{"paper":{"title":"A Method to Determine the Electric Field of Liquid Argon Time Projection Chambers Using a UV Laser System and its Application in MicroBooNE","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"A. Ashkenazi, A. Bhanderi, A. Bhat, A. Blake, A. Diaz, A. Ereditato, A. Hourlier, A. Lister, A. Marchionni, A. Mastbaum, A. Mogan, A.M. Szelc, A. Papadopoulou, A. Paudel, A.P. Furmanski, A. Rafique, A. Schukraft, A. Smith, B. Baller, B. Eberly, B. Kirby, B. Lundberg, B.R. Littlejohn, B. Russell, B.T. Fleming, B. Viren, C. Barnes, C.D. Moore, C. Hill, C. James, C. Mariani, C. Rudolf von Rohr, C. Zhang, D.A. Martinez Caicedo, D.A. Wickremasinghe, D. Caratelli, D. Cianci, D. Devitt, D. Franco, D. Garcia-Gamez, D. Goeldi, D. Lorca, D. Naples, D. Porzio, D.W. Schmitz, E.C. Huang, E. Church, E. Gramellini, E.L. Snider, E.O. Cohen, E. Piasetzky, F. Bay, F. Cavanna, G.A. Horton-Smith, G. Barr, G. Cerati, G. Karagiorgi, G. Pulliam, G.P. Zeller, G. Scanavini, G. Yarbrough, H.E. Rogers, H. Greenlee, H. Wei, I. Caro Terrazas, I. Kreslo, I. Lepetic, J. Anthony, J. Asaadi, J.H. Jo, J.I. Crespo-Anadon, J. Jan de Vries, J.J. Evans, J. Joshi, J.L. Raaf, J. Marshall, J. Martin-Albo, J.M. Conrad, J. Mills, J. Moon, J. Mousseau, J. Nowak, J. Sinclair, J. Spitz, J. St. John, J. Zennamo, K. Duffy, K. Mason, K. Miller, K. Mistry, K. Sutton, K. Terao, K. Woodruff, L. Camilleri, L. Cooper-Troendle, L. Domine, L. Escudero Sanchez, L.E. Yates, L. Gu, L. Jiang, L. Ren, L. Rochester, M. Alrashed, M.A. Uchida, M. Bass, M. Bishai, M. Convery, M. Del Tutto, M.H. Shaevitz, MicroBooNE collaboration: C. Adams, M. Kirby, M. Luethi, M. Mooney, M. Murphy, M. Ross-Lonergan, M. Soderberg, M. Stancari, M. Toups, M. Weber, M. Wospakrik, N. Foppiani, N. McConkey, N. Tagg, O. Goodwin, O. Hen, O. Palamara, P. Green, P. Guzowski, P. Hamilton, P. Nienaber, P. Spentzouris, R.A. Johnson, R. An, R. Carr, R. Castillo Fernandez, R. Grosso, R. Guenette, R.G. Van de Water, R. Itay, R.K. Neely, R. Murrells, R.S. Fitzpatrick, R. Sharankova, R.T. Thornton, S. Balasubramanian, S. Berkman, S. Dytman, S.F. Pate, S. Gardiner, S. Gollapinni, S. Lockwitz, S. Marcocci, S. Prince, S.R. Soleti, S. Soldner-Rembold, S. Sword-Fehlberg, S. Tufanli, S. Wolbers, T. Bolton, T. Kobilarcik, T. Mettler, T. Mohayai, T. Strauss, T. Usher, T. Wongjirad, T. Yang, V. Basque, V. Genty, V. Meddage, V. Pandey, V. Paolone, V. Papavassiliou, V. Radeka, W.C. Louis, W. Gu, W. Ketchum, W. Seligman, W. Tang, W. Van De Pontseele, W. Wu, X. Ji, X. Luo, X. Qian, Y. Chen, Y.J. Jwa, Y. Li, Y.-T. Tsai, Z. Pavlovic, Z. Williams","submitted_at":"2019-10-03T12:40:04Z","abstract_excerpt":"Liquid argon time projection chambers (LArTPCs) are now a standard detector technology for making accelerator neutrino measurements, due to their high material density, precise tracking, and calorimetric capabilities. An electric field (E-field) is required in such detectors to drift ionized electrons to the anode to be collected. The E-field of a TPC is often approximated to be uniform between the anode and the cathode planes. However, significant distortions can appear from effects such as mechanical deformations, electrode failures, or the accumulation of space charge generated by cosmic ra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.01430","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1910.01430/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}