Masaharu Nishikino
Japan Atomic Energy Research Institute
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Featured researches published by Masaharu Nishikino.
Optics Letters | 2003
M. Tanaka; Masaharu Nishikino; Tetsuya Kawachi; Noboru Hasegawa; Masataka Kado; Maki Kishimoto; K. Nagashima; Yoshiaki Kato
We demonstrate an x-ray laser at a wavelength of 13.9 nm with a beam divergence of 0.2 mrad, which is 1.8 times the diffraction limit. The x-ray laser is generated with two gain media; the seed x-ray pulse from the first medium is amplified in the second medium. The effect of refraction on x-ray propagation is reduced by spatially and temporally controlling the injection of the seed x-ray to the second medium.
IEEE Journal of Selected Topics in Quantum Electronics | 2004
Masaharu Nishikino; M. Tanaka; Yoshihiro Ochi; Maki Kishimoto; Masahiko Ishino; Noboru Hasegawa; Masataka Kado; Kouta Sukegawa; Tetsuya Kawachi; K. Nagashima
We have recently reported the successful development of a fully coherent X-ray laser (XRL) at 13.9 nm by an oscillator-amplifier configuration with two targets. In the experiment, a seed XRL beam from the first target is injected into a plasma amplifier at the second target. The observed XRL beam has full spatial coherence and 0.2 mrad of nearly diffraction-limited divergence. In order to improve the output fluence, the amplification properties of the XRL beam have been investigated using various plasma lengths of the second amplifier target. The output energy has been improved by a factor of ten, increasing the length of the gain region to 10 mm, resulting in about 0.2 /spl mu/J of output energy.
Proceedings of SPIE | 2005
Tetsuya Kawachi; K. Nagashima; Maki Kishimoto; Noboru Hasegawa; M. Tanaka; Yoshihiro Ochi; Masaharu Nishikino; Hayato Kawazome; Renzhong Tai; Kazumichi Namikawa; Yoshiaki Kato
Recent progress in x-ray laser (XRL) research in Japan Atomic Energy Agency (JAEA) is reviewed. The repetition-rate of the x-ray laser has been improved from each 20 minutes to 10 seconds (0.1 Hz) by installing new driver laser, TOPAZ, which allows us to promote the applications of fully spatial coherent 13.9 nm laser in the wide variety of research fields such as material science, single-shot x-ray holography and atomic physics. In order to improve the present performance of the x-ray lasers, we have investigated the possibilities of the enhancement of the peak brilliance using v-groove target and the generation of circularly polarized x-ray laser under a strong magnetic field. Towards shorter wavelength x-ray lasers, we have investigated several schemes. One is the use of reflection of the light by relativistic plasma mirror driven by laser-wake-field, and the other is photo-pumping scheme using Kα emission from a solid target.
SUPERSTRONG FIELDS IN PLASMAS: Third International Conference on Superstrong Fields in Plasmas | 2006
Masaharu Nishikino; M. Tanaka; Hayato Kawazome; Tetsuya Kawachi; Akira Sasaki; Noboru Hasegawa; Yoshihiro Ochi; Maki Kishimoto; K. Nagashima; Naofumi Ohnishi
We have developed a fully coherent x‐ray laser (XRL) at 13.9 nm by a double‐target configuration. In the experiment, a seed XRL beam from the first target is injected into a plasma amplifier at the second target. The amplified XRL beam has full spatial coherence, 0.2 mrad of the nearly diffraction limited divergence, and 25 nJ of the output energy. For various application researches, we improve the output energy and the beam property of the x‐ray laser. The gain‐length product was gL ∼ 8.2, and the maximum output energy of about 1 μJ is achieved. The divergence of the XRL is affected by the refraction influence in the amplifier medium and/or the diffraction by the small size of the gain medium. We made the 2‐D radiation hydrodynamics simulation code in order to investigate the generation of the gain medium plasma and the refraction influence.
Optical Science and Technology, SPIE's 48th Annual Meeting | 2003
O. Guilbaud; Matthew Edwards; A. Klisnick; David Ros; G. Jamelot; Denis Joyeux; D. Phalippou; Huajing Tang; Paul Neumayer; D. Ursescu; G.J. Tallents; Thomas Kuehl; K. Cassou; Kamal Bouhouch; Masataka Kado; Masaharu Nishikino; Kota Sukegawa; Maki Kishimoto; Masahiko Ishino; K. Nagashima; H. Daido; W. Seelig; Stefan Borneis; E. Gaul; W. Geithner; C. Hafner; Piotr P. Wiewior
We review our recent progress in the development of transient x-ray lasers and of their application to plasma diagnostic. The first observation of C-ray laser emission at the new PHELIX-GSI facility is reported. This TCE X-ray laser will be a promising tool for heavy-ion spectroscopy. We then present the main results obtained at the LULU-CPA facility with a compact high-resolution X-UV imaging device. This device was used to investigate the spatial source structure of the Ni-like silver transient X-ray laser under different pumping conditions. The key-role of the width of the background laser pulse on the shape of the emitting aperture is demonstrated. Finally the imaging device was used as an interference microscope for interferometry probing of a laser-produced plasma. We describe this experiment performed at APRC-JAERI.
SYNCHROTRON RADIATION INSTRUMENTATION: Eighth International Conference on Synchrotron Radiation Instrumentation | 2004
Renzhong Tai; Kazumichi Namikawa; Maki Kishimoto; M. Tanaka; A. Sawada; Noboru Hasegawa; Tetsuya Kawachi; Kouta Sukegawa; Masataka Kado; Yoshihiro Ochi; Masaharu Nishikino; K. Nagashima; H. Daido; Y. Kato; H. Maruyama; M. Ando
Picosecond x‐ray speckles experiment has been conducted with a simple setup. The source was a compact silver‐plasma‐based x‐ray laser, with a wavelength of 13.9 nm and pulse duration of 7 ps. The sample was a single crystal of BaTiO3, with ferroelectric multi‐domain structure (a/c domains). The matter correlation function, including statistical information of those randomly distributed scatterers (domains here) within the sample, was extracted by deconvolution of the speckle pattern. The instantaneous x‐ray speckle technique has proved to be particularly efficient to be used to observe fast microscopic‐scale phenomena that are hard to access with other methods currently.
Optical Science and Technology, SPIE's 48th Annual Meeting | 2003
K. Nagashima; M. Tanaka; Masaharu Nishikino; Maki Kishimoto; Masataka Kado; Tetsuya Kawachi; Noboru Hasegawa; Yoshihiro Ochi; Kouta Sukegawa; Renzhong Tai; Yoshiaki Kato
We have succeeded in developing a laser-pumped x-ray laser with full spatial coherence at 13.9 nm. A highly directed x-ray laser beam with the divergence of 0.2 mrad was generated from the double target experiment, where a seeding light from the first laser medium was amplified in the second medium. The observed divergence is close to the diffraction limited value within a factor of two. The seeding light was amplified in the second medium without refraction influence and the gain coefficient was about 8 cm-1. The gain region of the second medium was far away from the target surface compared with that of the first medium and located in the considerably low density region. From the measurement of visibility, it was found that the spatial coherent length is longer than the beam diameter.
Physical Review A | 2003
Masaharu Nishikino; M. Tanaka; K. Nagashima; Maki Kishimoto; Masataka Kado; Tetsuya Kawachi; Kouta Sukegawa; Yoshihiro Ochi; Noboru Hasegawa; Yoshiaki Kato
Applied Physics B | 2004
H. Tang; O. Guilbaud; G. Jamelot; D. Ros; A. Klisnick; Denis Joyeux; D. Phalippou; Masataka Kado; Masaharu Nishikino; Maki Kishimoto; Kouta Sukegawa; Masahiko Ishino; K. Nagashima; H. Daido
Applied Physics B | 2004
Yoshihiro Ochi; Tetsuya Kawachi; Noboru Hasegawa; Akira Sasaki; K. Nagashima; Kouta Sukegawa; Maki Kishimoto; M. Tanaka; Masaharu Nishikino; Masataka Kado