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1.
公开(公告)号:US10206272B2
公开(公告)日:2019-02-12
申请号:US15323115
申请日:2015-05-15
Applicant: HAMAMATSU PHOTONICS K.K.
Inventor: Nakahiro Satoh , Ryo Yoshimura , Masaru Takagi , Toshiyuki Kawashima , Hirofumi Kan
Abstract: The present invention relates to a method for manufacturing a tracer-encapsulated solid pellet for magnetic-confinement fusion, the method comprising a liquid droplet formation step of discharging an organic liquid containing an organic solvent into a stabilizing liquid to thereby form liquid droplets 12, and an organic solvent removal step of removing the organic solvent from the liquid droplets 12A. The organic liquid to be used is a liquid having a first organic polymer containing tracer atoms and a second organic polymer being an organic polymer different from the first organic polymer dissolved in the organic solvent, wherein the first organic polymer and the second organic polymer can be mutually phase-separated.
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公开(公告)号:US09805829B2
公开(公告)日:2017-10-31
申请号:US14434893
申请日:2013-10-10
Applicant: HAMAMATSU PHOTONICS K.K. , The Graduate School for the Creation of New Photonics Industries , TOYOTA JIDOSHA KABUSHIKI KAISHA
Inventor: Takashi Sekine , Takashi Kurita , Toshiyuki Kawashima , Nakahiro Satoh , Hirofumi Kan , Yoneyoshi Kitagawa , Yoshitaka Mori , Katsuhiro Ishii , Kazuhisa Fujita , Ryohei Hanayama , Shinichiro Okihara , Atsushi Sunahara , Osamu Komeda , Naoki Nakamura , Yasuhiko Nishimura , Hirozumi Azuma
Abstract: A target shell monitoring device 4 that monitors an attitude and a position of the target shell Tg1, a compression laser output device 5a that irradiates the target shell Tg1 with a compression laser light LS1, and a heating laser output device 6 that irradiates the target shell Tg1 with a heating laser light LS3 following the compression laser light LS1 are provided. The target shell Tg1 has a hollow spherical shell shape, includes an approximately spherical space Sp on an inner side thereof, includes at least one through hole H1 connecting an outer side thereof and the space Sp, and includes, on an outer surface Sf1 thereof, irradiation areas Ar1 and Ar2 to be irradiated with compression laser lights.
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公开(公告)号:US09672944B2
公开(公告)日:2017-06-06
申请号:US14948495
申请日:2015-11-23
Applicant: OSAKA UNIVERSITY , HAMAMATSU PHOTONICS K.K.
Inventor: Masakatsu Murakami , Nobuhiko Sarukura , Hiroshi Azechi , Ryo Yasuhara , Toshiyuki Kawashima , Hirofumi Kan
Abstract: 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.
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4.
公开(公告)号:US20150270019A1
公开(公告)日:2015-09-24
申请号:US14434893
申请日:2013-10-10
Applicant: HAMAMATSU PHOTONICS K.K. , THE GRADUATE SCHOOL FOR THE CREATION OF NEW PHOTONICS INDUSTRIES , TOYOTA JIDOSHA KABUSHIKI KAISHA
Inventor: Takashi Sekine , Takashi Kurita , Toshiyuki Kawashima , Nakahiro Satoh , Hirofumi Kan , Yoneyoshi Kitagawa , Yoshitaka Mori , Katsuhiro Ishii , Kazuhisa Fujita , Ryohei Hanayama , Shinichiro Okihara , Atsushi Sunahara , Osamu Komeda , Naoki Nakamura , Yasuhiko Nishimura , Hirozumi Azuma
Abstract: A target shell monitoring device 4 that monitors an attitude and a position of the target shell Tg1, a compression laser output device 5a that irradiates the target shell Tg1 with a compression laser light LS1, and a heating laser output device 6 that irradiates the target shell Tg1 with a heating laser light LS3 following the compression laser light LS1 are provided. The target shell Tg1 has a hollow spherical shell shape, includes an approximately spherical space Sp on an inner side thereof, includes at least one through hole H1 connecting an outer side thereof and the space Sp, and includes, on an outer surface Sf1 thereof, irradiation areas Ar1 and Ar2 to be irradiated with compression laser lights.
Abstract translation: 监视目标壳体Tg1的姿态和位置的目标壳体监视装置4,利用压缩激光LS1照射目标壳体Tg1的压缩激光输出装置5a以及照射目标壳体的加热用激光输出装置6 提供具有压缩激光LS1之后的加热激光LS3的Tg1。 目标壳Tg1具有中空球壳形状,在其内侧包括大致球形的空间Sp,包括至少一个连接其外侧的空间Sp和通孔H1,并且在其外表面Sf1上, 照射区域Ar1和Ar2照射压缩激光。
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公开(公告)号:US09882354B2
公开(公告)日:2018-01-30
申请号:US15124778
申请日:2015-03-03
Applicant: HAMAMATSU PHOTONICS K.K.
Inventor: Yujin Zheng , Hirofumi Kan
CPC classification number: H01S5/4062 , H01S3/0804 , H01S3/08081 , H01S3/0815 , H01S5/02438 , H01S5/026 , H01S5/10 , H01S5/141 , H01S5/4025 , H01S5/405 , H01S5/4068 , H01S5/42
Abstract: A semiconductor laser device includes: a semiconductor laser array in which a plurality of active layers that emit laser lights with a divergence angle θS (>4°) in a slow axis direction are arranged; a first optical element that reflects first partial lights by a first reflecting surface and returns the first partial lights to the active layers; and a second optical element that reflects partial mode lights of second partial lights by a second reflecting surface and returns the partial mode lights to the active layers, the first reflecting surface forms an angle equal to or greater than 2° and less than (θS/2) with a plane perpendicular to an optical axis direction of the active layers, and the second reflecting surface forms an angle greater than (−θS/2) and equal to or less than −2° with the plane perpendicular to the optical axis direction of the active layers.
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