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
    • 3. 发明授权
    • Radiation shield and optical lattice clock including radiation shield
    • US11493887B2
    • 2022-11-08
    • US16251619
    • 2019-01-18
    • RIKEN
    • Hidetoshi KatoriMasao TakamotoIchiro UshijimaTakehiro TawaraHideo Yokota
    • G04F5/14G02B5/20H03L7/26
    • Provided according to an embodiment of the present disclosure is a radiation shield 10 including a shield wall surrounding a hollow region capable of accommodating therein atoms for an optical lattice clock 100, the shield wall having, provided therein, at least two apertures communicating with outside. A geometrical shape of an inner wall surface of the shield wall is configured such that a difference between BBR shifts found under two conditions does not exceed a predetermined value over a range of position of atoms, the BBR shifts being caused in atoms 2 by emitted radiation emitted by the inner wall surface, incoming radiation leaking in from the outside through the apertures, and a reflection component of the emitted radiation and incoming radiation at the inner wall surface, the two conditions being a condition where the inner wall surface exhibits mirror reflection and a condition where the inner wall surface exhibits diffuse reflection, the range being where clock transition operation is carried out in the optical lattice clock, the inner wall surface facing the hollow region. Provided according to other embodiments of the present disclosure also are the optical lattice clock 100 including such a radiation shield, and a design method for the radiation shield.
    • 4. 发明授权
    • Optical lattice clock, clock device and laser light source
    • 光栅时钟,时钟器件和激光光源
    • US09553597B2
    • 2017-01-24
    • US14422177
    • 2013-08-12
    • RIKEN
    • Hidetoshi Katori
    • H03L7/26G04F5/14H01S3/067
    • H03L7/26G04F5/14H01S3/06791
    • Various embodiments improve accuracy by increasing the number of atoms engaged in a clock transitions in an optical lattice clock. An exemplary optical lattice clock an embodiment comprises an optical waveguide, an optical path, a laser light source, and a laser cooler. The optical path has a hollow pathway that extends from a first end to a second end while being surrounded with a tubular wall, which is used as a waveguide path. The optical path passes between mirrors and through the pathway. The laser light source supplies to the optical path a pair of lattice lasers (L1 and L2) propagating in opposite directions with each other. The laser cooler supplies cooled atoms that have two levels of electronic states associated with a clock transition to the vicinity of the first end of the optical waveguide.
    • 各种实施例通过增加在光栅格时钟中的时钟转换中引入的原子的数量来提高精度。 示例性光学晶格时钟实施例包括光波导,光路,激光光源和激光冷却器。 光路具有从第一端延伸到第二端的中空路径,同时被用作波导路径的管状壁围绕。 光路通过反射镜和通过通路。 激光源向光路提供一对彼此相反方向传播的格子激光器(L1和L2)。 激光冷却器提供具有与时钟转变相关联的两级电子状态的冷却原子到光波导的第一端附近。
    • 6. 发明申请
    • OPTICAL LATTICE CLOCK, CLOCK DEVICE AND LASER LIGHT SOURCE
    • 光学时钟,时钟设备和激光光源
    • US20150194972A1
    • 2015-07-09
    • US14422177
    • 2013-08-12
    • RIKEN
    • Hidetoshi Katori
    • H03L7/26H01S3/067G04F5/14
    • H03L7/26G04F5/14H01S3/06791
    • Various embodiments improve accuracy by increasing the number of atoms engaged in a clock transitions in an optical lattice clock. An exemplary optical lattice clock an embodiment comprises an optical waveguide, an optical path, a laser light source, and a laser cooler. The optical path has a hollow pathway that extends from a first end to a second end while being surrounded with a tubular wall, which is used as a waveguide path. The optical path passes between mirrors and through the pathway. The laser light source supplies to the optical path a pair of lattice lasers (L1 and L2) propagating in opposite directions with each other. The laser cooler supplies cooled atoms that have two levels of electronic states associated with a clock transition to the vicinity of the first end of the optical waveguide.
    • 各种实施例通过增加在光栅格时钟中的时钟转换中引入的原子的数量来提高精度。 示例性光学晶格时钟实施例包括光波导,光路,激光光源和激光冷却器。 光路具有从第一端延伸到第二端的中空路径,同时被用作波导路径的管状壁围绕。 光路通过反射镜和通过通路。 激光源向光路提供一对彼此相反方向传播的格子激光器(L1和L2)。 激光冷却器提供具有与时钟转变相关联的两级电子状态的冷却原子到光波导的第一端附近。