T. Nonaka
Osaka City University
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Featured researches published by T. Nonaka.
Astronomy and Astrophysics | 2009
Prasad Subramanian; H. M. Antia; S. Dugad; U. D. Goswami; Sourendu Gupta; Y. Hayashi; N. Ito; S. Kawakami; Haruo Kojima; P. K. Mohanty; P.K. Nayak; T. Nonaka; A. Oshima; K. Sivaprasad; H. Tanaka; S. C. Tonwar
Aims. We seek to estimate the average level of MHD turbulence near coronal mass ejection (CME) fronts as they propagate from the Sun to the Earth. Methods. We examined the cosmic ray data from the GRAPES-3 tracking muon telescope at Ooty, together with the data from other sources for three closely observed Forbush decrease events. Each of these event is associated with frontside halo coronal mass ejections (CMEs) and near-Earth magnetic clouds. The associated Forbush decreases are therefore expected to have significant contributions from the cosmic-ray depressions inside the CMEs/ejecta. In each case, we estimate the magnitude of the Forbush decrease using a simple model for the diffusion of high-energy protons through the largely closed field lines enclosing the CME as it expands and propagates from the Sun to the Earth. The diffusion of high-energy protons is inhibited by the smooth, large-scale magnetic field enclosing the CME and aided by the turbulent fluctuations near the CME front. We use estimates of the cross-field diffusion coefficientxa0
Astronomy and Astrophysics | 2013
K. P. Arunbabu; H. M. Antia; S. Dugad; Sourendu Gupta; Y. Hayashi; S. Kawakami; P. K. Mohanty; T. Nonaka; A. Oshima; Prasad Subramanian
D_{perp}
Journal of Physics G | 2012
H. Tanaka; S. Dugad; Sourendu Gupta; A. Jain; P. K. Mohanty; B.S. Rao; K. C. Ravindran; K. Sivaprasad; S. C. Tonwar; Y. Hayashi; N. Ito; S. Kawakami; M. Minamino; T. Nonaka; A. Oshima
derived from the published results of extensive Monte Carlo simulations of cosmic rays propagating through turbulent magnetic fields. We then compare our estimates with the magnitudes of the observed Forbush decreases. Results. Our method helps constrain the ratio of energy density in the turbulent magnetic fields to that in the mean magnetic fields near the CME fronts. This ratio is found to be ~2% for the 2001 April 11 Forbush decrease event, ~6% for the 2003 November 20 Forbush decrease event and ~249% for the much more energetic event of 2003 October 29.
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
Aims. We seek to identify the primary agents causing Forbush decreases (FDs) in high-rigidity cosmic rays observed from the Earth. In particular, we ask if these FDs are caused mainly by coronal mass ejections (CMEs) from the Sun that are directed towards the Earth, or by their associated shocks. Methods. We used the muon data at cutoff rigidities ranging from 14 to 24 GV from the GRAPES-3 tracking muon telescope to identify FD events. We selected those FD events that have a reasonably clean profile, and can be reasonably well associated with an Earth-directed CME and its associated shock. We employed two models: one that considers the CME as the sole cause of the FD (the CME-only model) and one that considers the shock as the only agent causing the FD (the shock-only model). We used an extensive set of observationally determined parameters for both models. The only free parameter in these models is the level of MHD turbulence in the sheath region, which mediates cosmic ray diffusion (into the CME for the CME-only model, and across the shock sheath for the shock-only model). Results. We find that good fits to the GRAPES-3 multi-rigidity data using the CME-only model require turbulence levels in the CME sheath region that are only slightly higher than those estimated for the quiescent solar wind. On the other hand, reasonable model fits with the shock-only model require turbulence levels in the sheath region that are an order of magnitude higher than those in the quiet solar wind. Conclusions. This observation naturally leads to the conclusion that the Earth-directed CMEs are the primary contributors to FDs observed in high-rigidity cosmic rays.
Brain | 2007
Masato Hasegawa; Tetsuaki Arai; Haruhiko Akiyama; T. Nonaka; Hiroshi Mori; Tomoyo Hashimoto; Mineo Yamazaki; Kiyomitsu Oyanagi
The composition and energy spectrum of primary cosmic rays (PCRs) are the only observables at high energies to study the nature of sources accelerating PCRs to �1000 TeV. These observables have been directly measured up to ∼300 TeV with detectors aboard balloons and satellites. But measurements at >1000 TeV have to be obtained indirectly from ground-based observations of extensive air showers. However, their interpretation relies on an inadequate knowledge of hadronic interactions at �1000 TeV. The GRAPES-3 experiment is designed to operate at �30 TeV providing a sizable overlap in energy with direct measurements, enabling the selection of a suitable model of hadronic interactions at ∼1000 TeV. We present salient features of GRAPES-3 including details of muon multiplicity distributions observed with a 560 m 2 detector as a function of shower size from an analysis of data of 545 days. These distributions were compared with expectations from Monte Carlo simulations, using some of the hadronic interaction generators in CORSIKA, to deduce energy spectra of five nuclear groups in the 100–1000 TeV region. A comparison of GRAPES-3 results with direct measurements indicates that SIBYLL provides a good description of hadronic interactions for interpreting our data. These measurements extend energy spectra and composition of PCRs that is consistent with extrapolation of direct measurements. (Some figures may appear in colour only in the online journal)
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
Solar flares accelerate charged particles through a variety of mechanisms, which may be constrained through observations at high energies (>10 GeV). We report here a search for direct emission of protons of energy (greater-or-similar sign)20 GeV in association with an X17 class solar flare that occurred on 28 October 2003, using a large area tracking muon telescope of the GRAPES-3 experiment at Ooty. Some features of the telescope, including its novel capability of high sensitivity search for the directional enhancement of the solar protons are also described. A 99% C.L. upper limit on the flux of protons due to the solar flare has been placed at 1.4x10{sup -6} cm{sup -2} s{sup -1} sr{sup -1}. A separate upper limit on the narrow solid angle flux of protons at 4x10{sup -6} cm{sup -2} s{sup -1} sr{sup -1} is also placed. Solar flares are also associated with coronal mass ejections, which propagate through the interplanetary space producing geomagnetic storms and Forbush decrease (Fd) events, upon their arrival at the Earth. New information on the structure and time evolution of the large Fd observed on 29 October 2003 by GRAPES-3 is presented. The onset of Fd in nine different solid angle bins ({approx}0.3 sr)morexa0» shows a remarkably similar behavior, with an evolution on a time scale of {approx}1 h. A power law dependence of the magnitude of the Fd on the cutoff rigidity has been derived, using the data from tracking muon telescope, over a narrow range of cutoff rigidity 14.3-24.0 GV, which shows a spectral slope {gamma}=0.53{+-}0.04, in agreement with earlier measurements.«xa0less
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
Astroparticle Physics | 2009
P. K. Mohanty; S.R. Dugad; U. D. Goswami; Sourendu Gupta; Y. Hayashi; A. Iyer; N. Ito; P. Jagadeesan; A. Jain; S. Karthikeyan; S. Kawakami; M. Minamino; S.D. Morris; P.K. Nayak; T. Nonaka; A. Oshima; B.S. Rao; K. C. Ravindran; H. Tanaka; S. C. Tonwar
Archive | 2009
T. Nonaka; Tetsuaki Arai; Haruhiko Akiyama; Masato Hasegawa; Makiko Yamashita