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M. Koga

Bio: M. Koga is an academic researcher from Tohoku University. The author has contributed to research in topics: Neutrino & Neutrino oscillation. The author has an hindex of 30, co-authored 46 publications receiving 12490 citations. Previous affiliations of M. Koga include Institute for the Physics and Mathematics of the Universe.


Papers
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Journal ArticleDOI
Y. Fukuda1, T. Hayakawa1, E. Ichihara1, Kunio Inoue1, K. Ishihara1, H. Ishino1, Yoshitaka Itow1, Takaaki Kajita1, J. Kameda1, S. Kasuga1, Ken-ichiro Kobayashi1, Yohei Kobayashi1, Yusuke Koshio1, M. Miura1, Masayuki Nakahata1, S. Nakayama1, A. Okada1, Ko Okumura1, N. Sakurai1, Masato Shiozawa1, Yoshihiro Suzuki1, Y. Takeuchi1, Y. Totsuka1, Shinya Yamada1, M. Earl2, Alec Habig2, E. Kearns2, M. D. Messier2, Kate Scholberg2, J. L. Stone2, Lawrence Sulak2, C. W. Walter2, M. Goldhaber3, T. Barszczxak4, D. Casper4, W. Gajewski4, P. G. Halverson4, J. Hsu4, W. R. Kropp4, L. R. Price4, Frederick Reines4, Michael B. Smy4, Henry W. Sobel4, Mark R. Vagins4, K. S. Ganezer5, W. E. Keig5, R. W. Ellsworth6, S. Tasaka7, J. W. Flanagan8, A. Kibayashi8, John G. Learned8, S. Matsuno8, V. J. Stenger8, D. Takemori8, T. Ishii, Junichi Kanzaki, T. Kobayashi, S. Mine, K. Nakamura, K. Nishikawa, Yuichi Oyama, A. Sakai, Makoto Sakuda, Osamu Sasaki, S. Echigo9, M. Kohama9, A. T. Suzuki9, Todd Haines10, Todd Haines4, E. Blaufuss11, B. K. Kim11, R. Sanford11, R. Svoboda11, M. L. Chen12, Z. Conner13, Z. Conner12, J. A. Goodman12, G. W. Sullivan12, J. Hill14, C. K. Jung14, K. Martens14, C. Mauger14, C. McGrew14, E. Sharkey14, B. Viren14, C. Yanagisawa14, W. Doki15, Kazumasa Miyano15, H. Okazawa15, C. Saji15, M. Takahata15, Y. Nagashima16, M. Takita16, Takashi Yamaguchi16, Minoru Yoshida16, Soo-Bong Kim17, M. Etoh18, K. Fujita18, Akira Hasegawa18, Takehisa Hasegawa18, S. Hatakeyama18, T. Iwamoto18, M. Koga18, Tomoyuki Maruyama18, Hiroshi Ogawa18, J. Shirai18, A. Suzuki18, F. Tsushima18, Masatoshi Koshiba1, M. Nemoto19, Kyoshi Nishijima19, T. Futagami20, Y. Hayato20, Y. Kanaya20, K. Kaneyuki20, Y. Watanabe20, D. Kielczewska21, D. Kielczewska4, R. A. Doyle22, J. S. George22, A. L. Stachyra22, L. Wai22, L. Wai23, R. J. Wilkes22, K. K. Young22 
Abstract: We present an analysis of atmospheric neutrino data from a 33.0 kton yr (535-day) exposure of the Super-Kamiokande detector. The data exhibit a zenith angle dependent deficit of muon neutrinos which is inconsistent with expectations based on calculations of the atmospheric neutrino flux. Experimental biases and uncertainties in the prediction of neutrino fluxes and cross sections are unable to explain our observation. The data are consistent, however, with two-flavor ${\ensuremath{ u}}_{\ensuremath{\mu}}\ensuremath{\leftrightarrow}{\ensuremath{ u}}_{\ensuremath{\tau}}$ oscillations with ${sin}^{2}2\ensuremath{\theta}g0.82$ and $5\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}l\ensuremath{\Delta}{m}^{2}l6\ifmmode\times\else\texttimes\fi{}1{0}^{\ensuremath{-}3}\mathrm{eV}{}^{2}$ at 90% confidence level.

3,784 citations

Journal ArticleDOI
K. Eguchi1, Sanshiro Enomoto1, K. Furuno1, J. Goldman1, H. Hanada1, H. Ikeda, Kiyohiro Ikeda1, Kunio Inoue, K. Ishihara1, W. Itoh1, T. Iwamoto1, Tomoya Kawaguchi1, T. Kawashima1, H. Kinoshita1, Yasuhiro Kishimoto, M. Koga, Y. Koseki1, T. Maeda1, T. Mitsui, M. Motoki, K. Nakajima1, M. Nakajima1, T. Nakajima1, Hiroshi Ogawa1, K. Owada1, T. Sakabe1, I. Shimizu, J. Shirai1, F. Suekane, A. Suzuki1, K. Tada1, Osamu Tajima1, T. Takayama1, K. Tamae1, Hideki Watanabe, J. Busenitz2, Z. Djurcic2, K. McKinny2, Dongming Mei2, A. Piepke2, E. Yakushev2, B. E. Berger3, Y. D. Chan3, M. P. Decowski3, D. A. Dwyer3, Stuart J. Freedman3, Y. Fu3, B. K. Fujikawa3, K. M. Heeger3, K. T. Lesko3, K. B. Luk3, Hitoshi Murayama3, D. R. Nygren3, C. E. Okada3, A. W. P. Poon3, H. M. Steiner3, Lindley Winslow3, G. A. Horton-Smith4, R. D. McKeown4, J. Ritter4, B. Tipton4, Petr Vogel4, C. E. Lane5, T. Miletic5, Peter Gorham, G. Guillian, John G. Learned, J. Maricic, S. Matsuno, Sandip Pakvasa, S. Dazeley6, S. Hatakeyama6, M. Murakami6, R. Svoboda6, B. D. Dieterle7, M. DiMauro7, J. A. Detwiler8, Giorgio Gratta8, K. Ishii8, N. Tolich8, Y. Uchida8, M. Batygov9, W. M. Bugg9, H. O. Cohn9, Yuri Efremenko9, Yuri Kamyshkov9, A. Kozlov9, Y. Nakamura9, L. De Braeckeleer10, L. De Braeckeleer11, C. R. Gould11, C. R. Gould10, Hugon J Karwowski10, Hugon J Karwowski11, D. M. Markoff11, D. M. Markoff10, J. A. Messimore10, J. A. Messimore11, Koji Nakamura10, Koji Nakamura11, Ryan Rohm11, Ryan Rohm10, Werner Tornow11, Werner Tornow10, Albert Young11, Albert Young10, Y. F. Wang 
TL;DR: In the context of two-flavor neutrino oscillations with CPT invariance, all solutions to the solar neutrinos problem except for the "large mixing angle" region are excluded.
Abstract: KamLAND has measured the flux of ν _e’s from distant nuclear reactors. We find fewer ν _e events than expected from standard assumptions about ν _e propagation at the 99.95% C.L. In a 162 ton·yr exposure the ratio of the observed inverse β-decay events to the expected number without ν _e disappearance is 0.611±0.085(stat)±0.041(syst) for ν _e energies >3.4 MeV. In the context of two-flavor neutrino oscillations with CPT invariance, all solutions to the solar neutrino problem except for the “large mixing angle” region are excluded.

2,108 citations

Journal ArticleDOI
TL;DR: An improved search for neutrinoless double-beta (0νββ) decay of ^{136}Xe in the KamLAND-Zen experiment is presented and a significant reduction of the xenon-loaded liquid scintillator contaminant identified in previous searches is achieved.
Abstract: We present an improved search for neutrinoless double-beta (0νββ) decay of ^{136}Xe in the KamLAND-Zen experiment. Owing to purification of the xenon-loaded liquid scintillator, we achieved a significant reduction of the ^{110m}Ag contaminant identified in previous searches. Combining the results from the first and second phase, we obtain a lower limit for the 0νββ decay half-life of T_{1/2}^{0ν}>1.07×10^{26} yr at 90% C.L., an almost sixfold improvement over previous limits. Using commonly adopted nuclear matrix element calculations, the corresponding upper limits on the effective Majorana neutrino mass are in the range 61-165 meV. For the most optimistic nuclear matrix elements, this limit reaches the bottom of the quasidegenerate neutrino mass region.

1,055 citations

Journal ArticleDOI
T. Araki1, K. Eguchi1, Sanshiro Enomoto1, K. Furuno1, Koichi Ichimura, H. Ikeda, Kunio Inoue, K. Ishihara1, K. Ishihara2, T. Iwamoto1, T. Iwamoto2, T. Kawashima1, Yasuhiro Kishimoto, M. Koga, Y. Koseki1, T. Maeda1, T. Mitsui, M. Motoki, K. Nakajima1, Hiroshi Ogawa1, K. Owada1, J. S. Ricol1, I. Shimizu, J. Shirai, F. Suekane, A. Suzuki1, K. Tada1, Osamu Tajima1, K. Tamae, Y. Tsuda1, Hiroko Watanabe, J. Busenitz3, T. Classen3, Z. Djurcic3, G. Keefer3, K. McKinny3, Dongming Mei4, Dongming Mei3, A. Piepke3, E. Yakushev3, B. E. Berger5, B. E. Berger6, Y. D. Chan6, Y. D. Chan5, M. P. Decowski5, M. P. Decowski6, D. A. Dwyer6, D. A. Dwyer5, Stuart J. Freedman6, Stuart J. Freedman5, Y. Fu6, Y. Fu5, B. K. Fujikawa6, B. K. Fujikawa5, J. Goldman6, J. Goldman5, Frederick Gray6, Frederick Gray5, K. M. Heeger5, K. M. Heeger6, K. T. Lesko5, K. T. Lesko6, Kam Biu Luk6, Kam Biu Luk5, Hitoshi Murayama5, Hitoshi Murayama6, A. W. P. Poon5, A. W. P. Poon6, H. M. Steiner5, H. M. Steiner6, Lindley Winslow5, Lindley Winslow6, G. A. Horton-Smith7, G. A. Horton-Smith8, C. Mauger7, R. D. McKeown7, Petr Vogel7, C. E. Lane9, T. Miletic9, Peter Gorham, G. Guillian, John G. Learned, J. Maricic, S. Matsuno, Sandip Pakvasa, S. Dazeley10, S. Hatakeyama10, A. Rojas10, Robert Svoboda10, B. D. Dieterle11, J. A. Detwiler12, Giorgio Gratta12, K. Ishii12, N. Tolich12, Y. Uchida13, Y. Uchida12, M. Batygov14, W. M. Bugg14, Yuri Efremenko14, Y. Kamyshkov14, A. Kozlov14, Y. Nakamura14, C. R. Gould15, C. R. Gould16, Hugon J Karwowski15, Hugon J Karwowski16, D. M. Markoff16, D. M. Markoff15, J. A. Messimore16, J. A. Messimore15, Koji Nakamura16, Koji Nakamura15, Ryan Rohm15, Ryan Rohm16, Werner Tornow16, Werner Tornow15, R. Wendell16, R. Wendell15, Albert Young15, Albert Young16, M. J. Chen, Y. F. Wang, F. Piquemal17 
TL;DR: In this article, a study of neutrino oscillation based on a 766 ton/year exposure of KamLAND to reactor antineutrinos is presented, where the observed energy spectrum disagrees with the expected spectral shape.
Abstract: We present results of a study of neutrino oscillation based on a 766 ton/year exposure of KamLAND to reactor antineutrinos. We observe 258 [overline nu ]e candidate events with energies above 3.4 MeV compared to 365.2±23.7 events expected in the absence of neutrino oscillation. Accounting for 17.8±7.3 expected background events, the statistical significance for reactor [overline nu ]e disappearance is 99.998%. The observed energy spectrum disagrees with the expected spectral shape in the absence of neutrino oscillation at 99.6% significance and prefers the distortion expected from [overline nu ]e oscillation effects. A two-neutrino oscillation analysis of the KamLAND data gives Deltam2=7.9 -0.5 +0.6 ×10-5 eV2. A global analysis of data from KamLAND and solar-neutrino experiments yields Deltam2=7.9 -0.5 +0.6 ×10-5 eV2 and tan2theta=0.40 -0.07 +0.10 , the most precise determination to date.

992 citations

Journal ArticleDOI
S. Fukuda1, Y. Fukuda1, T. Hayakawa1, E. Ichihara1  +183 moreInstitutions (28)
TL;DR: Super-Kamiokande is the world's largest water Cherenkov detector, with net mass 50,000 tons as discussed by the authors, which collected 1678 live-days of data, observing neutrinos from the Sun, Earth's atmosphere, and the K2K long-baseline neutrino beam with high efficiency.
Abstract: Super-Kamiokande is the world's largest water Cherenkov detector, with net mass 50,000 tons. During the period April, 1996 to July, 2001, Super-Kamiokande I collected 1678 live-days of data, observing neutrinos from the Sun, Earth's atmosphere, and the K2K long-baseline neutrino beam with high efficiency. These data provided crucial information for our current understanding of neutrino oscillations, as well as setting stringent limits on nucleon decay. In this paper, we describe the detector in detail, including its site, configuration, data acquisition equipment, online and offline software, and calibration systems which were used during Super-Kamiokande I.

708 citations


Cited by
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28 Jul 2005
TL;DR: PfPMP1)与感染红细胞、树突状组胞以及胎盘的单个或多个受体作用,在黏附及免疫逃避中起关键的作�ly.
Abstract: 抗原变异可使得多种致病微生物易于逃避宿主免疫应答。表达在感染红细胞表面的恶性疟原虫红细胞表面蛋白1(PfPMP1)与感染红细胞、内皮细胞、树突状细胞以及胎盘的单个或多个受体作用,在黏附及免疫逃避中起关键的作用。每个单倍体基因组var基因家族编码约60种成员,通过启动转录不同的var基因变异体为抗原变异提供了分子基础。

18,940 citations

Journal ArticleDOI
TL;DR: In this article, the Wilkinson Microwave Anisotropy Probe (WMAP) 5-year data were used to constrain the physics of cosmic inflation via Gaussianity, adiabaticity, the power spectrum of primordial fluctuations, gravitational waves, and spatial curvature.
Abstract: The Wilkinson Microwave Anisotropy Probe (WMAP) 5-year data provide stringent limits on deviations from the minimal, six-parameter Λ cold dark matter model. We report these limits and use them to constrain the physics of cosmic inflation via Gaussianity, adiabaticity, the power spectrum of primordial fluctuations, gravitational waves, and spatial curvature. We also constrain models of dark energy via its equation of state, parity-violating interaction, and neutrino properties, such as mass and the number of species. We detect no convincing deviations from the minimal model. The six parameters and the corresponding 68% uncertainties, derived from the WMAP data combined with the distance measurements from the Type Ia supernovae (SN) and the Baryon Acoustic Oscillations (BAO) in the distribution of galaxies, are: Ω b h 2 = 0.02267+0.00058 –0.00059, Ω c h 2 = 0.1131 ± 0.0034, ΩΛ = 0.726 ± 0.015, ns = 0.960 ± 0.013, τ = 0.084 ± 0.016, and at k = 0.002 Mpc-1. From these, we derive σ8 = 0.812 ± 0.026, H 0 = 70.5 ± 1.3 km s-1 Mpc–1, Ω b = 0.0456 ± 0.0015, Ω c = 0.228 ± 0.013, Ω m h 2 = 0.1358+0.0037 –0.0036, z reion = 10.9 ± 1.4, and t 0 = 13.72 ± 0.12 Gyr. With the WMAP data combined with BAO and SN, we find the limit on the tensor-to-scalar ratio of r 1 is disfavored even when gravitational waves are included, which constrains the models of inflation that can produce significant gravitational waves, such as chaotic or power-law inflation models, or a blue spectrum, such as hybrid inflation models. We obtain tight, simultaneous limits on the (constant) equation of state of dark energy and the spatial curvature of the universe: –0.14 < 1 + w < 0.12(95%CL) and –0.0179 < Ω k < 0.0081(95%CL). We provide a set of WMAP distance priors, to test a variety of dark energy models with spatial curvature. We test a time-dependent w with a present value constrained as –0.33 < 1 + w 0 < 0.21 (95% CL). Temperature and dark matter fluctuations are found to obey the adiabatic relation to within 8.9% and 2.1% for the axion-type and curvaton-type dark matter, respectively. The power spectra of TB and EB correlations constrain a parity-violating interaction, which rotates the polarization angle and converts E to B. The polarization angle could not be rotated more than –59 < Δα < 24 (95% CL) between the decoupling and the present epoch. We find the limit on the total mass of massive neutrinos of ∑m ν < 0.67 eV(95%CL), which is free from the uncertainty in the normalization of the large-scale structure data. The number of relativistic degrees of freedom (dof), expressed in units of the effective number of neutrino species, is constrained as N eff = 4.4 ± 1.5 (68%), consistent with the standard value of 3.04. Finally, quantitative limits on physically-motivated primordial non-Gaussianity parameters are –9 < f local NL < 111 (95% CL) and –151 < f equil NL < 253 (95% CL) for the local and equilateral models, respectively.

5,904 citations

Journal ArticleDOI
TL;DR: In this article, the neutralino is proposed as the lightest superpartner in many supersymmetric theories, and it is shown how to calculate the cosmological abundance of neutralino and event rates for both direct and indirect detection schemes.

1,670 citations

01 Apr 2003
TL;DR: In this paper, the authors measured the flux of neutrino from distant nuclear reactors and found fewer nu;(e) events than expected from standard assumptions about nu; (e) propagation at the 99.95% C.L.yr exposure.
Abstract: KamLAND has measured the flux of nu;(e)'s from distant nuclear reactors. We find fewer nu;(e) events than expected from standard assumptions about nu;(e) propagation at the 99.95% C.L. In a 162 ton.yr exposure the ratio of the observed inverse beta-decay events to the expected number without nu;(e) disappearance is 0.611+/-0.085(stat)+/-0.041(syst) for nu;(e) energies >3.4 MeV. In the context of two-flavor neutrino oscillations with CPT invariance, all solutions to the solar neutrino problem except for the "large mixing angle" region are excluded.

1,659 citations

Journal ArticleDOI
Luca Amendola1, Stephen Appleby2, Anastasios Avgoustidis3, David Bacon4, Tessa Baker5, Marco Baldi6, Marco Baldi7, Marco Baldi8, Nicola Bartolo9, Nicola Bartolo7, Alain Blanchard10, Camille Bonvin11, Stefano Borgani12, Stefano Borgani7, Enzo Branchini13, Enzo Branchini7, Clare Burrage3, Stefano Camera, Carmelita Carbone14, Carmelita Carbone7, Luciano Casarini15, Luciano Casarini16, Mark Cropper17, Claudia de Rham18, J. P. Dietrich19, Cinzia Di Porto, Ruth Durrer11, Anne Ealet, Pedro G. Ferreira5, Fabio Finelli7, Juan Garcia-Bellido20, Tommaso Giannantonio19, Luigi Guzzo7, Luigi Guzzo14, Alan Heavens18, Lavinia Heisenberg21, Catherine Heymans22, Henk Hoekstra23, Lukas Hollenstein, Rory Holmes, Zhiqi Hwang24, Knud Jahnke25, Thomas D. Kitching17, Tomi S. Koivisto26, Martin Kunz11, Giuseppe Vacca27, Eric V. Linder28, M. March29, Valerio Marra30, Carlos Martins31, Elisabetta Majerotto11, Dida Markovic32, David J. E. Marsh33, Federico Marulli7, Federico Marulli6, Richard Massey34, Yannick Mellier35, Francesco Montanari36, David F. Mota16, Nelson J. Nunes37, Will J. Percival32, Valeria Pettorino38, Valeria Pettorino39, Cristiano Porciani, Claudia Quercellini, Justin I. Read40, Massimiliano Rinaldi41, Domenico Sapone42, Ignacy Sawicki43, Roberto Scaramella, Constantinos Skordis44, Constantinos Skordis43, Fergus Simpson45, Andy Taylor22, Shaun A. Thomas, Roberto Trotta18, Licia Verde45, Filippo Vernizzi38, Adrian Vollmer, Yun Wang46, Jochen Weller19, T. G. Zlosnik47 
TL;DR: Euclid is a European Space Agency medium-class mission selected for launch in 2020 within the cosmic vision 2015-2025 program as discussed by the authors, which will explore the expansion history of the universe and the evolution of cosmic structures by measuring shapes and red-shift of galaxies as well as the distribution of clusters of galaxies over a large fraction of the sky.
Abstract: Euclid is a European Space Agency medium-class mission selected for launch in 2020 within the cosmic vision 2015–2025 program. The main goal of Euclid is to understand the origin of the accelerated expansion of the universe. Euclid will explore the expansion history of the universe and the evolution of cosmic structures by measuring shapes and red-shifts of galaxies as well as the distribution of clusters of galaxies over a large fraction of the sky. Although the main driver for Euclid is the nature of dark energy, Euclid science covers a vast range of topics, from cosmology to galaxy evolution to planetary research. In this review we focus on cosmology and fundamental physics, with a strong emphasis on science beyond the current standard models. We discuss five broad topics: dark energy and modified gravity, dark matter, initial conditions, basic assumptions and questions of methodology in the data analysis. This review has been planned and carried out within Euclid’s Theory Working Group and is meant to provide a guide to the scientific themes that will underlie the activity of the group during the preparation of the Euclid mission.

1,211 citations