P. Agnes, L. Agostino, I. Albuquerque, T. Alexander, A. Alton, D. Asner, H. Back, B. Baldin, K. Biery, V. Bocci, G. Bonfini, W. Bonivento, M. Bossa, B. Bottino, A. Brigatti, J. Brodsky, F. Budano, S. Bussino, M. Cadeddu, M. Cadoni, F. Calaprice, N. Canci, A. Candela, M. Caravati, M. Cariello, M. Carlini, S. Catalanotti, P. Cavalcante, A. Chepurnov, C. Cicalò, A. Cocco, G. Covone, D. D’Angelo, M. D’Incecco, S. Davini, S. Cecco, M. Deo, M. Vincenzi, A. Derbin, A. Devoto, F. D. Eusanio, G. D. Pietro, C. Dionisi, E. Edkins, A. Empl, A. Fan, G. Fiorillo, K. Fomenko, D. Franco, F. Gabriele, C. Galbiati, S. Giagu, C. Giganti, G. Giovanetti, A. Goretti, F. Granato, M. Gromov, M. Guan, Y. Guardincerri, B. Hackett, K. Herner, D. Hughes, P. Humble, E. Hungerford, A. Ianni, A. Ianni, I. James, T. Johnson, C. Jollet, K. Keeter, C. Kendziora, G. Koh, D. Korablev, G. Korga, A. Kubankin, X. Li, M. Lissia, B. Loer, P. Lombardi, G. Longo, Y. Ma, A. Machado, I. Machulin, A. Mandarano, S. Mari, J. Maricic, L. Marini, C. Mart
{"title":"lng暗面实验现状与展望","authors":"P. Agnes, L. Agostino, I. Albuquerque, T. Alexander, A. Alton, D. Asner, H. Back, B. Baldin, K. Biery, V. Bocci, G. Bonfini, W. Bonivento, M. Bossa, B. Bottino, A. Brigatti, J. Brodsky, F. Budano, S. Bussino, M. Cadeddu, M. Cadoni, F. Calaprice, N. Canci, A. Candela, M. Caravati, M. Cariello, M. Carlini, S. Catalanotti, P. Cavalcante, A. Chepurnov, C. Cicalò, A. Cocco, G. Covone, D. D’Angelo, M. D’Incecco, S. Davini, S. Cecco, M. Deo, M. Vincenzi, A. Derbin, A. Devoto, F. D. Eusanio, G. D. Pietro, C. Dionisi, E. Edkins, A. Empl, A. Fan, G. Fiorillo, K. Fomenko, D. Franco, F. Gabriele, C. Galbiati, S. Giagu, C. Giganti, G. Giovanetti, A. Goretti, F. Granato, M. Gromov, M. Guan, Y. Guardincerri, B. Hackett, K. Herner, D. Hughes, P. Humble, E. Hungerford, A. Ianni, A. Ianni, I. James, T. Johnson, C. Jollet, K. Keeter, C. Kendziora, G. Koh, D. Korablev, G. Korga, A. Kubankin, X. Li, M. Lissia, B. Loer, P. Lombardi, G. Longo, Y. Ma, A. Machado, I. Machulin, A. Mandarano, S. Mari, J. Maricic, L. Marini, C. Mart","doi":"10.1393/NCC/I2017-17164-8","DOIUrl":null,"url":null,"abstract":"The DarkSide experiment aims to perform a background-free direct search for dark matter with a dual-phase argon TPC. The current phase of the experiment, DarkSide-50, is acquiring data at Laboratori Nazionali del Gran Sasso and produced the most sensitive limit on the WIMP-nucleon cross section ever obtained with a liquid argon target (2.0 × 10−44 cm2 for a WIMP mass of 100 GeV/c2 ). The future phase of the experiment will be a 20 t fiducial mass detector, designed to reach a sensitivity of ∼ 1 × 10−47 cm2 (at 1 TeV/c2 WIMP mass) with a backgroundfree exposure of 100 ty. This work contains a discussion of the current status of the DarkSide-50 WIMP search and of the results which are more relevant for the construction of the future detector.","PeriodicalId":81495,"journal":{"name":"Il Nuovo cimento della Societa italiana di fisica. 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Status and perspective of the DarkSide experiment at LNGS
The DarkSide experiment aims to perform a background-free direct search for dark matter with a dual-phase argon TPC. The current phase of the experiment, DarkSide-50, is acquiring data at Laboratori Nazionali del Gran Sasso and produced the most sensitive limit on the WIMP-nucleon cross section ever obtained with a liquid argon target (2.0 × 10−44 cm2 for a WIMP mass of 100 GeV/c2 ). The future phase of the experiment will be a 20 t fiducial mass detector, designed to reach a sensitivity of ∼ 1 × 10−47 cm2 (at 1 TeV/c2 WIMP mass) with a backgroundfree exposure of 100 ty. This work contains a discussion of the current status of the DarkSide-50 WIMP search and of the results which are more relevant for the construction of the future detector.
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