S. Kawakami
Osaka City University
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Featured researches published by S. Kawakami.
Astroparticle Physics | 2003
M. Takeda; N. Sakaki; K. Honda; M. Chikawa; M. Fukushima; N. Hayashida; N. Inoue; Kenichi Kadota; F. Kakimoto; K. Kamata; S. Kawaguchi; S. Kawakami; Y. Kawasaki; N. Kawasumi; Ayman Mahrous; K. Mase; S. Mizobuchi; Y. Morizane; M. Nagano; H. Ohoka; S. Osone; Makoto Sasaki; Masaki Sasano; H.M. Shimizu; K. Shinozaki; M. Teshima; R. Torii; I. Tsushima; Yukio Uchihori; Tomohiko Yamamoto
Abstract Using data from more than 10 years of observations with the Akeno Giant Air Shower Array (AGASA), we published a result that the energy spectrum of ultra-high energy cosmic rays extends beyond the cutoff energy predicted by Greisen [Rhys. Rev. Lett. 16 (1966) 748] and Zatsepin and Kuzmin [Zh. Eksp. Teor. Fiz. 4 (1966) 114]. In this paper, we reevaluate the energy determination method used for AGASA events with respect to the lateral distribution of shower particles, their attenuation with zenith angle, shower front structure, delayed particles observed far from the core and other factors. The currently assigned energies of AGASA events have an accuracy of ±25% in event-reconstruction resolution and ±18% in systematic errors around 10 20 eV. This systematic uncertainty is independent of primary energy above 10 19 eV. Based on the energy spectrum from 10 14.5 eV to a few times 10 20 eV determined at Akeno, there are surely events above 10 20 eV and the energy spectrum extends up to a few times 10 20 eV without a GZK cutoff.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
O. Adriani; M. van den Akker; S. Banerjee; J. Bähr; B. Betev; D. Bourilkov; S. Bottai; G. J. Bobbink; A.M. Cartacci; M. Chemarin; G. Chen; Hf Chen; T. Chiarusi; C.J. Dai; L.K. Ding; I. Duran; G. Faber; J. Fay; H.J. Grabosch; H. Groenstege; Y.N. Guo; S.K. Gupta; Ch. Haller; Y. Hayashi; Z.X. He; T. Hebbeker; H. Hofer; H. Hoferjun; A.X. Huo; N. Ito
AbstractThe L3 detector at the CERN electron–positron collider, LEP, has been employed for the study of cosmic ray muons.The muon spectrometer of L3 consists of a set of high-precision drift chambers installed inside a magnet with avolume of about 1000 m 3 and a field of 0:5T: Muon momenta are measured with a resolution of a few percentat 50 GeV: The detector is located under 30 m of overburden. A scintillator air shower array of 54 m by 30 mis installed on the roof of the surface hall above L3 in order to estimate the energy and the core position of theshower associated with a sample of detected muons. Thanks to the unique properties of the L3þC detector, muonresearch topics relevant to various current problems in cosmic ray and particle astrophysics can be studied. r 2002Elsevier Science B.V. All rights reserved. PACS: 95.55.Vj; 98.70.Sa; 96.40.Tv; 95.85.RyKeywords: L3+C detector; Cosmic rays; Muon spectrum; Astroparticle physics 1. IntroductionThe L3þ C experiment (Figs. 1 and 2), installedat the Large Electron Positron collider (LEP) atCERN, Geneva, consists of two major parts:firstly, below ground, the L3 muon spectrometer[1], which is comprised of a large 0:5 T magnetwith a volume of 1000 m
Pramana | 1982
M. R. Krishnaswamy; M. G. K. Menon; N. K. Mondal; V. S. Narasimham; B.V. Sreekantan; Y. Hayashi; N Ito; S. Kawakami; S Miyake
The neutrino events recorded in the Kolar Gold Field Nucleon Decay detector are analysed here. It is shown that there is good agreement between the observations and the estimates based on the intensities of atmospheric neutrinos and interaction cross-sections of neutrinos available from accelerator experiments. In the context of the search for proton decay, we show that the low energy (<2 GeV) neutrino events, which would provide the main background, are suppressed at thekgf site since it is situated near geomagnetic equator, where the geomagnetic cut-off rigidities are high. A comparison of the predicted characteristics ofv-induced events with thekgf observations shows that, within the statistical accuracy of the present data, the signal due to nucleon decay stands out distinctly within thev-induced background.
Journal of the Physical Society of Japan | 2009
Hisashi Kawai; Sho Yoshida; J. H. Kim; S. Roh; Dongsu Ryu; H. Yoshii; S. Nam; I. H. Park; J. Yang; B.G. Cheon; E.J. Cho; H.B. Kim; J.H. Kim; K. Tanaka; F. Cohen; M. Fukushima; N. Hayashida; K. Hiyama; D. Ikeda; E. Kido; Y. Kondo; T. Nonaka; M. Ohnishi; H. Ohoka; S. Ozawa; H. Sagawa; N. Sakurai; T.-A. Shibata; H. Shimodaira; M. Takeda
The Telescope Array (TA) is a large scale ground experiment in Utah, USA for the measurement of extensive air showers from the ultra-high energy cosmic rays. Its construction is completed in March, 2008 and the data taking started.
Pramana | 2005
Sourendu Gupta; Y. Hayashi; A. Jain; S. Karthikeyan; S. Kawakami; K. C. Ravindran; S. C. Tonwar
A high-performance, low-cost, leading edge discriminator has been designed with a timing performance comparable to state-of-the-art, commercially available discriminators. A timing error of 16 ps is achieved under ideal operating conditions. Under more realistic operating conditions the discriminator displays a timing error of 90 ps. It has an intrinsic double pulse resolution of 4 ns which is better than most commercial discriminators. A low-cost discriminator is an essential requirement of the GRAPES-3 experiment where a large number of discriminator channels are used.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
Tomohiko Yamamoto; M. Chikawa; N. Hayashida; S. Kawakami; N. Minagawa; Y. Morizane; Masaki Sasano; M. Teshima; K. Yasui
We have developed an atmospheric monitoring system for the Telescope Array experiment at Akeno Observatory. It consists of a Nd:YAG laser with an alt-azimuth shooting system and a small light receiver. This system is installed inside an air conditioned weather-proof dome. All parts, including the dome, laser, shooter, receiver, and optical devices are fully controlled by a personal computer utilizing the Linux operating system. It is now operated as a back-scattering LIDAR system. For the Telescope Array experiment, to estimate energy reliably and to obtain the correct shower development profile, the light transmittance in the atmosphere needs to be calibrated with high accuracy. Based on observational results using this monitoring system, we consider this LIDAR to be a very powerful technique for Telescope Array experiments. The details of this system and its atmospheric monitoring technique will be discussed.
Nuclear Physics B - Proceedings Supplements | 2008
H. Kawai; Sho Yoshida; H. Yoshii; K. Tanaka; F. Cohen; M. Fukushima; N. Hayashida; K. Hiyama; D. Ikeda; E. Kido; Y. Kondo; T. Nonaka; M. Ohnishi; H. Ohoka; S. Ozawa; H. Sagawa; N. Sakurai; T.-A. Shibata; H. Shimodaira; M. Takeda; A. Taketa; M. Takita; H. Tokuno; R. Torii; S. Udo; Y. Yamakawa; Hirofumi Fujii; T. Matsuda; M. Tanaka; H. Yamaoka
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
Sourendu Gupta; Yuri Aikawa; N. V. Gopalakrishnan; Y. Hayashi; Noriaki Ikeda; N. Ito; A. Jain; Alexander V. St. John; S. Karthikeyan; S. Kawakami; T. Matsuyama; Deepak Mohanty; P.K. Mohanty; S.D. Morris; T. Nonaka; A. Oshima; B.S. Rao; K. C. Ravindran; M. Sasano; K. Sivaprasad; B. V. Sreekantan; Hiroyuki Tanaka; S. C. Tonwar; K. Viswanathan; T. Yoshikoshi
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
Y. Hayashi; Yuri Aikawa; N. V. Gopalakrishnan; Sourendu Gupta; Noriaki Ikeda; N. Ito; A. Jain; Alexander V. St. John; S. Karthikeyan; S. Kawakami; Haruo Kojima; T. Matsuyama; Deepak Mohanty; P.K. Mohanty; S.D. Morris; T. Nonaka; A. Oshima; B.S. Rao; K. C. Ravindran; M. Sasano; K. Sivaprasad; B. V. Sreekantan; Hiroyuki Tanaka; S. C. Tonwar; K. Viswanathan; T. Yoshikoshi
Physical Review D | 2006
T. Nonaka; Y. Hayashi; N. Ito; S. Kawakami; T. Matsuyama; A. Oshima; Hiroyuki Tanaka; T. Yoshikoshi; Sourendu Gupta; A. Jain; S. Karthikeyan; P. K. Mohanty; S.D. Morris; B.S. Rao; K. C. Ravindran; K. Sivaprasad; B. V. Sreekantan; S. C. Tonwar; K. Viswanathan; Haruo Kojima