计有利地能够产生不同的激发波长并检测不同的发射波长。 荧光测量方法包括产生激励信号的步骤; 将激励信号传输到被研究的系统,其响应地产生发射信号; 并用荧光计检测激发信号和发射信号,然后使用检测到的激发信号作为参考信号来校准荧光计,并消除发射信号中的失真误差。 使用激励信号作为参考信号提供校准荧光计并消除发射信号中的失真误差的有利的简单方式。 替代方法允许对发射信号和激励信号的精确形状进行轮廓分析。 荧光测定方法和装置可以有利地用于进行直接荧光寿命测量和用于进行相位荧光测定。
    • 9. 发明授权
    • Method and system for determining the wavelength of light transmitted
through an optical fiber
    • 用于确定透过光纤的光的波长的方法和系统
    • US6052179A
    • 2000-04-18
    • US59739
    • 1998-04-14
    • John D. ProhaskaLothar U. KempenRobert A. Lieberman
    • John D. ProhaskaLothar U. KempenRobert A. Lieberman
    • G01B9/02G01D5/353
    • G01D5/35335G01D5/35316
    • A method of determining the wavelength of light transmitted in an optical fiber comprises the steps of filtering the light using a filter, and then detecting the filtered light, and then determining the wavelength of the filtered light. The filter comprises a fiber grating which is recorded in a portion of the optical fiber. The fiber grating preferably has a modulated index of refraction with a modulation amplitude that varies from a first end to a second end of the fiber grating, and a modulation period defined by a grating constant that varies from the first end to the second end of the fiber grating. The fiber grating at least partially prevents transmission of light within a wavelength spectrum, and prevents transmission of a substantially larger portion of the light at a first end of the wavelength spectrum than at a second end of the wavelength spectrum. Therefore, the wavelength of the filtered light can be determined by determining a proportion of the light which was transmitted by the filter. The proportion of light which is transmitted by the filter is preferably linearly related to the wavelength of the light.
    • 确定在光纤中传输的光的波长的方法包括以下步骤:使用滤光片对光进行滤光,然后检测滤光,然后确定滤光的波长。 滤光器包括记录在光纤的一部分中的光纤光栅。 光纤光栅优选地具有从光纤光栅的第一端到第二端变化的调制幅度的调制折射率,以及由光栅常数变化的调制周期,该调制周期从第一端到第二端变化 光纤光栅。 光纤光栅至少部分地防止波长光谱中的光的透射,并且防止在波长光谱的第一端处的光的实质上较大部分的光在波长光谱的第二端的透射。 因此,可以通过确定由滤光器透射的光的比例来确定滤光光的波长。 由滤光器透射的光的比例优选与光的波长成线性关系。