Y. Honda
KEK
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Publication
Featured researches published by Y. Honda.
Physical Review Special Topics-accelerators and Beams | 2010
P. Bambade; M. Alabau Pons; John Amann; D. Angal-Kalinin; R. Apsimon; S. Araki; A. Aryshev; Sha Bai; P. Bellomo; D. R. Bett; G.A. Blair; B. Bolzon; Stewart Boogert; G. Boorman; P. N. Burrows; G. Christian; P. Coe; Ben Constance; J P Delahaye; Laurence Deacon; E. Elsen; A. Faus-Golfe; Masafumi Fukuda; J. Gao; N. Geffroy; E. Gianfelice-Wendt; H. Guler; Hitoshi Hayano; A. Heo; Y. Honda
ATF2 is a final-focus test beam line which aims to focus the low emittance beam from the ATF damping ring to a vertical size of about 37 nm and to demonstrate nanometer level beam stability. Several advanced beam diagnostics and feedback tools are used. In December 2008, construction and installation were completed and beam commissioning started, supported by an international team of Asian, European, and U. S. scientists. The present status and first results are described.
Physical Review Special Topics-accelerators and Beams | 2012
Youngim Kim; Robert Ainsworth; A. Aryshev; S. Boogert; G. Boorman; J. Frisch; A. Heo; Y. Honda; W. H. Hwang; Jung-Yun Huang; Eun-Joo Kim; S. H. Kim; A. Lyapin; T. Naito; Justin May; D. McCormick; R. E. Mellor; S. Molloy; J. Nelson; S. J. Park; Y. J. Park; M. Ross; S. Shin; C. Swinson; T.I. Smith; Nobuhiro Terunuma; T. Tauchi; J. Urakawa; Gannon White
The Accelerator Test Facility 2 (ATF2) is a scaled demonstrator system for final focus beam lines of linear high energy colliders. This paper describes the high resolution cavity beam position monitor (BPM) system, which is a part of the ATF2 diagnostics. Two types of cavity BPMs are used, C-band operating at 6.423 GHz, and S-band at 2.888 GHz with an increased beam aperture. The cavities, electronics, and digital processing are described. The resolution of the C-band system with attenuators was determined to be approximately 250 nm and 1 � m for the S-band system. Without attenuation the best recorded C-band cavity resolution was 27 nm.
Journal of the Physical Society of Japan | 2009
Hirotaka Shimizu; Sakae Araki; Yoshisato Funahashi; Y. Honda; Toshiyuki Okugi; T. Omori; Nobuhiro Terunuma; Junji Urakawa; Masao Kuriki; S. Miyoshi; Tohru Takahashi; Yasuaki Ushio; T. Hirose; K. Sakaue; Masakazu Washio; P Guoxi; Xp Li; 李小平; 裴国玺
We studied gamma-ray generation by the laser-Compton scattering using a Fabry-Perot optical resonant cavity at the KEK-ATF electron storage ring. The laser power was enhanced up to 388 W in the optical resonant cavity with an injection power of 7 W in the ATF operation environments. The yield of photons for a crossing of a laser pulse and an electron bunch was 3.3 +/- 0.6, which was consistent with a numerical estimate. In this paper, we report construction, installation and future prospect toward the polarized positron generation for the International Linear Collider.
Applied Physics Letters | 2017
A. Aryshev; M. Shevelev; Y. Honda; Nobuhiro Terunuma; J. Urakawa
We present the response time measurements of a Cs2Te photocathode illuminated with two 100 fs duration, variable time separation laser pulses at 266 nm wavelength. The response time was confirmed in dispersive region downstream of a 12-cell standing wave S-band acceleration structure using a well-known RF zero-crossing technique. At the same time it was also measured by changing mechanical path-length difference between two micro-bunches. Both methods agree that Cs2Te photocathode time response is of the order of 250 fs and thereby it is possible to generate and control a THz sequence of relativistic electron bunches by a conventional S-band RF gun. This result further opens a possibility to construct wide-range tunable THz FEL.
Physical review accelerators and beams | 2017
A. Aryshev; A. P. Potylitsyn; G. A. Naumenko; M. Shevelev; K. Lekomtsev; L. G. Sukhikh; P. Karataev; Y. Honda; Nobuhiro Terunuma; J. Urakawa
Investigation of coherent Smith-Purcell Radiation (SPR) spectral characteristics was performed both experimentally and by numerical simulation. The measurement of SPR spectral line shapes of different diffraction orders was carried out at KEK LUCX facility. A pair of room-temperature Schottky barrier diode (SBD) detectors with sensitivity bands of
Journal of Instrumentation | 2013
A. Heo; Eun-San Kim; H. J. Kim; D. C. Son; Y. Honda; T. Tauchi
60-90
ieee particle accelerator conference | 2005
Shunsuke Araki; H. Hayano; Yu Higashi; Y. Honda; Kenji Kanazawa; Koichi Kubo; Tsuyoshi Kume; M. Kuriki; Sho Kuroda; M. Masuzawa; Tomoyuki Naito; T. Okugi; R. Sugahara; Tatsuro Takahashi; T. Tauchi; Nobuhiro Terunuma; N. Toge; J. Urakawa; V. Vogel; Hiroshi Yamaoka; K. Yokoya; J. Gao; Wenxin Liu; Guanhong Pei; Jiacheng Wang; B. Grishanov; P. Logachev; F. Podgorny; Valery I. Telnov; D. Angal-Kalinin
~GHz and
Journal of Instrumentation | 2014
Y. I. Kim; S. Boogert; Y. Honda; A. Lyapin; H. Park; Nobuhiro Terunuma; T. Tauchi; Junji Urakawa
320-460
ieee particle accelerator conference | 2007
S. Walston; Chun-Jen Chung; P Fitsos; J. Gronberg; Marc Ross; O. Khainovski; Y Kolomensky; P. Loscutoff; Mel Slater; Murray Thomson; David G. Ward; S. Boogert; Vladimir Vogel; R. Meller; Alexey Lyapin; S Malton; David A. B. Miller; Jerome Frisch; S. Hinton; John May; Daniel McCormick; S. Smith; Tim Smith; Gannon White; Toyoko Orimoto; Hitoshi Hayano; Y. Honda; Nobuhiro Terunuma; Junji Urakawa
~GHz was used in the measurements. Reasonable agreement of experimental results and simulations performed with CST Studio Suite justifies the use of different narrow-band SBD detectors to investigate different SPR diffraction orders. It was shown that monochromaticity of the SPR spectral lines increases with diffraction order. The comparison of coherent transition radiation and coherent SPR intensities in sub-THz frequency range showed that the brightnesses of both radiation mechanisms were comparable. A fine tuning feasibility of the SPR spectral lines is discussed.
Physical Review Letters | 2014
Glen White; R. Ainsworth; Tomoya Akagi; J. Alabau-Gonzalvo; D. Angal-Kalinin; S. Araki; A. Aryshev; Sha Bai; P. Bambade; D. R. Bett; G.A. Blair; C. Blanch; O. Blanco; N. Blaskovic-Kraljevic; B. Bolzon; S. Boogert; P. N. Burrows; Glenn Christian; L. Corner; M. R. Davis; A. Faus-Golfe; Masafumi Fukuda; J. Gao; H. García-Morales; N. Geffroy; Hitoshi Hayano; A. Heo; M. Hildreth; Y. Honda; J. Y. Huang
We have developed an S-band cavity Beam Position Monitor (BPM) in order to measure the position of an electron beam in the final focus area at ATF2, which is the test facility for the final focus design for the International Linear Collider (ILC). The lattice of the ILC Beam Delivery System (BDS) has been modified, requiring a larger physical aperture of 40 mm in the final focus area. The beam orbit measurement in this area is now covered with high resolution S-Band cavity BPMs. In this paper we summarize the design of the cavity BPM and the first experimental results. The calibration slopes were measured as 0.87 counts/?m in the x-coordinate direction and 1.16 counts/?m in the y-coordinate direction.