Polarization state measuring apparatus
    231.
    发明公开
    Polarization state measuring apparatus 审中-公开
    Vorrichtung zur Messung des Polarisationszustandes

    公开(公告)号:EP1596172A2

    公开(公告)日:2005-11-16

    申请号:EP04022711.8

    申请日:2004-09-23

    Inventor: Kubo, Teruhiro

    CPC classification number: G01J4/04

    Abstract: A polarization state measuring apparatus of the present invention branches an input signal light into a plurality of signal lights by optical couplers, gives polarization and phase shift which are different from each other, to the signal lights by a plurality of optical elements arranged on optical branch paths, detects the power of each of the signal lights by the corresponding light receiving elements, and after adjusting at least differences in the optical branch paths, processes electrical signals output from the light receiving elements by operating means, to acquire information related to a polarization state of the input signal light. As a result, it is possible to provide a small size polarization state measuring apparatus which can correct differences in arrival times of the signal lights to the light receiving elements, which occur due to differences in the optical path lengths of the plurality of optical branch paths, to thereby measure the polarization state of the input signal light with high accuracy.

    Abstract translation: 本发明的偏振状态测量装置通过光耦合器将输入信号光分支成多个信号光,通过布置在光分支上的多个光学元件将信号光分别彼此不同的极化和相移 通过相应的光接收元件检测每个信号光的功率,并且在调整至少光分支路径的差异之后,通过操作装置处理从光接收元件输出的电信号,以获取与偏振相关的信息 输入信号灯的状态。 结果,可以提供一种小尺寸偏振状态测量装置,其可以校正由于多个光分支路径的光路长度的差异而导致的信号光到达光接收元件的到达时间的差异 ,从而以高精度测量输入信号光的偏振状态。

    POLARIZATION CONVERSION UNIT FOR REDUCING POLARIZATION DEPENDENT MEASUREMENT ERRORS
    233.
    发明公开
    POLARIZATION CONVERSION UNIT FOR REDUCING POLARIZATION DEPENDENT MEASUREMENT ERRORS 审中-公开
    偏振转换单元用于减少POLARISATIONSABHûNGIGEN测量误差

    公开(公告)号:EP1558902A1

    公开(公告)日:2005-08-03

    申请号:EP02808047.1

    申请日:2002-10-25

    CPC classification number: G01J4/00 G01J4/04

    Abstract: A first optical signal with a first polarization state is received by a polarization conversion unit. From this first optical signal, a set of n derived optical signals with n different well-defined polarization states i, i = 1, ..., n, is generated, whereby n is a natural number greater than one. Said n different well-defined polarization states are chosen such that polarization dependent measurement errors of the n derived optical signals cancel each other when averaged irrespective of the first optical signal's polarization state. Therefore, polarization dependent measurement errors can be reduced or even eliminated.

    BIREFRINGENCE MEASUREMENT AT DEEP-ULTRAVIOLET WAVELENGTHS
    234.
    发明公开
    BIREFRINGENCE MEASUREMENT AT DEEP-ULTRAVIOLET WAVELENGTHS 有权
    双断用于测量波长的远紫外线

    公开(公告)号:EP1397651A4

    公开(公告)日:2005-06-22

    申请号:EP02744424

    申请日:2002-06-17

    Abstract: Provided are systems and methods for precisely measuring birefringence properties of optical elements, especially those elements that are used in deep ultraviolet (DUV) wavelengths. The system includes two photoelastic modulators (PEM) (126, 128) located on opposite sides of the sample (136). Each PEM is operable for modulating the polarity of a light beam that passes though the sample. The system also includes a polarizer (124) associated with one PEM, an analyzer (130) associated with the other PEM, and a detector (132) for measuring the intensity of the light after it passes through the PEMs, polarizer, and analyzer. Described are techniques for determining birefringence properties across a wide range. For example, a dual-wavelength source light embodiment is provided for measuring relatively high levels of birefringence. Also provided is technique for selecting the most accurate and efficient one of a number of approaches to determining birefringence properties depending upon the estimated value of the birefringence to be detected for a given sample optical element.

    BIREFRINGENCE MEASUREMENT SYSTEM
    235.
    发明公开
    BIREFRINGENCE MEASUREMENT SYSTEM 审中-公开
    法测量双边BREAK

    公开(公告)号:EP1060369A4

    公开(公告)日:2005-01-19

    申请号:EP99934336

    申请日:1999-02-17

    CPC classification number: G01J4/04 G01N21/23

    Abstract: A practical system and method for precisely measuring low-level birefrigence properties (retardance and fast axis orientation) of optical materials (26). The system permits multiple measurements to be taken across the area of a sample to detect and graphically display (100) variations in the birefrigence properties across the sample area. In a preferred embodiment, the system incorporates a photoelastic modulator (24) for modulating polarized light that is then directed through a sample (26). The beam ('Bi') propagating from the sample is separated into two parts, with one part ('B1') having a polarization direction different than the polarization direction of the other beam part ('B2'). These separate beam parts are then processed as distinct channels. Detection mechanisms (32, 50) associated with each channel detect the time varying light intensity corresponding to each of the two parts of the beam. This information is combined for calculating a precise measure of the retardance induced by the sample, as well as the sample's fast axis orientation.

    IMAGING SPECTROMETER
    236.
    发明公开
    IMAGING SPECTROMETER 有权
    IMAGE管辖谱仪

    公开(公告)号:EP1495293A1

    公开(公告)日:2005-01-12

    申请号:EP03718940.4

    申请日:2003-04-15

    CPC classification number: G01J4/04 G01J3/2823 G01J3/447 G01J3/51

    Abstract: An imaging spectrometer (2) is disclosed that comprises imaging means for dividing a received image into two or more spatially separated spectral images and means for detecting each spectral image (4), and is characterised in that the imaging means comprises at least one polarising beam splitter (18, 20, 22; 64, 68, 72). The polarising beam splitter may be a Wollaston prism. In one embodiment of the invention, the imaging means comprises image replication means (12) to produce two or more spatially separated images, and one or more filter elements such as dichroic filters (8) which act to alter the spectral characteristics of one or more of the spatially separated images. In a further embodiment of the invention the imaging means comprises one or more spectral replication means arranged in optical series, each spectral replication means comprising an optical retardation element (62, 66, 70) and a polarising beam splitter (64, 68, 72).

    POLARIZATION BEARING DETECTION TYPE TWO-DIMENSIONAL LIGHT RECEPTION TIMING DETECTING DEVICE AND SURFACE SHAPE MEASURING DEVICE USING IT
    237.
    发明公开
    POLARIZATION BEARING DETECTION TYPE TWO-DIMENSIONAL LIGHT RECEPTION TIMING DETECTING DEVICE AND SURFACE SHAPE MEASURING DEVICE USING IT 审中-公开
    ZWEIDIMENSIONALE LICHTEMPFANGS-TIMINGDETEKTIONSEINRICHTUNG DES POLARISATIONSLAGEDETEKTIONSTYPS UND OBFLOWCHEMFORMESSEINRICHTUNG DAMIT

    公开(公告)号:EP1482273A1

    公开(公告)日:2004-12-01

    申请号:EP03707195.8

    申请日:2003-03-03

    CPC classification number: G01B11/25 G01B11/24 G01J4/04

    Abstract: A polarization bearing detection type two-dimensional light reception timing detecting device for implementing a fast surface shape measurement that can accommodate an animal body measurement, and a surface shape measuring device using it. In Fig.8, the polarization bearing of a detection light is turned in synchronization with slit light scanning, and the polarization bearing is two-dimensionally recorded by two sets of analyzers (5, 6) and storage type image detectors in a crossed Nicols arrangement, thereby it is possible to determine, with only one-time imaging, timing at which a slit light is beamed into respected pixels in the storage type image detectors (7,8).

    Abstract translation: 偏振轴承的检测光与狭缝光扫描同步,以便使用正交尼科尔布置的一对分析器(5,6)和存储型图像检测器(7,8)二维地记录偏振轴承。 还包括表面形状测量装置的独立权利要求。

    BIREFRINGENCE MEASUREMENT AT DEEP-ULTRAVIOLET WAVELENGTHS
    238.
    发明公开
    BIREFRINGENCE MEASUREMENT AT DEEP-ULTRAVIOLET WAVELENGTHS 有权
    双断用于测量波长的远紫外线

    公开(公告)号:EP1397651A1

    公开(公告)日:2004-03-17

    申请号:EP02744424.9

    申请日:2002-06-17

    Abstract: Provided are systems and methods for precisely measuring birefringence properties of optical elements, especially those elements that are used in deep ultraviolet (DUV) wavelengths. The system includes two photoelastic modulators (PEM) (126, 128) located on opposite sides of the sample (136). Each PEM is operable for modulating the polarity of a light beam that passes though the sample. The system also includes a polarizer (124) associated with one PEM, an analyzer (130) associated with the other PEM, and a detector (132) for measuring the intensity of the light after it passes through the PEMs, polarizer, and analyzer. Described are techniques for determining birefringence properties across a wide range. For example, a dual-wavelength source light embodiment is provided for measuring relatively high levels of birefringence. Also provided is technique for selecting the most accurate and efficient one of a number of approaches to determining birefringence properties depending upon the estimated value of the birefringence to be detected for a given sample optical element.

    PARALLEL DETECTING, SPECTROSCOPIC ELLIPSOMETERS/POLARIMETERS
    240.
    发明公开
    PARALLEL DETECTING, SPECTROSCOPIC ELLIPSOMETERS/POLARIMETERS 审中-公开
    平行检测仪

    公开(公告)号:EP1218707A1

    公开(公告)日:2002-07-03

    申请号:EP00950757.5

    申请日:2000-07-27

    CPC classification number: G01J4/04 G01J3/447 G01J4/00 G01N21/211

    Abstract: The parallel detecting spectroscopic ellipsometer/polarimeter sensor (10) has no moving parts and operates in real-time for in-situ monitoring of the thin film surface properties of a sample (22) within a processing chamber. It includes a multi-spectral source of radiation (12) for producing a collimated beam of radiation (14) directed towards the surface of the sample through a polarizer (16). The thus polarized collimated beam of radiation impacts and is reflected from the surface of the sample (22), thereby changing its polarization state due to the intrinsic material properties of the sample (22). The light reflected from the sample (22) is separated into four separate polarized filtered beams (36, 38, 58, 62), each having individual spectral intensities. Data about said four individual spectral intensities is collected within the processing chamber, and is transmitted into one or more spectrometers. The data of all four individual spectral intensities is then analyzed using transformation algorithms, in real-time.

Patent Agency Ranking