会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 1. 发明公开
    • Interferometer and method for controlling the coalescence of a pair of photons
    • 干涉仪和控制一对光子聚合的方法
    • EP2543957A8
    • 2013-05-22
    • EP12175470.9
    • 2012-07-06
    • Selex Sistemi Integrati S.p.A.
    • Bovino, Fabio Antonio
    • G01B9/02
    • G01B9/02001G01B9/02014G01B2290/55H04L9/0852
    • An interferometer for controlling the coalescence of a pair of photons, including: an optical source (51,52), which generates a first and a second pump pulse coherent with each other and shifted in time by a delay (τ); and a first interferometric stage (I a ), which receives the first pump pulse and generates an antisymmetric state with two coalescent photons 1 / 2 ( | 2 1 , 0 2 〉 - | 0 1 , 2 2 〉 . The interferometer also includes a second interferometric stage (I s ), which receives the second pump pulse and generates a symmetric state with two coalescent photons 1 / 2 ⋅ | 2 1 , 0 2 〉 + | 0 1 , 2 2 〉 , the first and the second interferometric stages being connected in a manner such that the interferometer outputs a final state equal to a weighted sum of the antisymmetric state and of the symmetric state 1 / 2 ⋅ | 2 1 , 0 2 〉 + | 0 1 , 2 2 〉 + e iτ ⋅ 1 / 2 ⋅ ⁢ | 2 1 , 0 2 〉 - | 0 1 , 2 2 〉 , the weights of the sum being a function of the delay.
    • 一种用于控制一对光子聚合的干涉仪,包括:一个光源(51,52),它产生彼此相干并且在时间上延迟一个延迟(τ)的第一和第二泵浦脉冲; 和第一干涉仪阶段(Ia),其接收第一泵浦脉冲并且产生具有两个聚结光子1/2(| 21,02> - | 01,22>)的反对称状态。干涉仪还包括第二干涉测量级(Is) ,其接收第二泵浦脉冲并且产生具有两个聚结光子的对称状态,第一和第二干涉仪级以这样的方式连接,使得干涉仪输出最终的 状态等于反对称状态和对称状态的加权和1 /2⋅| 21,02> + | 01,22> +eiτ⋅1/2⋅| 21,02> - | 01,22>,则 总和的权重是延迟的函数。
    • 6. 发明公开
    • Interferometer and method for controlling the coalescence of a pair of photons
    • Interferometer und Verfahren zur Steuerung der Koaleszenz eines Photonenpaares
    • EP2543957A1
    • 2013-01-09
    • EP12175470.9
    • 2012-07-06
    • Selex Sistemi Integrati S.p.A.
    • Bovino, Fabio Antonio
    • G01B9/02
    • G01B9/02001G01B9/02014G01B2290/55H04L9/0852
    • An interferometer for controlling the coalescence of a pair of photons, including: an optical source (51,52), which generates a first and a second pump pulse coherent with each other and shifted in time by a delay (τ); and a first interferometric stage (I a ), which receives the first pump pulse and generates an antisymmetric state with two coalescent photons (1/√2(|2 1 , 0 2 > - |0 1 , 2 2 >)). The interferometer also includes a second interferometric stage (I s ), which receives the second pump pulse and generates a symmetric state with two coalescent photons ((1/√2·(|2 1 , 0 2 > - |0 1 , 2 2 >))), the first and the second interferometric stages being connected in a manner such that the interferometer outputs a final state equal to a weighted sum of the antisymmetric state and of the symmetric state ((1/√2(|2 1 , 0 2 > - |0 1 , 2 2 >))), the weights of the sum being a function of the delay.
    • 一种用于控制一对光子的聚结的干涉仪,包括:光源(51,52),其产生彼此相干并在时间上延迟延迟(Ä)的第一和第二泵浦脉冲; 和第一干涉级(I a),其接收第一泵浦脉冲并且产生具有两个聚结光子1/2(| 2 1,0 2ªª| | 1,2 2)的反对称状态。干涉仪还包括 第二干涉级(I s),其接收第二泵浦脉冲并且产生具有两个聚结光子的对称状态1/2 <| 2 1,0 2ªª+ | | | | | | | | | | | | | | | 以这样的方式连接,使得干涉仪输出等于反对称状态和对称状态的加权和的最终状态1/2 <| 2 1,2 2ªª+ 1/2 < ¢| 2 1,0 2ªª - | 0 1,2 2ªª,和的权重是延迟的函数。
    • 8. 发明公开
    • COHERENT SPECTROSCOPIC METHODS WITH EXTENDED INTERROGATION TIMES AND SYSTEMS IMPLEMENTING SUCH METHODS
    • 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
    • EP3233719A1
    • 2017-10-25
    • EP15823154.8
    • 2015-12-18
    • Centre National de la Recherche Scientifique (C.N.R.S.)Institut d'Optique Graduate SchoolObservatoire de Paris
    • BERTOLDI, AndreaKOHLHAAS, RalfLANDRAGIN, ArnaudBOUYER, Philippe, Luc
    • B82Y10/00G01V7/00G04F5/14G06N99/00H03L7/26
    • G01J3/453B82Y10/00G01B2290/55G01J9/02G01V7/06G04F5/14
    • 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 .
    • 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。
    • 9. 发明公开
    • Coherent spectroscopic methods with extended interrogation times and systems implementing such
    • 相干光谱方法与扩展的查询时间和系统的实施
    • EP3034463A1
    • 2016-06-22
    • EP14307085.2
    • 2014-12-18
    • CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE -CNRS-Institut d'Optique Graduate SchoolObservatoire de Paris
    • Bertoldi, AndreaKohlhaas, RalfLandragin, ArnaudBouyer, Philippe, Luc
    • B82Y10/00G01V7/00G04F5/14G06N99/00H03L7/26
    • G01J3/453B82Y10/00G01B2290/55G01J9/02G01V7/06G04F5/14
    • 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 .
    • 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。