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Showing papers by "Tsuyoshi Nakaya published in 2006"


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


Journal ArticleDOI
J. P. Cravens1, K. Abe2, T. Iida2, K. Ishihara2  +147 moreInstitutions (34)
TL;DR: The results of the second phase of the Super-Kamiokande solar neutrino measurement are presented and compared to the first phase in this paper, showing no evidence of systematic tendencies between the first and second phases.
Abstract: The results of the second phase of the Super-Kamiokande solar neutrino measurement are presented and compared to the first phase. The solar neutrino flux spectrum and time variation as well as oscillation results are statistically consistent with the first phase and do not show spectral distortion. The time-dependent flux measurement of the combined first and second phases coincides with the full period of solar cycle 23 and shows no correlation with solar activity. The measured {sup 8}B total flux is (2.38{+-}0.05(stat.){sub -0.15}{sup +0.16}(sys.))x10{sup 6} cm{sup -2} s{sup -1} and the day-night difference is found to be (-6.3{+-}4.2(stat.){+-}3.7(sys.))%. There is no evidence of systematic tendencies between the first and second phases.

439 citations


Journal ArticleDOI
J. Hosaka1, K. Ishihara1, J. Kameda1, Yusuke Koshio1, A. Minamino1, C. Mitsuda1, M. Miura1, Shigetaka Moriyama1, Masayuki Nakahata1, Toshio Namba1, Y. Obayashi1, Masato Shiozawa1, Yasunari Suzuki1, Atsushi Takeda1, Y. Takeuchi1, Shinya Yamada1, I. Higuchi1, M. Ishitsuka1, Takaaki Kajita1, K. Kaneyuki1, G. Mitsuka1, Shoei Nakayama1, H. Nishino1, A. Okada1, Ko Okumura1, C. Saji1, Y. Takenaga1, S. Clark2, Shantanu Desai3, Shantanu Desai2, E. Kearns2, S. Likhoded2, J. L. Stone2, L. R. Sulak2, W. Wang2, M. Goldhaber4, David William Casper5, J. P. Cravens5, W. R. Kropp5, D. W. Liu5, S. Mine5, C. Regis5, Michael B. Smy5, Henry W. Sobel5, C. W. Sterner5, Mark R. Vagins5, K. S. Ganezer6, J. Hill6, W. E. Keig6, J. S. Jang7, J. Y. Kim7, I. T. Lim7, Kate Scholberg8, C. W. Walter8, R. A. Wendell8, R. W. Ellsworth9, Shigeki Tasaka10, E. Guillian, A. Kibayashi, J. G. Learned, S. Matsuno, M. D. Messier11, Y. Hayato1, A. K. Ichikawa, T. Ishida, T. Ishii, T. Iwashita, T. Kobayashi, T. Nakadaira, K. Nakamura, K. Nitta, Yuichi Oyama, Y. Totsuka, Atsumu Suzuki12, Masaya Hasegawa13, I. Kato13, I. Kato14, H. Maesaka13, Tsuyoshi Nakaya13, K. Nishikawa13, Takanori Sasaki13, Hiroshi Sato13, Shoji Yamamoto13, Masashi Yokoyama13, T. J. Haines15, T. J. Haines5, S. Dazeley16, S. Hatakeyama16, R. Svoboda16, E. Blaufuss17, J. A. Goodman17, G. W. Sullivan17, D. Turcan17, Jodi Cooley18, Alec Habig19, Y. Fukuda20, T. Sato20, Yoshitaka Itow21, C. K. Jung22, T. Kato22, Katsuhiro Kobayashi22, M. Malek22, C. Mauger22, C. McGrew22, A. Sarrat1, A. Sarrat22, C. Yanagisawa22, N. Tamura23, Makoto Sakuda24, Yoshitaka Kuno25, Minoru Yoshida25, S. B. Kim26, J. Yoo26, T. Ishizuka27, H. Okazawa27, Y. Choi28, H. Seo28, Y. Gando29, Takehisa Hasegawa29, Kunio Inoue29, J. Shirai29, A. Suzuki29, Kyoshi Nishijima30, Hirokazu Ishino31, Y. Watanabe31, Masatoshi Koshiba1, D. Kielczewska32, D. Kielczewska5, J. Zalipska32, H. G. Berns33, R. Gran19, R. Gran33, K. K. Shiraishi33, A. L. Stachyra33, K. Washburn33, R. J. Wilkes33 
TL;DR: In this article, the results of a three-flavor oscillation analysis using Super-Kamiokande I atmospheric neutrino data, with the assumption of one mass scale dominance, were reported.
Abstract: We report on the results of a three-flavor oscillation analysis using Super-Kamiokande I atmospheric neutrino data, with the assumption of one mass scale dominance ($\ensuremath{\Delta}{m}_{12}^{2}=0$). No significant flux change due to matter effect, which occurs when neutrinos propagate inside the Earth for ${\ensuremath{\theta}}_{13}\ensuremath{ e}0$, has been seen either in a multi-GeV ${\ensuremath{ u}}_{e}$-rich sample or in a ${\ensuremath{ u}}_{\ensuremath{\mu}}$-rich sample. Both normal and inverted mass hierarchy hypotheses are tested and both are consistent with observation. Using Super-Kamiokande data only, 2-dimensional 90% confidence allowed regions are obtained: mixing angles are constrained to ${sin }^{2}{\ensuremath{\theta}}_{13}l0.14$ and $0.37l{sin }^{2}{\ensuremath{\theta}}_{23}l0.65$ for the normal mass hierarchy. Weaker constraints, ${sin }^{2}{\ensuremath{\theta}}_{13}l0.27$ and $0.37l{sin }^{2}{\ensuremath{\theta}}_{23}l0.69$, are obtained for the inverted mass hierarchy case.

155 citations


Journal ArticleDOI
R. Gran1, R. Gran2, E. J. Jeon3, E. Aliu4  +160 moreInstitutions (29)
TL;DR: In this paper, the weak nucleon axial-vector form factor for quasielastic interactions was determined using neutrino interaction data from the K2K Scintillating Fiber detector.
Abstract: The weak nucleon axial-vector form factor for quasielastic interactions is determined using neutrino interaction data from the K2K Scintillating Fiber detector in the neutrino beam at KEK. More than 12 000 events are analyzed, of which half are charged-current quasielastic interactions ${\ensuremath{ u}}_{\ensuremath{\mu}}n\ensuremath{\rightarrow}{\ensuremath{\mu}}^{\ensuremath{-}}p$ occurring primarily in oxygen nuclei. We use a relativistic Fermi gas model for oxygen and assume the form factor is approximately a dipole with one parameter, the axial-vector mass ${M}_{A}$, and fit to the shape of the distribution of the square of the momentum transfer from the nucleon to the nucleus. Our best fit result for ${M}_{A}=1.20\ifmmode\pm\else\textpm\fi{}0.12\text{ }\text{ }\mathrm{GeV}$. Furthermore, this analysis includes updated vector form factors from recent electron scattering experiments and a discussion of the effects of the nucleon momentum on the shape of the fitted distributions.

135 citations


Journal ArticleDOI
K. Abe1, Y. Hayato1, T. Iida1, K. Ishihara1, J. Kameda1, Yusuke Koshio1, A. Minamino1, C. Mitsuda1, M. Miura1, Shigetaka Moriyama1, Masayuki Nakahata1, Y. Obayashi1, H. Ogawa1, Masato Shiozawa1, Yasunari Suzuki1, Atsushi Takeda1, Y. Takeuchi1, K. Ueshima1, I. Higuchi1, C. Ishihara1, M. Ishitsuka1, Takaaki Kajita1, K. Kaneyuki1, G. Mitsuka1, Shoei Nakayama1, H. Nishino1, Ko Okumura1, C. Saji1, Y. Takenaga1, Y. Totsuka1, S. Clark2, Shantanu Desai2, Frédéric Dufour2, E. Kearns2, S. Likhoded2, Michael Litos2, J. L. Raaf2, J. L. Stone2, L. R. Sulak2, W. Wang2, M. Goldhaber3, David William Casper4, J. P. Cravens4, W. R. Kropp4, D. W. Liu4, S. Mine4, C. Regis4, Michael B. Smy4, Henry W. Sobel4, Mark R. Vagins4, K. S. Ganezer5, J. Hill5, W. E. Keig5, J. S. Jang6, J. Y. Kim6, I. T. Lim6, Kate Scholberg7, N. Tanimoto7, C. W. Walter7, R. A. Wendell7, R. W. Ellsworth8, Shigeki Tasaka9, E. Guillian, J. G. Learned, S. Matsuno, M. D. Messier10, A. K. Ichikawa, T. Ishida, T. Ishii, T. Iwashita, T. Kobayashi, T. Nakadaira, K. Nakamura, K. Nitta, Yuichi Oyama, Atsumu Suzuki11, Masaya Hasegawa12, I. Kato12, H. Maesaka12, Tsuyoshi Nakaya12, K. Nishikawa12, Takanori Sasaki12, Hiroshi Sato12, Shoji Yamamoto12, Masashi Yokoyama12, Todd Haines13, S. Dazeley14, S. Hatakeyama14, R. Svoboda14, G. W. Sullivan15, Alec Habig16, R. Gran16, Y. Fukuda17, T. Sato17, Yoshitaka Itow18, T. Koike18, C. K. Jung19, T. Kato19, Katsuhiro Kobayashi19, M. Malek19, C. McGrew19, A. Sarrat1, A. Sarrat19, R. Terri19, C. Yanagisawa19, N. Tamura20, Makoto Sakuda21, M. Sugihara21, Y. Kuno22, Minoru Yoshida22, S. B. Kim23, J. Yoo23, T. Ishizuka24, H. Okazawa24, Y. Choi25, H. Seo25, Y. Gando26, Takehisa Hasegawa26, Kunio Inoue26, H. Ishii27, Kyoshi Nishijima27, Hirokazu Ishino28, Y. Watanabe28, Masatoshi Koshiba1, D. Kielczewska4, D. Kielczewska29, J. Zalipska29, H. G. Berns30, K. K. Shiraishi30, K. Washburn30, R. J. Wilkes30 
TL;DR: A search for the appearance of tau neutrino appearance from nu(mu) <--> nu(tau) oscillations in the atmospheric neutrinos has been performed using 1489.2 days of atmospheric neutRino data from the Super-Kamiokande-I experiment.
Abstract: A search for the appearance of tau neutrinos from ${\ensuremath{ u}}_{\ensuremath{\mu}}\ensuremath{\leftrightarrow}{\ensuremath{ u}}_{\ensuremath{\tau}}$ oscillations in the atmospheric neutrinos has been performed using 1489.2 days of atmospheric neutrino data from the Super-Kamiokande-I experiment. A best fit tau neutrino appearance signal of $138\ifmmode\pm\else\textpm\fi{}48(\mathrm{stat}{)}_{\ensuremath{-}32}^{+15}(\mathrm{syst})$ events is obtained with an expectation of $78\ifmmode\pm\else\textpm\fi{}26(\mathrm{syst})$. The hypothesis of no tau neutrino appearance is disfavored by 2.4 sigma.

92 citations


Journal ArticleDOI
M. G. Catanesi, M. T. Muciaccia, E. Radicioni, S. Simone, Rob Edgecock1, Malcolm Ellis1, S. Robbins1, F. J. P. Soler1, Claus Gößling2, M. Mass2, S.A. Bunyatov3, Artem Chukanov3, D. Dedovitch3, A. Elagin3, Mikhail Ivanovitch Gostkin3, A. Guskov3, D. Khartchenko3, O. Klimov3, A. Krasnoperov3, D. Kustov3, K. Nikolaev3, B. A. Popov3, V. Serdiouk3, V. Tereshchenko3, Alexey Zhemchugov3, E. Di Capua, G. Vidal-Sitjes, A. Artamonov4, P. Arce4, S. Gianì4, Simone Gilardoni4, P. Gorbunov4, A. Grant4, A. Grossheim4, P M Gruber4, Vladimir Ivanchenko4, A. Kayis-Topaksu4, L. Linssen4, J. Panman4, Ioannis Papadopoulos4, J. Pasternak4, E. Tcherniaev4, Ilya Tsukerman4, Rob Veenhof4, C. Wiebusch4, P. Zucchelli4, A. Blondel5, Silvia Borghi5, Manuela Campanelli5, A. Cervera-Villanueva5, M. C. Morone5, G. Prior5, R. Schroeter5, I. Kato6, Tsuyoshi Nakaya6, K. Nishikawa6, S. Ueda6, V. Ableev, U. Gastaldi, G.B. Mills7, J.S. Graulich8, Ghislain Grégoire8, M. Bonesini, Marta Calvi, A. De Min, Federico Ferri, Marco Paganoni, F. Paleari, Mikhail Kirsanov, A. Bagulya9, V. Grichine9, N. G. Polukhina9, V. Palladino, L. Coney10, D. W. Schmitz10, G.D. Barr11, A. De Santo11, C. Pattison11, Kai Zuber11, F. Bobisut, D. Gibin, A. Guglielmi, Marco Laveder, Alessandro Menegolli, M. Mezzetto, J. Dumarchez, S. Troquereau, F. Vannucci, V. V. Ammosov, V. A. Gapienko, V. I. Koreshev, A. Semak, Yu M. Sviridov, V. G. Zaets, U. Dore12, Domizia Orestano, M. Pasquali, Fr Pastore, A. Tonazzo, L. Tortora, C. N. Booth13, Craig Buttar13, Paul Hodgson13, L. Howlett13, M. Bogomilov14, M. Chizhov14, D. Kolev14, R. Tsenov14, S. Piperov15, Petar Temnikov15, M. Apollonio, P. Chimenti, G. Giannini, Giovanni Santin, Y. Hayato16, A. Ichikawa16, Takashi Kobayashi16, Jordi Burguet-Castell17, J.J. Gómez-Cadenas17, P. Novella17, M. Sorel17, A. Tornero17 
TL;DR: In this paper, the PS detector design, construction, commissioning, and operation is described and the authors gratefully acknowledge the help and support of the PS beam staff and of the numerous technical collaborators who contributed to the detector design and construction.

66 citations


Journal ArticleDOI
TL;DR: In this paper, an experimental strategy for resolving the octant degeneracy by combining reactor measurement of the T2K phase II experiment and a particle accelerator with an exposure of 10 GW was discussed.
Abstract: If the lepton mixing angle ${\ensuremath{\theta}}_{23}$ is not maximal, there arises a problem of ambiguity in determining ${\ensuremath{\theta}}_{23}$ due to the existence of two degenerate solutions, one in the first and the other in the second octant. We discuss an experimental strategy for resolving the ${\ensuremath{\theta}}_{23}$ octant degeneracy by combining reactor measurement of ${\ensuremath{\theta}}_{13}$ with accelerator ${\ensuremath{ u}}_{\ensuremath{\mu}}$ disappearance and ${\ensuremath{ u}}_{e}$ appearance experiments. The robustness of the ${\ensuremath{\theta}}_{23}$ degeneracy and the difficulty in lifting it only by accelerator experiments with conventional ${\ensuremath{ u}}_{\ensuremath{\mu}}$ (and ${\overline{\ensuremath{ u}}}_{\ensuremath{\mu}}$) beams are demonstrated by analytical and numerical treatments. Our method offers a way to overcome the difficulty and can resolve the degeneracy between solutions ${sin }^{2}{\ensuremath{\theta}}_{23}=0.4$ and ${sin }^{2}{\ensuremath{\theta}}_{23}=0.6$ if ${sin }^{2}2{\ensuremath{\theta}}_{13}\ensuremath{\gtrsim}0.05$ at 95% CL by assuming the T2K phase II experiment and a reactor measurement with an exposure of 10 GW\ifmmode\cdot\else\textperiodcentered\fi{}kt\ifmmode\cdot\else\textperiodcentered\fi{}yr. The dependence of the resolving power of the octant degeneracy on the systematic errors of reactor experiments is also examined.

58 citations


Journal ArticleDOI
Shoji Yamamoto1, J. Zalipska, E. Aliu2, S. Andringa2  +159 moreInstitutions (29)
TL;DR: In this paper, an improved search for the K2K long-baseline neutrino oscillation was performed using the full data sample of 9.2x10{sup 19} protons on target.
Abstract: We performed an improved search for {nu}{sub {mu}}{yields}{nu}{sub e} oscillation with the KEK to Kamioka (K2K) long-baseline neutrino oscillation experiment, using the full data sample of 9.2x10{sup 19} protons on target. No evidence for a {nu}{sub e} appearance signal was found, and we set bounds on the {nu}{sub {mu}}{yields}{nu}{sub e} oscillation parameters. At {delta}m{sup 2}=2.8x10{sup -3} eV{sup 2}, the best-fit value of the K2K {nu}{sub {mu}} disappearance analysis, we set an upper limit of sin{sup 2}2{theta}{sub {mu}}{sub e}<0.13 at a 90% confidence level.

43 citations


Proceedings ArticleDOI
01 Jan 2006
TL;DR: The multi-pixel photon counter (MPPC) as discussed by the authors is a newly developed photodetector with an excellent photon counting capability, it also has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature.
Abstract: The multi-pixel photon counter (MPPC) is a newly developed photodetector with an excellent photon counting capability. It also has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature. The basic performance of samples has been measured. A gain of ~106 is achieved with a noise rate less than 500 kHz with 1 p.e. threshold, and cross-talk probability of less than 40% at room temperature. The photon detection efficiency for green light is twice or more that of the photomultiplier tubes. It is found that the basic performance of the MPPC is satisfactory for use in real experiments.

38 citations


Journal ArticleDOI
K. Abe1, J. Hosaka1, T. Iida1, K. Ishihara1, J. Kameda1, Yusuke Koshio1, A. Minamino1, C. Mitsuda1, M. Miura1, Shigetaka Moriyama1, Masayuki Nakahata1, Y. Obayashi1, Hiroshi Ogawa1, Masato Shiozawa1, Yasunari Suzuki1, Atsushi Takeda1, Y. Takeuchi1, I. Higuchi1, C. Ishihara1, M. Ishitsuka1, Takaaki Kajita1, K. Kaneyuki1, G. Mitsuka1, Shoei Nakayama1, H. Nishino1, A. Okada1, Ko Okumura1, C. Saji1, Y. Takenaga1, S. Clark2, Shantanu Desai3, Shantanu Desai2, Frédéric Dufour2, E. Kearns2, S. Likhoded2, Michael Litos2, J. L. Raaf2, J. L. Stone2, Lawrence Sulak2, W. Wang2, M. Goldhaber4, David William Casper5, J. P. Cravens5, J. Dunmore5, W. R. Kropp5, D. W. Liu5, S. Mine5, C. Regis5, Michael B. Smy5, Henry W. Sobel5, Mark R. Vagins5, K. S. Ganezer6, John Hill6, W. E. Keig6, J. S. Jang7, J. Y. Kim7, I. T. Lim7, Kate Scholberg8, N. Tanimoto8, C. W. Walter8, R. A. Wendell8, R. W. Ellsworth9, Shigeki Tasaka10, G. Guillian11, John G. Learned11, S. Matsuno11, M. D. Messier12, Y. Hayato1, Y. Hayato13, A. K. Ichikawa13, T. Ishida13, T. Ishii13, T. Iwashita13, T. Kobayashi13, T. Nakadaira13, Koji Nakamura13, K. Nitta13, Yuichi Oyama13, Y. Totsuka13, Y. Totsuka1, Atsumu Suzuki14, Masaya Hasegawa15, Katsuki Hiraide15, I. Kato15, I. Kato16, H. Maesaka15, Tsuyoshi Nakaya15, K. Nishikawa15, Takanori Sasaki15, Hiroshi Sato15, Shoji Yamamoto15, Masashi Yokoyama15, T. J. Haines5, T. J. Haines17, S. Dazeley18, S. Hatakeyama18, R. Svoboda18, G. W. Sullivan19, D. Turcan19, M. E. C. Swanson20, A. Clough21, Alec Habig21, Y. Fukuda22, T. Sato22, Yoshitaka Itow23, T. Koike23, C. K. Jung24, T. Kato24, Katsuhiro Kobayashi24, Magdalena Malek24, C. McGrew24, A. Sarrat24, R. Terri24, C. Yanagisawa24, N. Tamura25, Makoto Sakuda26, M. Sugihara26, Y. Kuno27, Minoru Yoshida27, S. B. Kim28, B. S. Yang28, J. Yoo28, T. Ishizuka29, H. Okazawa29, Y. Choi30, H. Seo30, Y. Gando31, Takehisa Hasegawa31, Kunio Inoue31, H. Ishii32, Kyoshi Nishijima32, Hirokazu Ishino33, Y. Watanabe33, Masatoshi Koshiba1, D. Kielczewska5, D. Kielczewska34, J. Zalipska34, H. G. Berns35, R. Gran21, R. Gran35, K. K. Shiraishi35, A. L. Stachyra35, E. Thrane35, K. Washburn35, R. J. Wilkes35 
TL;DR: In this article, the results from several studies used to search for astrophysical sources of high-energy neutrinos using the Super-Kamiokande I (1996 April-2001 July) neutrino-induced upward-going muon data were presented.
Abstract: We present the results from several studies used to search for astrophysical sources of high-energy neutrinos using the Super-Kamiokande I (1996 April-2001 July) neutrino-induced upward-going muon data. The data set consists of 2359 events with minimum energy 1.6 GeV, of which 1892 are through-going and 467 stop within the detector. The results of several independent analyses are presented, including searches for point sources using directional and temporal information and a search for signatures of cosmic-ray interactions with the interstellar medium in the upward-going muons. No statistically significant evidence for point sources or any diffuse flux from the plane of the Galaxy was found, so specific limits on fluxes from likely point sources are calculated. The 90% confidence level (CL) upper limits on upward-going muon flux from astronomical sources that are located in the southern hemisphere and always under the horizon for Super-Kamiokande are ~ × 10-15 cm-2 s-1.

31 citations


Journal ArticleDOI
M. E. C. Swanson1, K. Abe2, J. Hosaka2, T. Iida2  +146 moreInstitutions (37)
TL;DR: In this article, the upward-going muon flux induced by neutrinos from active galactic nuclei is expected to exceed the flux due to atmospheric neutrinuclear sources, and a search for this astrophysical neutrino flux is performed by looking for upwardgoing muons in the highest energy data sample from the Super-Kamiokande detector using 1679.6 live days of data.
Abstract: Many astrophysical models predict a diffuse flux of high-energy neutrinos from active galactic nuclei and other extragalactic sources. At muon energies above 1 TeV, the upward-going muon flux induced by neutrinos from active galactic nuclei is expected to exceed the flux due to atmospheric neutrinos. We have performed a search for this astrophysical neutrino flux by looking for upward-going muons in the highest energy data sample from the Super-Kamiokande detector using 1679.6 live days of data. We found one extremely high energy upward-going muon event, compared with an expected atmospheric neutrino background of 0.46 ± 0.23 events. Using this result, we set an upper limit on the diffuse flux of upward-going muons due to neutrinos from astrophysical sources in the muon energy range 3.16-100 TeV.

01 Jan 2006
TL;DR: The multipixel photon counter (MPPC) as discussed by the authors is a newly developed photodetector with an excellent photon counting capability, which has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature.
Abstract: The multipixel photon counter (MPPC) is a newly developed photodetector with an excellent photon counting capability. It also has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature. The basic performance of samples has been measured. A gain of ~106 is achieved with a noise rate less than 500 kHz with 1 p.e. threshold, and cross-talk probability of less than 40% at room temperature. The photon detection efficiency for green light is twice or more that of the photomultiplier tubes. It is found that the basic performance of the MPPC is satisfactory for use in real experiments.

Posted Content
TL;DR: The multi-pixel photon counter (MPPC) as mentioned in this paper is a newly developed photodetector with an excellent photon counting capability, which has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature.
Abstract: The multi-pixel photon counter (MPPC) is a newly developed photodetector with an excellent photon counting capability. It also has many attractive features such as small size, high gain, low operation voltage and power consumption, and capability of operating in magnetic fields and in room temperature. The basic performance of samples has been measured. A gain of ~10^6 is achieved with a noise rate less than 1 MHz with 1 p.e. threshold, and cross-talk probability of less than 30% at room temperature. The photon detection efficiency for green light is twice or more that of the photomultiplier tubes. It is found that the basic performance of the MPPC is satisfactory for use in real experiments.