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K. Ishihara

Other affiliations: Tohoku University
Bio: K. Ishihara is an academic researcher from University of Tokyo. The author has contributed to research in topics: Neutrino & Neutrino oscillation. The author has an hindex of 41, co-authored 56 publications receiving 13902 citations. Previous affiliations of K. Ishihara include Tohoku University.


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 Haines4, Todd Haines10, E. Blaufuss11, B. K. Kim11, R. Sanford11, R. Svoboda11, M. L. Chen12, Z. Conner12, Z. Conner13, 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. Wai23, L. Wai22, 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
T. Araki1, K. Eguchi1, Sanshiro Enomoto1, K. Furuno1, Koichi Ichimura, H. Ikeda, Kunio Inoue, K. Ishihara2, K. Ishihara1, T. Iwamoto2, T. Iwamoto1, 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. Dwyer5, D. A. Dwyer6, Stuart J. Freedman5, Stuart J. Freedman6, Y. Fu6, Y. Fu5, B. K. Fujikawa5, B. K. Fujikawa6, J. Goldman5, J. Goldman6, Frederick Gray5, Frederick Gray6, K. M. Heeger5, K. M. Heeger6, K. T. Lesko6, K. T. Lesko5, Kam Biu Luk6, Kam Biu Luk5, Hitoshi Murayama5, Hitoshi Murayama6, A. W. P. Poon5, A. W. P. Poon6, H. M. Steiner6, H. M. Steiner5, 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 Karwowski16, Hugon J Karwowski15, D. M. Markoff16, D. M. Markoff15, J. A. Messimore15, J. A. Messimore16, Koji Nakamura16, Koji Nakamura15, Ryan Rohm15, Ryan Rohm16, Werner Tornow16, Werner Tornow15, R. Wendell15, R. Wendell16, Albert Young16, Albert Young15, 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
Y. Ashie1, J. Hosaka1, K. Ishihara1, Yoshitaka Itow1, J. Kameda1, Yusuke Koshio1, A. Minamino1, C. Mitsuda1, M. Miura1, Shigetaka Moriyama1, Masayuki Nakahata1, Toshio Namba1, R. Nambu1, Y. Obayashi1, Masato Shiozawa1, Yoshihiro Suzuki1, Y. Takeuchi1, K. Taki1, Shinya Yamada1, M. Ishitsuka1, Takaaki Kajita1, K. Kaneyuki1, Shoei Nakayama1, A. Okada1, Ko Okumura1, C. Saji1, Y. Takenaga1, S. Clark2, Shantanu Desai2, E. Kearns2, S. Likhoded2, J. L. Stone2, L. R. Sulak2, W. Wang2, M. Goldhaber3, David William Casper4, J. P. Cravens4, W. Gajewski4, W. R. Kropp4, D. W. Liu4, S. Mine4, Michael B. Smy4, Henry W. Sobel4, C. W. Sterner4, Mark R. Vagins4, K. S. Ganezer5, John Hill5, W. E. Keig5, J. S. Jang6, J. Y. Kim6, I. T. Lim6, Kate Scholberg7, C. W. Walter7, R. W. Ellsworth8, S. Tasaka9, G. Guillian, A. Kibayashi, John G. Learned, S. Matsuno, D. Takemori, M. D. Messier10, Y. Hayato, A. K. Ichikawa, T. Ishida, T. Ishii, T. Iwashita, Takashi Kobayashi, T. Maruyama11, Koji Nakamura, K. Nitta, Yuichi Oyama, Makoto Sakuda12, Y. Totsuka, Atsumu Suzuki13, Masaya Hasegawa14, K. Hayashi14, I. Kato14, H. Maesaka14, Taichi Morita14, Tsuyoshi Nakaya14, K. Nishikawa14, T. Sasaki14, S. Ueda14, Shoji Yamamoto14, Todd Haines4, Todd Haines15, S. Dazeley16, S. Hatakeyama16, R. Svoboda16, E. Blaufuss17, J. A. Goodman17, G. W. Sullivan17, D. Turcan17, Alec Habig18, Y. Fukuda19, C. K. Jung20, T. Kato20, Katsuhiro Kobayashi20, Magdalena Malek20, C. Mauger20, C. McGrew20, A. Sarrat20, E. Sharkey20, C. Yanagisawa20, T. Toshito21, Kazumasa Miyano22, N. Tamura22, J. Ishii23, Y. Kuno23, Minoru Yoshida23, S. B. Kim24, J. Yoo24, H. Okazawa, T. Ishizuka25, Y. Choi26, H. Seo26, Y. Gando27, Takehisa Hasegawa27, Kunio Inoue27, J. Shirai27, A. Suzuki27, Masatoshi Koshiba1, Y. Nakajima28, Kyoshi Nishijima28, T. Harada29, Hirokazu Ishino29, Y. Watanabe29, D. Kielczewska30, D. Kielczewska4, J. Zalipska30, H. G. Berns31, R. Gran31, K. K. Shiraishi31, A. L. Stachyra31, K. Washburn31, R. J. Wilkes31 
TL;DR: In this article, a combined analysis of fully-contained, partially-contained and upward-going muon atmospheric neutrino data from a 1489 d exposure of the Super-Kamiokande detector is presented.
Abstract: We present a combined analysis of fully-contained, partially-contained and upward-going muon atmospheric neutrino data from a 1489 d exposure of the Super-Kamiokande detector. The data samples span roughly five decades in neutrino energy, from 100 MeV to 10 TeV. A detailed Monte Carlo comparison is described and presented. The data is fit to the Monte Carlo expectation, and is found to be consistent with neutrino oscillations of {nu}{sub {mu}}{r_reversible}{nu}{sub {tau}} with sin{sup 2}2{theta}>0.92 and 1.5x10{sup -3}<{delta}m{sup 2}<3.4x10{sup -3} eV{sup 2} at 90% confidence level.

701 citations

Journal ArticleDOI
Y. Fukuda1, T. Hayakawa1, E. Ichihara1, Kunio Inoue1, K. Ishihara1, H. Ishino1, Yoshitaka Itow1, Takaaki Kajita1, J. Kameda1, S. Kasuga1, K. Kobayashi1, Yohei Kobayashi1, Yusuke Koshio1, K. Martens1, M. Miura1, Masayuki Nakahata1, S. Nakayama1, A. Okada1, M. Oketa1, Ko Okumura1, M. Ota1, N. Sakurai1, Masato Shiozawa1, Yasunari Suzuki1, Y. Takeuchi1, Y. Totsuka1, Shinya Yamada1, M. Earl2, Alec Habig2, J. T. Hong2, E. Kearns2, S. B. Kim2, S. B. Kim3, M. Masuzawa2, M. D. Messier2, Kate Scholberg2, J. L. Stone2, L. R. Sulak2, C. W. Walter2, M. Goldhaber4, T. Barszczak5, W. Gajewski5, P. G. Halverson5, J. Hsu5, W. R. Kropp5, L. R. Price5, Frederick Reines5, H. W. Sobel5, Mark R. Vagins5, K. S. Ganezer6, W. E. Keig6, R. W. Ellsworth7, S. Tasaka8, J. W. Flanagan9, A. Kibayashi9, John G. Learned9, S. Matsuno9, V. J. Stenger9, D. Takemori9, T. Ishii, Junichi Kanzaki, T. Kobayashi, K. Nakamura, K. Nishikawa, Yuichi Oyama, A. Sakai, Makoto Sakuda, Osamu Sasaki, S. Echigo10, M. Kohama10, A. T. Suzuki10, Todd Haines5, Todd Haines11, E. Blaufuss12, R. Sanford12, R. Svoboda12, M. L. Chen13, Z. Conner14, Z. Conner13, J. A. Goodman13, G. W. Sullivan13, Masaki Mori15, Masaki Mori1, J. Hill16, C. K. Jung16, C. Mauger16, C. McGrew16, E. Sharkey16, B. Viren16, C. Yanagisawa16, W. Doki17, T. Ishizuka18, T. Ishizuka17, Y. Kitaguchi17, H. Koga17, Kazumasa Miyano17, H. Okazawa17, C. Saji17, M. Takahata17, A. Kusano19, Y. Nagashima19, M. Takita19, T. Yamaguchi19, Minoru Yoshida19, M. Etoh20, K. Fujita20, Akira Hasegawa20, Takehisa Hasegawa20, S. Hatakeyama20, T. Iwamoto20, T. Kinebuchi20, M. Koga20, T. Maruyama20, Hiroshi Ogawa20, A. Suzuki20, F. Tsushima20, Masatoshi Koshiba1, M. Nemoto21, Kyoshi Nishijima21, T. Futagami22, Y. Hayato22, Y. Kanaya22, K. Kaneyuki22, Y. Watanabe22, D. Kielczewska5, D. Kielczewska23, R. A. Doyle24, J. S. George24, A. L. Stachyra24, L. Wai24, J. Wilkes24, K. K. Young24 
TL;DR: The first results of the solar neutrino flux measurement from Super-Kamiokande are presented in this article, where the results are obtained from data taken between 31 May 1996, and 23 June 1997.
Abstract: The first results of the solar neutrino flux measurement from Super-Kamiokande are presented. The results shown here are obtained from data taken between 31 May 1996, and 23 June 1997. Using our measurement of recoil electrons with energies above 6.5 MeV, we infer the total flux of ${}^{8}\mathrm{B}$ solar neutrinos to be $2.42\ifmmode\pm\else\textpm\fi{}0.06(\mathrm{stat}{)}_{\ensuremath{-}0.07}^{+0.10}(\mathrm{syst})\ifmmode\times\else\texttimes\fi{}{10}^{6}\mathrm{cm}{}^{\ensuremath{-}2}{\mathrm{s}}^{\ensuremath{-}1}$. This result is consistent with the Kamiokande measurement and is 36% of the flux predicted by the BP95 solar model. The flux is also measured in 1.5 month subsets and shown to be consistent with a constant rate.

677 citations

Journal ArticleDOI
M. H. Ahn1, E. Aliu2, S. Andringa2, Shigeki Aoki3  +217 moreInstitutions (29)
TL;DR: In this article, measurements of {nu}{sub {mu}} disappearance in K2K, the KEK to Kamioka long-baseline neutrino oscillation experiment are presented.
Abstract: We present measurements of {nu}{sub {mu}} disappearance in K2K, the KEK to Kamioka long-baseline neutrino oscillation experiment. One-hundred and twelve beam-originated neutrino events are observed in the fiducial volume of Super-Kamiokande with an expectation of 158.1{sub -8.6}{sup +9.2} events without oscillation. A distortion of the energy spectrum is also seen in 58 single-ring muonlike events with reconstructed energies. The probability that the observations are explained by the expectation for no neutrino oscillation is 0.0015% (4.3{sigma}). In a two-flavor oscillation scenario, the allowed {delta}m{sup 2} region at sin{sup 2}2{theta}=1 is between 1.9 and 3.5x10{sup -3} eV{sup 2} at the 90% C.L. with a best-fit value of 2.8x10{sup -3} eV{sup 2}.

672 citations


Cited by
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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

Journal ArticleDOI
TL;DR: In this paper, the authors employed a matrix-based power spectrum estimation method using pseudo-Karhunen-Loeve eigenmodes, producing uncorrelated minimum-variance measurements in 20 k-bands of both the clustering power and its anisotropy due to redshift-space distortions.
Abstract: We measure the large-scale real-space power spectrum P(k) using luminous red galaxies (LRGs) in the Sloan Digital Sky Survey (SDSS) and use this measurement to sharpen constraints on cosmological parameters from the Wilkinson Microwave Anisotropy Probe (WMAP). We employ a matrix-based power spectrum estimation method using Pseudo-Karhunen-Loeve eigenmodes, producing uncorrelated minimum-variance measurements in 20 k-bands of both the clustering power and its anisotropy due to redshift-space distortions, with narrow and well-behaved window functions in the range 0.01h/Mpc 0.1h/Mpc and associated nonlinear complications, yet agree well with more aggressive published analyses where nonlinear modeling is crucial.

1,481 citations

Journal ArticleDOI
Luca Amendola1, Stephen Appleby2, Anastasios Avgoustidis3, David Bacon4, Tessa Baker5, Marco Baldi6, Marco Baldi7, Marco Baldi8, Nicola Bartolo7, Nicola Bartolo9, Alain Blanchard10, Camille Bonvin11, Stefano Borgani7, Stefano Borgani12, Enzo Branchini13, Enzo Branchini7, Clare Burrage3, Stefano Camera, Carmelita Carbone7, Carmelita Carbone14, 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 Vernizzi39, 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

Journal ArticleDOI
TL;DR: In this paper, the cosmological results from a combined analysis of galaxy clustering and weak gravitational lensing, using 1321 deg2 of griz imaging data from the first year of the Dark Energy Survey (DES Y1), were presented.
Abstract: We present cosmological results from a combined analysis of galaxy clustering and weak gravitational lensing, using 1321 deg2 of griz imaging data from the first year of the Dark Energy Survey (DES Y1). We combine three two-point functions: (i) the cosmic shear correlation function of 26 million source galaxies in four redshift bins, (ii) the galaxy angular autocorrelation function of 650,000 luminous red galaxies in five redshift bins, and (iii) the galaxy-shear cross-correlation of luminous red galaxy positions and source galaxy shears. To demonstrate the robustness of these results, we use independent pairs of galaxy shape, photometric-redshift estimation and validation, and likelihood analysis pipelines. To prevent confirmation bias, the bulk of the analysis was carried out while "blind" to the true results; we describe an extensive suite of systematics checks performed and passed during this blinded phase. The data are modeled in flat ΛCDM and wCDM cosmologies, marginalizing over 20 nuisance parameters, varying 6 (for ΛCDM) or 7 (for wCDM) cosmological parameters including the neutrino mass density and including the 457×457 element analytic covariance matrix. We find consistent cosmological results from these three two-point functions and from their combination obtain S8≡σ8(Ωm/0.3)0.5=0.773-0.020+0.026 and Ωm=0.267-0.017+0.030 for ΛCDM; for wCDM, we find S8=0.782-0.024+0.036, Ωm=0.284-0.030+0.033, and w=-0.82-0.20+0.21 at 68% C.L. The precision of these DES Y1 constraints rivals that from the Planck cosmic microwave background measurements, allowing a comparison of structure in the very early and late Universe on equal terms. Although the DES Y1 best-fit values for S8 and Ωm are lower than the central values from Planck for both ΛCDM and wCDM, the Bayes factor indicates that the DES Y1 and Planck data sets are consistent with each other in the context of ΛCDM. Combining DES Y1 with Planck, baryonic acoustic oscillation measurements from SDSS, 6dF, and BOSS and type Ia supernovae from the Joint Lightcurve Analysis data set, we derive very tight constraints on cosmological parameters: S8=0.802±0.012 and Ωm=0.298±0.007 in ΛCDM and w=-1.00-0.04+0.05 in wCDM. Upcoming Dark Energy Survey analyses will provide more stringent tests of the ΛCDM model and extensions such as a time-varying equation of state of dark energy or modified gravity.

1,201 citations