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Joseph D. Parker

Bio: Joseph D. Parker is an academic researcher from Kyoto University. The author has contributed to research in topics: Neutron imaging & Neutron. The author has an hindex of 19, co-authored 79 publications receiving 1256 citations.


Papers
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Journal ArticleDOI
S. P. Ahlen1, Niayesh Afshordi2, Niayesh Afshordi3, James Battat4, J. Billard5, Nassim Bozorgnia6, S. Burgos7, T. Caldwell8, T. Caldwell4, J. M. Carmona9, S. Cebrián9, P. Colas, T. Dafni9, E. J. Daw10, D. Dujmic4, A. Dushkin11, William Fedus4, Efrain J. Ferrer, D. Finkbeiner12, Peter H. Fisher4, J. Forbes7, T. Fusayasu13, J. Galán9, T. Gamble10, C. Ghag14, Ioannis Giomataris, Michael Gold15, Haley Louise Gomez9, M. E. Gomez16, Paolo Gondolo17, Anne M. Green18, C. Grignon5, O. Guillaudin5, C. Hagemann15, Kaori Hattori19, Shawn Wesley Henderson4, N. Higashi19, C. Ida19, F.J. Iguaz9, Andrew Inglis1, I. G. Irastorza9, Satoru Iwaki19, A. C. Kaboth4, Shigeto Kabuki19, J. Kadyk20, Nitya Kallivayalil4, H. Kubo19, Shunsuke Kurosawa19, V. A. Kudryavtsev10, T. Lamy5, Richard C. Lanza4, T. B. Lawson10, A. Lee4, E. R. Lee15, T. Lin12, D. Loomba15, Jeremy Lopez4, G. Luzón9, T. Manobu, J. Martoff21, F. Mayet5, B. Mccluskey10, E. H. Miller15, Kentaro Miuchi19, Jocelyn Monroe4, B. Morgan22, D. Muna23, A. St. J. Murphy14, Tatsuhiro Naka24, K. Nakamura19, M. Nakamura24, T. Nakano24, G.G. Nicklin10, H. Nishimura19, K. Niwa24, Sean Paling10, Joseph D. Parker19, A. Petkov7, M. Pipe10, K. Pushkin7, Matthew R. Robinson10, Arturo Rodriguez Rodriguez9, Jose Rodríguez-Quintero16, T. Sahin4, Robyn E. Sanderson4, N. Sanghi15, D. Santos5, O. Sato24, Tatsuya Sawano19, G. Sciolla4, Hiroyuki Sekiya25, Tracy R. Slatyer12, D. P. Snowden-Ifft7, N. J. C. Spooner10, A. Sugiyama26, A. Takada, M. Takahashi19, A. Takeda25, Toru Tanimori19, Kojiro Taniue19, A. Tomás9, H. Tomita1, K. Tsuchiya19, J. Turk15, E. Tziaferi10, K. Ueno19, S. E. Vahsen20, R. Vanderspek4, J D Vergados27, J.A. Villar9, H. Wellenstein11, I. Wolfe4, R. K. Yamamoto4, H. Yegoryan4 
TL;DR: The case for a dark matter detector with directional sensitivity was presented at the 2009 CYGNUS workshop on directional dark matter detection, and contributions from theorists and experimental groups in the field as mentioned in this paper.
Abstract: We present the case for a dark matter detector with directional sensitivity. This document was developed at the 2009 CYGNUS workshop on directional dark matter detection, and contains contributions from theorists and experimental groups in the field. We describe the need for a dark matter detector with directional sensitivity; each directional dark matter experiment presents their project's status; and we close with a feasibility study for scaling up to a one ton directional detector, which would cost around $150M.

224 citations

Journal ArticleDOI
James Battat1, I. G. Irastorza2, A. Aleksandrov3, T. Asada4, E. Baracchini3, J. Billard5, J. Billard6, G. Bosson5, O. Bourrion5, Jerome Bouvier5, A. Buonaura3, K. Burdge7, K. Burdge8, S. Cebrián2, P. Colas9, L. Consiglio3, T. Dafni2, Nicola D'Ambrosio3, Cosmin Deaconu8, Cosmin Deaconu10, G. De Lellis3, T. Descombes5, A. Di Crescenzo3, N. Di Marco3, Gabriela Druitt11, Richard Eggleston11, E. Ferrer-Ribas9, T. Fusayasu12, Javier Galan2, G. Galati3, J. A. Garcia2, J. G. Garza2, V. Gentile, M. Garcia-Sciveres13, Y. Giomataris9, Natalia Guerrero8, Natalia Guerrero11, O. Guillaudin5, A. M. Guler14, J. L. Harton15, T. Hashimoto16, M. T. Hedges17, F.J. Iguaz2, T. Ikeda16, I. Jaegle18, J. A. Kadyk13, Taishi Katsuragawa4, S. Komura19, H. Kubo19, Ken'ichi Kuge20, J. Lamblin5, Adele Lauria3, E. R. Lee21, P.M. Lewis17, Michael Leyton11, Michael Leyton8, D. Loomba21, Jeremy Lopez22, Jeremy Lopez8, G. Luzón2, F. Mayet5, H. Mirallas2, Kentaro Miuchi16, Tetsuya Mizumoto19, Y. Mizumura19, P. Monacelli3, Jocelyn Monroe11, Jocelyn Monroe23, Maria Cristina Montesi3, Tatsuhiro Naka4, Koji Nakamura19, H. Nishimura19, Atsuhiko Ochi16, T. Papevangelou9, Joseph D. Parker, N. S. Phan21, F. Pupilli3, J.P. Richer5, Q. Riffard24, Giovanni Rosa3, D. Santos5, Tatsuya Sawano19, Hiroyuki Sekiya25, Ihn Sik Seong17, Daniel P. Snowden-Ifft26, N. J. C. Spooner27, A. Sugiyama12, Ryosuke Taishaku16, A. Takada19, A. Takeda25, M. Tanaka23, Toru Tanimori19, T. N. Thorpe17, Valeri Tioukov3, H. Tomita8, A. Umemoto4, S. E. Vahsen17, Y. Yamaguchi16, M. Yoshimoto4, E. Zayas8 
TL;DR: In this paper, the authors review the various detector readout technologies used by directional detectors, summarize the challenges, advantages and drawbacks of each approach, and discuss future prospects for these technologies.

100 citations

Journal ArticleDOI
TL;DR: In this article, a direction-sensitive dark matter search experiment at Kamioka underground laboratory with the NEWAGE-0.3a detector was performed, which achieved a new record of 5400 pb for 150 GeV / c 2 WIMPs.

98 citations

Journal ArticleDOI
TL;DR: In this article, the first measurement of the λ(1405) photoproduction cross section was made, and the line shapes of λ (1405)-generated lines were measured in two photon energy ranges: near the production threshold (1.5 to 2.0 GeV) and far from it (2.0
Abstract: Differential cross sections for {gamma}p{yields}K{sup +}{lambda}(1405) and {gamma}p{yields}K{sup +}{sigma}{sup 0}(1385) reactions have been measured in the photon energy range from 1.5 to 2.4 GeV and the angular range of 0.8

74 citations

Journal ArticleDOI
TL;DR: In this article, a search for the K − p p bound state (the lightest kaonic nucleus) was performed using the γ d → K + π − X reaction at E γ = 1.5 − 2.4 GeV at LEPS/SPring-8.

74 citations


Cited by
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Journal Article
TL;DR: In this article, a self-scanned 1024 element photodiode array and a minicomputer are used to measure the phase (wavefront) in the interference pattern of an interferometer to lambda/100.
Abstract: A self-scanned 1024 element photodiode array and minicomputer are used to measure the phase (wavefront) in the interference pattern of an interferometer to lambda/100. The photodiode array samples intensities over a 32 x 32 matrix in the interference pattern as the length of the reference arm is varied piezoelectrically. Using these data the minicomputer synchronously detects the phase at each of the 1024 points by a Fourier series method and displays the wavefront in contour and perspective plot on a storage oscilloscope in less than 1 min (Bruning et al. Paper WE16, OSA Annual Meeting, Oct. 1972). The array of intensities is sampled and averaged many times in a random fashion so that the effects of air turbulence, vibrations, and thermal drifts are minimized. Very significant is the fact that wavefront errors in the interferometer are easily determined and may be automatically subtracted from current or subsequent wavefrots. Various programs supporting the measurement system include software for determining the aperture boundary, sum and difference of wavefronts, removal or insertion of tilt and focus errors, and routines for spatial manipulation of wavefronts. FFT programs transform wavefront data into point spread function and modulus and phase of the optical transfer function of lenses. Display programs plot these functions in contour and perspective. The system has been designed to optimize the collection of data to give higher than usual accuracy in measuring the individual elements and final performance of assembled diffraction limited optical systems, and furthermore, the short loop time of a few minutes makes the system an attractive alternative to constraints imposed by test glasses in the optical shop.

1,300 citations

01 Jan 2003
TL;DR: In this paper, the thermal and epithermal self-shielding factors in different materials (Al, Au, Cd, Co, Cu, Eu, Gd, In, Ir, Mo, Ni, Pt, Pb, Rh, Sc, Sm and Ta) and different geometries (foils, wires, spheres and) have been calculated using the MCNP code.
Abstract: The presence of a sample in the neutron field of a nuclear reactor creates a perturbation of the local neutron fluxes. In general, the interpretation of the sample activation due to thermal and epithermal neutrons requires the knowledge of two corrective parameters: the thermal neutron self-shielding factor, Gth, and the resonance neutron self-shielding factor, Gres. Thermal neutron self-shielding factors in different materials (Al, Au, Cd, Co, Cu, Eu, Gd, In, Ir, Mo, Ni, Pt, Pb, Rh, Sc, Sm and Ta) and different geometries (foils, wires, spheres and) have been calculated by using the MCNP code.

473 citations

Journal ArticleDOI
TL;DR: In this paper, the status of direct dark matter searches is summarized, focusing on the detector technologies used to directly detect a dark matter particle producing recoil energies in the keV energy scale.
Abstract: In recent decades, several detector technologies have been developed with the quest to directly detect dark matter interactions and to test one of the most important unsolved questions in modern physics. The sensitivity of these experiments has improved with a tremendous speed due to a constant development of the detectors and analysis methods, proving uniquely suited devices to solve the dark matter puzzle, as all other discovery strategies can only indirectly infer its existence. Despite the overwhelming evidence for dark matter from cosmological indications at small and large scales, clear evidence for a particle explaining these observations remains absent. This review summarises the status of direct dark matter searches, focusing on the detector technologies used to directly detect a dark matter particle producing recoil energies in the keV energy scale. The phenomenological signal expectations, main background sources, statistical treatment of data and calibration strategies are discussed.

395 citations