OPTICAL MEASURING METHOD, AND OPTICAL MEASURING SYSTEM

    公开(公告)号:EP4431888A1

    公开(公告)日:2024-09-18

    申请号:EP21963334.4

    申请日:2021-11-08

    Inventor: SHIMODA, Kensaku

    CPC classification number: G03H1/04 G01B11/24 G01J9/02 G01N21/45 G03H1/08

    Abstract: An optical measurement method includes: preparing an optical system for recording a hologram caused by modulating, with a reference beam, an object beam obtained by illumination of a sample with illumination light, the reference beam being coherent to the illumination light; arranging a calibration unit on an optical path of the illumination light in a state where there is no sample, the calibration unit including an optical system that produces a known optical wave distribution; recording a first hologram caused while the calibration unit is producing an optical wave distribution; and calculating information about an optical wave distribution of the reference beam based on information indicating a position where the calibration unit is arranged, the known optical wave distribution, and the first hologram.

    COHERENT SPECTROSCOPIC METHODS WITH EXTENDED INTERROGATION TIMES AND SYSTEMS IMPLEMENTING SUCH METHODS
    4.
    发明公开
    COHERENT SPECTROSCOPIC METHODS WITH EXTENDED INTERROGATION TIMES AND SYSTEMS IMPLEMENTING SUCH METHODS 审中-公开
    具有延长穿刺时间的相干光谱学方法和实施这些方法的系统

    公开(公告)号:EP3233719A1

    公开(公告)日:2017-10-25

    申请号:EP15823154.8

    申请日:2015-12-18

    Abstract: Coherent spectroscopic methods are described, to measure the total phase difference during an extended interrogation interval between the signal delivered by a local oscillator (10) and that given by a quantum system (QS). According to one or more embodiments, the method may comprise reading out at the end of successive interrogation sub-intervals (T i ) intermediate error signals corresponding to the approximate phase difference (Õ) between the phase of the LO signal and that of the quantum system, using coherence preserving measurements; shifting at the end of each interrogation sub-intervals (T i ) the phase of the local oscillator signal, by a known correction value (Õ (i) FB ) so as to avoid that the phase difference approaches the limit of the inversion region; reading out a final phase difference (Õ f ) between the phase of the prestabilized oscillator signal and that of the quantum system using a precise measurement with no restriction on the destruction; reconstructing a total phase difference over the extended interrogation interval, as the sum of the final phase difference (Õ f ) and the opposite of all the applied phase corrections - ˆ‘ i Æ FB i .

    Abstract translation: 描述相干光谱方法,以测量在由本地振荡器(10)传送的信号与由量子系统(QS)给出的信号之间的扩展询问间隔期间的总相位差。 根据一个或多个实施例,该方法可以包括在连续询问子间隔(Ti)结束时读出对应于LO信号的相位与量子系统的相位之间的近似相位差(φ)的中间误差信号 ,使用保持相干性测量; 在每个询问子区间(Ti)结束时将本地振荡器信号的相位移动已知的校正值(φ(i)FB),以避免相位差接近反转区域的极限; 使用精确测量读出预稳定化的振荡器信号的相位与量子系统的相位之间的最终相位差(φf),而不对破坏进行限制; 将扩展询问间隔内的总相位差重建为最终相位差(φf)与所有施加的相位校正图(I)的相反之和。

    Coherent spectroscopic methods with extended interrogation times and systems implementing such
    7.
    发明公开
    Coherent spectroscopic methods with extended interrogation times and systems implementing such 审中-公开
    相干光谱方法与扩展的查询时间和系统的实施

    公开(公告)号:EP3034463A1

    公开(公告)日:2016-06-22

    申请号:EP14307085.2

    申请日:2014-12-18

    Abstract: Coherent spectroscopic methods are described, to measure the total phase difference during an extended interrogation interval between the signal delivered by a local oscillator (10) and that given by a quantum system (QS). According to one or more embodiments, the method may comprise reading out at the end of successive interrogation sub-intervals (T i ) intermediate error signals corresponding to the approximate phase difference (ϕ) between the phase of the LO signal and that of the quantum system, using coherence preserving measurements; shifting at the end of each interrogation sub-intervals (T i ) the phase of the local oscillator signal, by a known correction value (ϕ (i) FB ) so as to avoid that the phase difference approaches the limit of the inversion region; reading out a final phase difference (ϕ f ) between the phase of the prestabilized oscillator signal and that of the quantum system using a precise measurement with no restriction on the destruction; reconstructing a total phase difference over the extended interrogation interval, as the sum of the final phase difference (ϕ f ) and the opposite of all the applied phase corrections - ∑ i φ FB i .

    Abstract translation: 相干光谱方法被描述,测量在由本地振荡器(10),也由一个量子系统(QS)给定传送的信号之间的扩展间隔询问期间的总相位差。 。根据一个或多个实施方案中,所述方法可包括在所述端部中读出连续的询问的子间隔(T I)中间误差信号对应于所述LO信号的相位之间的近似相位差(O),也做了量子 系统,使用相干性测量保留; 在每个询问的子间隔(T i)所述本地振荡器信号的相位,的端部移动通过公知的修正值(O(ⅰ)FB),以便避免,DASS死相位差接近反转区域的限制; 读出振荡器信号的相位之间的最终相位差(Õf)和预稳定确实使用具有上破坏没有限制精确测量该量子系统的; 重建在扩展询问间隔总相位差,作为最终的相位差(Õf)和所有的应用相位校正的相对的总和 - “我ÆFB我。

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