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    • 1. 发明申请
    • OPTICAL WAVEGUIDE
    • 光波导
    • US20070269178A1
    • 2007-11-22
    • US11750608
    • 2007-05-18
    • Nobuhiko SarukuraKo AosakiHideki SatoYoshihiko Sakane
    • Nobuhiko SarukuraKo AosakiHideki SatoYoshihiko Sakane
    • G02B6/00
    • G02B6/1225B82Y20/00G01J3/42
    • Materials transparent to terahertz waves are very limited, and it is difficult to obtain the required performance by selecting the material. Further, it is also difficult to search for a novel material. Therefore, by letting a known material transparent to terahertz waves have a photonic crystal structure and controlling the structure, an optical waveguide having the required properties is provided. An optical waveguide for propagation of far-infrared radiation in the terahertz region, which optical waveguide is made of a fluorinated amorphous polymer. Particularly preferred is a polymer having a fluorinated aliphatic ring structure in its main chain, obtained by cyclopolymerization of a fluorinated monomer having at least two polymerizable double bonds.
    • 对太赫兹波透明的材料非常有限,通过选择材料难以获得所需的性能。 此外,还难以搜索新材料。 因此,通过使已知的对太赫兹波透明的材料具有光子晶体结构并控制结构,提供了具有所需特性的光波导。 用于在太赫兹区域中传播远红外辐射的光波导,该光波导由氟化无定形聚合物制成。 特别优选的是在其主链中具有氟化脂族环结构的聚合物,其通过具有至少两个可聚合双键的氟化单体的环化聚合获得。
    • 2. 发明授权
    • Optical waveguide
    • 光波导
    • US07440671B2
    • 2008-10-21
    • US11750608
    • 2007-05-18
    • Nobuhiko SarukuraKo AosakiHideki SatoYoshihiko Sakane
    • Nobuhiko SarukuraKo AosakiHideki SatoYoshihiko Sakane
    • G02B6/00G02B6/02
    • G02B6/1225B82Y20/00G01J3/42
    • Materials transparent to terahertz waves are very limited, and it is difficult to obtain the required performance by selecting the material. Further, it is also difficult to search for a novel material. Therefore, by letting a known material transparent to terahertz waves have a photonic crystal structure and controlling the structure, an optical waveguide having the required properties is provided.An optical waveguide for propagation of far-infrared radiation in the terahertz region, which optical waveguide is made of a fluorinated amorphous polymer. Particularly preferred is a polymer having a fluorinated aliphatic ring structure in its main chain, obtained by cyclopolymerization of a fluorinated monomer having at least two polymerizable double bonds.
    • 对太赫兹波透明的材料非常有限,通过选择材料难以获得所需的性能。 此外,还难以搜索新材料。 因此,通过使已知的对太赫兹波透明的材料具有光子晶体结构并控制结构,提供了具有所需特性的光波导。 用于在太赫兹区域中传播远红外辐射的光波导,该光波导由氟化无定形聚合物制成。 特别优选的是在其主链中具有氟化脂族环结构的聚合物,其通过具有至少两个可聚合双键的氟化单体的环化聚合获得。
    • 3. 发明授权
    • Production method and device for hologram
    • 全息图的制作方法和装置
    • US06633419B2
    • 2003-10-14
    • US09890274
    • 2001-11-09
    • Hideo HosonoMasahiro HiranoNobuhiko SarukuraKenichi Kawamura
    • Hideo HosonoMasahiro HiranoNobuhiko SarukuraKenichi Kawamura
    • G03H104
    • G03H1/04G02B2006/12107G03H1/0272G03H2001/0482G03H2222/33G03H2260/62G03H2270/11G03H2270/13H01S3/0057
    • A method and apparatus for producing a hologram using a two-beam laser interference exposure process, comprising the steps of using as a light source a femtosecond laser having a pulse width of 900-10 femtoseconds and a peak output of 1 GW or more and capable of generating a pulse beam at or close to the Fourier transform limit, dividing the pulse beam from the laser into two by a beam splitter, controlling the two beams temporally through an optical delay circuit and spatially using plane and concave mirrors each having a slightly rotatable reflection surface to converge the beams on a surface of or within a substrate for recording a hologram at an energy density of 100 GW/cm2 or more with keeping each polarization plane of the two beams in parallel so as to match the converged spot of the two beams temporally and spatially, whereby a hologram is recorded irreversibly on the substrate formed of a transparent material, semiconductor material or metallic material.
    • 一种使用双光束激光干涉曝光工艺制造全息图的方法和装置,包括以下步骤:使用具有900-10飞秒脉冲宽度和1GW或更大的峰值输出的飞秒激光,并具有能力 在或者接近于傅里叶变换极限的情况下产生脉冲束,通过分束器将来自激光器的脉冲光束分成两个,通过光学延迟电路暂时控制两个光束,并在空间上使用每个具有可旋转的平面和凹面镜 反射表面以将光束会聚在衬底的表面或衬底内,用于以100GW / cm 2的能量密度记录全息图,同时保持两个光束的每个偏振面 平行地在时间上和空间上匹配两个光束的会聚点,由此在由透明材料,半导体材料或金属材料形成的基板上不可逆地记录全息图。
    • 5. 发明申请
    • METHOD OF DETERMINING NUCLEAR FUSION IRRADIATION COORDINATES, DEVICE FOR DETERMINING NUCLEAR FUSION IRRADIATION COORDINATES, AND NUCLEAR FUSION DEVICE
    • 确定核熔融辐射坐标的方法,用于确定核熔融辐射坐标的装置和核熔融装置
    • US20120155590A1
    • 2012-06-21
    • US13388500
    • 2010-07-20
    • Masakatsu MurakamiNobuhiko SarukuraHiroshi AzechiRyo YasuharaToshiyuki KawashimaHirofumi Kan
    • Masakatsu MurakamiNobuhiko SarukuraHiroshi AzechiRyo YasuharaToshiyuki KawashimaHirofumi Kan
    • G21B1/00G06F17/10
    • G21B1/23H05H1/22
    • An object of the present invention is to efficiently improve uniformity of energy lines to be irradiated. A method of determining nuclear fusion irradiation coordinates according to the present invention is a method of calculating irradiation coordinates when energy lines are irradiated onto a nuclear fusion target, and comprises an initial arrangement step S202 of virtually arranging electric charges Qi at initial coordinates of the number of irradiation coordinates NB on a spherical surface S0 set by using random numbers, a coordinate analysis step S203 of analyzing coordinates ri of the electric charges Qi in time series based on coulomb forces acting among the electric charges Qi by constraining the coordinates ri onto the spherical surface S0, potential evaluation steps S205 and S206 of determining a timing at which potential energies of the electric charges Qi were stabilized based on the coordinates ri, and an irradiation coordinate deriving step S207 of deriving coordinates ri at the timing at which potential energies were stabilized as irradiation coordinates of energy lines in a case where a nuclear fusion target is arranged at the center of the spherical surface S0.
    • 本发明的目的在于有效地提高被照射的能量线的均匀性。 根据本发明的确定核聚变照射坐标的方法是当将能量线照射到核聚变靶上时计算辐射坐标的方法,包括在数字的初始坐标处虚拟地布置电荷Qi的初始布置步骤S202 在通过使用随机数设置的球面S0上的照射坐标NB的坐标分析步骤S203,其基于通过将坐标ri约束到球面上来分析基于通过电荷Qi之间的库仑力的时间序列的电荷Qi的坐标ri 表面S0,基于坐标ri确定电荷Qi的势能的定时的电位评估步骤S205和S206以及在势能稳定的定时导出坐标ri的照射坐标导出步骤S207 作为能量线的照射坐标 将核聚变靶设置在球面S0的中央的情况。
    • 7. 发明授权
    • Method of determining nuclear fusion irradiation coordinates, device for determining nuclear fusion irradiation coordinates, and nuclear fusion device
    • 确定核聚变辐射坐标的方法,确定核聚变辐射坐标的装置和核聚变装置
    • US09230694B2
    • 2016-01-05
    • US13388500
    • 2010-07-20
    • Masakatsu MurakamiNobuhiko SarukuraHiroshi AzechiRyo YasuharaToshiyuki KawashimaHirofumi Kan
    • Masakatsu MurakamiNobuhiko SarukuraHiroshi AzechiRyo YasuharaToshiyuki KawashimaHirofumi Kan
    • G21B1/00G21B1/23H05H1/22
    • G21B1/23H05H1/22
    • An object of the present invention is to efficiently improve uniformity of energy lines to be irradiated. A method of determining nuclear fusion irradiation coordinates according to the present invention is a method of calculating irradiation coordinates when energy lines are irradiated onto a nuclear fusion target, and comprises an initial arrangement step S202 of virtually arranging electric charges Qi at initial coordinates of the number of irradiation coordinates NB on a spherical surface S0 set by using random numbers, a coordinate analysis step S203 of analyzing coordinates ri of the electric charges Qi in time series based on coulomb forces acting among the electric charges Qi by constraining the coordinates ri onto the spherical surface S0, potential evaluation steps S205 and S206 of determining a timing at which potential energies of the electric charges Qi were stabilized based on the coordinates ri, and an irradiation coordinate deriving step S207 of deriving coordinates ri at the timing at which potential energies were stabilized as irradiation coordinates of energy lines in a case where a nuclear fusion target is arranged at the center of the spherical surface S0.
    • 本发明的目的在于有效地提高被照射的能量线的均匀性。 根据本发明的确定核聚变照射坐标的方法是当将能量线照射到核聚变靶上时计算辐射坐标的方法,包括在数字的初始坐标处虚拟地布置电荷Qi的初始布置步骤S202 在通过使用随机数设置的球面S0上的照射坐标NB的坐标分析步骤S203,其基于通过将坐标ri约束到球面上来分析基于通过电荷Qi之间的库仑力的时间序列的电荷Qi的坐标ri 表面S0,基于坐标ri确定电荷Qi的势能的定时的电位评估步骤S205和S206以及在势能稳定的定时导出坐标ri的照射坐标导出步骤S207 作为能量线的照射坐标 将核聚变靶设置在球面S0的中央的情况。