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    • 2. 发明公开
    • COMPACT LITTROW-TYPE SCANNING SPECTROGRAPH
    • KOMPAKTER RASTERSPEKTROGRAPH DES LITTROW-TYPS
    • EP1451541A4
    • 2008-08-13
    • EP01988169
    • 2001-11-19
    • JOBIN YVON INC
    • JIANG WUSLUTTER WARREN STEPHENLANGE KEVIN
    • G01J3/02G01J3/22
    • G01J3/02G01J3/021G01J3/0218G01J3/0221G01J3/0243G01J3/0256G01J3/0291G01J3/22
    • A Littrow-type spectrometer or monochromator using a folded light path to provide a compact optical instrument is disclosed. Light enters the instrument through an inlet aperture on a planar mirror. The aperture is located at the focus of a parabolic collimetor mirror. Collimated light reflected by the parabolic miror is reflected back to the planar mirror, which is positioned at an angle to the collimated light. The light reflected from the planar mirror is directed at a planar grating that produces diffracted light having all the wavelengths input into the system, including light of a selected wavelength, back towards the planar mirror. Light having the selected wavelength is thus caused to fall on the parabolic mirror. The parabolic mirror then focuses the selected wavelength of light ont a light exit aperture that is juxtaposed to the inlet light aperture. The planar grating can be rotatably mounted to scan the input light spectrum.
    • 公开了一种利用折叠光路来提供紧凑型光学仪器的利特罗型分光计或单色仪。 光线通过平面镜上的入口进入仪器。 光圈位于抛物面准直镜的焦点处。 由抛物镜反射的准直光被反射回平面镜,该平面镜与平行光成一定角度。 从平面镜反射的光被导向平面光栅,该平面光栅产生具有输入到系统中的所有波长的衍射光,包括选定波长的光回到平面镜。 具有选定波长的光因此落在抛物面镜上。 抛物面反射镜然后将选定波长的光聚焦在与入射光孔并列的光出射孔上。 平面光栅可旋转安装以扫描输入光谱。
    • 4. 发明公开
    • CONVOLUTION METHOD FOR MEASURING LASER BANDWIDTH
    • 折叠式激光测量带宽方法
    • EP1417462A1
    • 2004-05-12
    • EP02752594.8
    • 2002-07-25
    • Cymer, Inc.
    • HAAS, StevenSANDSTROM, Richard, L.HOFMANN, ThomasERSHOV, Alexander, I.
    • G01J3/18
    • G01J3/26G01J1/4257G01J3/02G01J3/027G01J3/12G01J3/1809G01J3/22G01J3/28G01J9/02
    • A simple, reliable, easy to use method for calculating bandwidth data of very narrow band laser beams based on bandwidth data obtained with a spectrometer in circumstances where the laser bandwidths are not large compared to the slit function of the spectrometer. The slit function of the spectrometer is determined (20). Spectral data of the laser beam is measured with the spectrometer to produce a measured laser beam spectrum which represents a convolution of the laser beam spectrum and the spectrometer slit function (76). This measured laser spectrum is then mathematically convolved with the slit function of the spectrometer to produce a doubly convolved spectrum. Bandwidth values representing true laser bandwidths are determined from measured laser spectrum and the doubly convolved spectrum. Preferably the true laser bandwidths are calculated by determining the difference between 'twice a measured laser bandwidth' and a corresponding 'doubly convolved bandwidth.' This method provides an excellent estimate of the true laser bandwidth because 'twice the measured laser bandwidth' represents two laser bandwidths and two spectrometer slit function bandwidths and the 'doubly convolved bandwidth' represents one laser bandwidth and two spectrometer slit function bandwidths. Thus, the difference is a representation of the true laser bandwidth. In a preferred embodiment the bandwidth parameters measured are the full width half-maximum bandwidth and the 95% integral bandwidth.
    • 6. 发明公开
    • A GAS CELL
    • GASZELLE
    • EP1588148A1
    • 2005-10-26
    • EP04702475.7
    • 2004-01-15
    • Senseair AB
    • MARTIN, Hans, Göran, Evald
    • G01N21/17
    • G01N21/3504G01J3/22G01N21/314G01N2021/3137G01N2021/317
    • The present invention relates to a gas cell which is included in a gas sensor and adapted to establish the presence of a gas and/or for determining the concentration of one such gas (G), comprising a cavity (2') which is delimited by wall portions that have light reflecting properties and which is intended to enclose a volume ((G)) of said gas, and further comprising a light source (3) which is adapted to emit a light bundle (3a') directed for reflection between cavity-associated and opposing wall portions, wherein a light bundle (3a') is comprised of light rays which are reflected in a concave wall mirror surface (2b') and adapted to be directed onto one or more light receivers (4, 5) which function to detect an absorption wavelength corresponding to the gas sample ((G)). The concave curved wall mirror surface (2b') is adapted to reflect an obliquely received divergent light bundle (3a') from the light source (3) onto a flat grating-allocated cavity-associated wall surface (2g') whose reflecting surface includes or is structured as a Littrow arrangement (2g'). The light bundle (3a') is adapted to fall onto the flat wall surface (2g') at an angle which lies close to the Blaze angle of the grating wherewith, inter alia, an absorption wavelength corresponding to the chosen gas sample ((G)) and present in the light bundle (3a') is caused to be reflected and diffracted ((3a')) by said flat wall surface (2g') in a straight opposite direction so as to be reflected again in said curved mirror surface (2b') and directed diffracted towards each of said light receivers (4, 5).
    • 7. 发明公开
    • HIGH RESOLUTION SPECTRAL MEASUREMENT DEVICE
    • 高分辨率光谱测量
    • EP1485686A2
    • 2004-12-15
    • EP03744588.9
    • 2003-01-15
    • Cymer, Inc.
    • SANDSTROM, Richard, L.ERSHOV, Alexander, I.PARTLO, William, N.FOMENKOV, Igor, V.SMITH, Scott, T.BROWN, Daniel, J., W.
    • G01J3/18
    • G01J3/26G01J1/4257G01J3/02G01J3/0205G01J3/12G01J3/1804G01J3/22G01J9/02
    • A high resolution spectral measurement device. A preferred embodiment presents an extremely narrow slit function in the ultraviolet range and is very useful for measuring bandwidth of narrow-band excimer lasers used for integrated circuit lithography. Light from the laser is focused into a diffuser (D) and the diffused light exiting the diffuser (D) illuminates an etalon (ET). A portion of its light exiting the etalon (ET) is collected and directed into a slit (S1) positioned at a fringe pattern of the etalon (ET). Light passing through the slit (S1) is collimated and the collimated light illuminates a grating (GR1) positioned in an approximately Littrow configuration which disperses the light according to wavelength. A portion of the dispersed light representing the wavelength corresponding to the selected etalon fringe is passed through a second slit and monitored by a light detector. When the etalon (ET) and the grating (GR1) are tuned to the same precise wavelength a slit function is defined which is extremely narrow such as about 0.034pm (FWHM) and about 0.091pm (95 percent integral). The bandwidth of a laser beam can be measured very accurately by a directing portion of the laser beam into the insulator and scanning the laser wavelength over a range which includes the monochromator slit wavelength. In a second embodiment the second slit and the light detector is replaced by a photodiode array (PDA) and the bandwidth of a laser beam is determined by analyzing a set of scan data from the photodiode array (PDA). Alternately, the laser wavelength can be fixed near the middle of the spectrum range of the grating spectrometer (50), and the etalon (ET) can be scanned.
    • 8. 发明公开
    • ECHELLE-POLYCHROMATOR
    • SCALE-多色
    • EP0587683A1
    • 1994-03-23
    • EP92911706.0
    • 1992-06-05
    • BODENSEEWERK PERKIN-ELMER GMBH
    • FLOREK, StefanBECKER-ROSS, Helmut
    • G01J3
    • G01J3/14G01J3/1809G01J3/22G01J3/2803G01J2003/1208G01J2003/1286G01J2003/1828
    • Un premier monochromateur (14) doté d'une prisme (20) est monté à l'avant d'un polychromateur à échelle (50). La dispersion linéaire du premier monochromateur (14) est susceptible de varier lorsqu'on modifie la dispersion angulaire du prisme (20). Une position spectrale déterminée et son environnement immédiat sont analysés avec une résolution élevée, au moyen d'une grille échelle (54). Des moyens sont prévus afin que, en fonction de chacune des longueurs d'onde moyennes observées, d'une part le réseau détecteur (66) du polychromateur à échelle (50) soit totalement utilisé et, d'autre part, les perturbations soient écartées du polychromateur à échelle (50). Dans ce but, la dispersion linéaire du premier monochromateur est variable.
    • 具有棱镜(20)的第一单色仪(14)安装在梯形多色仪(50)的前面。 当修改棱镜(20)的角色散时,第一单色器(14)的线性色散很可能发生变化。 使用比例尺网格(54)以高分辨率分析确定的光谱位置及其直接环境。 设置装置,使得,取决于在一方面中观察到的检测器阵列(66),每个平均波长缩放多色仪(50)被完全使用,并且在另一方面,扰动间隔的 缩放多色仪(50)。 为此,第一单色器的线性色散是可变的。
    • 10. 发明公开
    • COMPACT LITTROW-TYPE SCANNING SPECTROGRAPH
    • 紧凑型LITTROW型扫描光谱
    • EP1451541A2
    • 2004-09-01
    • EP01988169.7
    • 2001-11-19
    • Jobin Yvon Inc.
    • JIANG, WuSLUTTER, Warren, StephenLANGE, Kevin
    • G01J1/00
    • G01J3/02G01J3/021G01J3/0218G01J3/0221G01J3/0243G01J3/0256G01J3/0291G01J3/22
    • A Littrow-type spectrometer or monochromator (10) using a folded light path to provide a compact optical instrument is disclosed. Light enters the instrument through an inlet aperture on a planar mirror (14). The aperture is located at the focus of a parabolic collimetor-mirror (18). Collimated light reflected by the parabolic mirror is reflected back to the planar mirror, which is positioned at an angle to the collimated light. The light reflected from the planar mirror is directed at a planar grating (20) that produces diffracted light having all the wavelengths input into the system, including light of a selected wavelength, back towards the planar mirror. Light having the selected wavelength is thus caused to fall on the parabolic mirror. The parabolic mirror then focuses the selected wavelength of light ont a light exit aperture that is juxtaposed to the inlet light aperture. The planar grating can be rotatably mounted to scan the input light spectrum.
    • 公开了利用折叠光路提供小型光学仪器的利特罗型分光计或单色器​​(10)。 光线通过平面镜(14)上的入口进入仪器。 光圈位于抛物面准直镜(18)的焦点处。 由抛物面镜反射的准直光被反射回平面镜,该平面镜与平行光成一定角度。 从平面镜反射的光被导向平面光栅(20),该平面光栅产生具有输入到系统中的所有波长(包括选定波长的光)的衍射光返回平面镜。 具有选定波长的光因此落在抛物面镜上。 抛物面反射镜然后将选定波长的光聚焦在与入射光孔并列的光出射孔上。 平面光栅可旋转安装以扫描输入光谱。