28 research outputs found
Volume I. Introduction to DUNE
- Author
- Abi B.
- Acciarri R.
- Acero M.A.
- Adamov G.
- Adams D.
- Adinolfi M.
- Ahmad Z.
- Ahmed J.
- Alba J. Bazo
- Alion T.
- Almeida R.M. De
- Alonso M. Rodriguez
- Alt C.
- Anderson J.
- Andreopoulos C.
- Andrews M.
- Andrianala F.
- Andringa S.
- Ankowski A.
- Antonova M.
- Antusch S.
- Aranda-Fernandez A.
- Ariga A.
- Arnold L.O.
- Arroyave M.A.
- Asaadi J.
- Astiz I.L. De Icaza
- Aurisano A.
- Aushev V.
- Autiero D.
- Azfar F.
- Back H.
- Back J.J.
- Backhouse C.
- Baesso P.
- Bagby L.
- Bajou R.
- Balasubramanian S.
- Baldi P.
- Bambah B.
- Barao F.
- Barenboim G.
- Barker G.
- Barkhouse Wayne A.
- Barnes C.
- Barr G.
- Barros N.
- Barrow J.L.
- Bashyal A.
- Basque V.
- Bay F.
- Beacom J.F.
- Bechetoille E.
- Behera B.
- Bellantoni L.
- Bellettini G.
- Bellini V.
- Beltramello O.
- Belver D.
- Benekos N.
- Berg R. Van
- Berger J.
- Berkman S.
- Bermeo L. Gomez
- Bernardini P.
- Berner R.M.
- Berns H.
- Bertolucci S.
- Betancourt M.
- Bezawada Y.
- Bhattacharjee M.
- Bhuyan B.
- Biagi S.
- Bian J.
- Biassoni M.
- Biery K.
- Bilki B.
- Bishai M.
- Bitadze A.
- Blake A.
- Blaszczyk F.
- Blazey G.
- Blucher E.
- Boissevain J.
- Bolognesi S.
- Bolton T.
- Bonesini M.
- Bongrand M.
- Bonini F.
- Bonis I. De
- Booth A.
- Booth C.
- Bordoni S.
- Borkum A.
- Boschi T.
- Bostan N.
- Bour P.
- Boyd S.
- Boyden D.
- Bracinik J.
- Braga D.
- Brailsford D.
- Brandt A.
- Bremer J.
- Brew C.
- Brianne E.
- Brice S.J.
- Brizzolari C.
- Bromberg C.
- Brooijmans G.
- Brooke J.
- Bross A.
- Brunetti G.
- Buchanan N.
- Budd H.
- Bueno L. Molina
- Caicedo D.A. Martinez
- Caiulo D.
- Calafiura P.
- Calcutt J.
- Calin M.
- Calvez S.
- Calvo E.
- Camilleri L.
- Caminata A.
- Campanelli M.
- Campo A. Olivares Del
- Caratelli D.
- Carini G.
- Carlus B.
- Carniti P.
- Carranza H.
- Castillo A.
- Castromonte C.
- Cattadori C.
- Cavalier F.
- Cavanna F.
- Centro S.
- Cerati G.
- Cervelli A.
- Chalifour M.
- Chang C.
- Chardonnet E.
- Chatterjee A.
- Chattopadhyay S.
- Chaves J.
- Chen H.
- Chen M.
- Chen Y.
- Cherdack D.
- Chi C.
- Childress S.
- Chiriacescu A.
- Cho K.
- Choubey S.
- Christensen A.
- Christian D.
- Christodoulou G.
- Church E.
- Clarke P.
- Coan T.E.
- Cocco A.G.
- Coelho J.
- Conley E.
- Conrad J.
- Convery M.
- Corwin L.
- Cotte P.
- Cremaldi L.
- Cremonesi L.
- Crespo-Anad J.I.
- Cristaldo E.
- Cross R.
- Cuesta C.
- Cui Y.
- Cussans D.
- Dabrowski M.
- David Q.
- Davies G.S.
- Davini S.
- Dawson J.
- de Oliveira M. Leigui
- de Souza H. Vieira
- de Water R.G. Van
- De K.
- Debbins P.
- Decowski M.
- Deisting A.
- Delbart A.
- Delepine D.
- Delgado M.
- Delgado M. Ramirez
- Dell\u27Acqua A.
- DeMuth D.M.
- Dennis S.
- Densham C.
- Deptuch G.
- Dharmapalan R.
- Dias M.
- Diaz F.
- Diaz J.
- Ding P.
- Distefano C.
- Diurba R.
- Diwan M.
- Djurcic Z.
- Dokania N.
- Dolinski M.
- Domine L.
- Domizio S. Di
- Douglas D.
- Drielsma F.
- Duchesneau D.
- Duffy K.
- Dunne P.
- Durkin T.
- Duyang H.
- Dvornikov O.
- Dwyer D.
- Dyshkant A.
- Eads M.
- Edmunds D.
- Eisch J.
- Emery S.
- Ereditato A.
- Escobar C.
- Evans J.J.
- Ewart E.
- Ezeribe A.C.
- Fahey K.
- Fajardo L.S. Gomez
- Falcone A.
- Farnese C.
- Farzan Y.
- Felix J.
- Fernandez-Martinez E.
- Ferraro F.
- Fields L.
- Filkins A.
- Filthaut F.
- Fitzpatrick R.S.
- Flanagan W.
- Fleming B.
- Flight R.
- Forero D. Vanegas
- Fowler J.
- Fox W.
- Franc J.
- Francis K.
- Franco D.
- Freeman J.
- Freestone J.
- Fried J.
- Friedland A.
- Fuess S.
- Furic I.
- Furmanski A.P.
- Gago A.
- Gallagher H.
- Gallego-Ros A.
- Gallice N.
- Galymov V.
- Gamberini E.
- Gamble T.
- Gandhi R.
- Gandrajula R.
- Gao S.
- Garceris M.Á.
- Garcia-Gamez D.
- Gardiner S.
- Gastler D.
- Ge G.
- Gelli B.
- Gendotti A.
- Gent S.
- Ghorbani-Moghaddam Z.
- Gibin D.
- Gil-Botella I.
- Girerd C.
- Giri A.
- Giulio L. Di
- Gnani D.
- Gogota O.
- Gold M.
- Gollapinni S.
- Gollwitzer K.
- Gomes R.A.
- Gonnella F.
- Gonzalez-Cuevas J.
- Goodman M.C.
- Goodwin O.
- Goswami S.
- Gotti C.
- Goudzovski E.
- Gouvea A. De
- Grace C.
- Graham M.
- Gramellini E.
- Gran R.
- Granados E.
- Grant A.
- Grant C.
- Gratieri D.
- Green P.
- Green S.
- Greenler L.
- Greenwood M.
- Greer J.
- Griffith C.
- Groh M.
- Grudzinski J.
- Grzelak K.
- Gu W.
- Guarino V.
- Guenette R.
- Guglielmi A.
- Guo B.
- Guthikonda K.
- Gutierrez R.
- Guzowski P.
- Guzzo M.M.
- Gwon S.
- Habig A.
- Hackenburg A.
- Hadavand H.
- Haenni R.
- Hahn A.
- Haigh J.
- Haiston J.
- Hamernik T.
- Hamilton P.
- Han J.
- Harder K.
- Harris D.A.
- Hartnell J.
- Hasegawa T.
- Hatcher R.
- Hazen E.
- Heavey A.
- Heeger K.M.
- Hennessy K.
- Henry S.
- Herner K.
- Hertel L.
- Hesam A.S.
- Hewes J.
- Hill T.
- Hillier S.J.
- Himmel A.
- Hoff J.
- Hohl C.
- Holanda P.C. De
- Holin A.
- Hoppe E.
- Horton-Smith G.A.
- Hostert M.
- Hourlier A.
- Howard B.
- Howell R.
- Huang J.
- Huang J.
- Hugon J.
- Iles G.
- Iliescu A.M.
- Illingworth R.
- Ioannisian A.
- Itay R.
- Izmaylov A.
- James E.
- Jargowsky B.
- Jediny F.
- Jesús-Valls C.
- Ji X.
- Jiang L.
- Jiménez S.
- Jipa A.
- Joglekar A.
- Johnson C.
- Johnson R.
- Jones B.
- Jones S.
- Jong P. De
- Jung C.
- Junk T.
- Jwa Y.
- Kabirnezhad M.
- Kaboth A.
- Kadenko I.
- Kamiya F.
- Karagiorgi G.
- Karcher A.
- Karolak M.
- Karyotakis Y.
- Kasai S.
- Kasetti S.P.
- Kashur L.
- Kazaryan N.
- Kearns E.
- Keener P.
- Kelly K.J.
- Kemp E.
- Ketchum W.
- Kettell S.
- Khabibullin M.
- Khotjantsev A.
- Khvedelidze A.
- Kim D.
- King B.
- Kirby B.
- Kirby M.
- Klein J.
- Koehler K.
- Koerner L.W.
- Kohn S.
- Koller P.P.
- Kordosky M.
- Kosc T.
- Kose U.
- Kostelecky V.
- Kothekar K.
- Krennrich F.
- Kreslo I.
- Kudenko Y.
- Kudryavtsev V.
- Kulagin S.
- Kumar J.
- Kumar R.
- Kuruppu C.
- Kus V.
- Kutter T.
- Lambert A.
- Lande K.
- Lane C.E.
- Lang K.
- Langford T.
- Lasorak P.
- Last D.
- Lastoria C.
- Laundrie A.
- Lawrence A.
- Lazanu I.
- LaZur R.
- Le T.
- Learned J.
- LeBrun P.
- Lehnert R.
- Leitner M.
- Leyton M.
- Li L.
- Li S.
- Li S.
- Li T.
- Li Y.
- Liao H.
- Lin C.
- Lin S.
- Lister A.
- Littlejohn B.R.
- Liu J.
- Lockwitz S.
- Loew T.
- Lokajicek M.
- Lomidze I.
- Long K.
- Loo K.
- Lorca D.
- Lord T.
- LoSecco J.
- Louis W.C.
- Luk K.
- Luo X.
- Lurgio P. De
- Lurkin N.
- Lux T.
- Luzio V.P.
- MacFarland D.
- Machado A.
- Machado P.
- Macias C.
- Macier J.
- Maddalena A.
- Madigan P.
- Magill S.
- Mahn K.
- Maio A.
- Maloney J.A.
- Mandrioli G.
- Maneira J.C.
- Manenti L.
- Manly S.
- Mann A.
- Manolopoulos K.
- Marchionni A.
- Marciano W.
- Marfatia D.
- Mariani C.
- Maricic J.
- Marinho F.
- Marino A.D.
- Marshak M.
- Marshall C.
- Marshall J.
- Marteau J.
- Martin-Albo J.
- Martinez N.
- Martynenko S.
- Mason K.
- Mastbaum A.
- Masud M.
- Matsuno S.
- Matthews J.
- Mauger C.
- Mauri N.
- Mavrokoridis K.
- Mazza R.
- Mazzacane A.
- Mazzucato E.
- McCluskey E.
- McConkey N.
- McFarland K.S.
- McGrew C.
- McNab A.
- Mefodiev A.
- Mehta P.
- Melas P.
- Mellinato M.
- Mena O.
- Menary S.
- Mendez H.
- Menegolli A.
- Menendez P. Fernandez
- Meng G.
- Messier M.
- Metcalf W.
- Mewes M.
- Meyer H.
- Miao T.
- Michna G.
- Miedema T.
- Migenda J.
- Milincic R.
- Miller W.
- Mills J.
- Milne C.
- Mineev O.
- Miotto G. Lehmann
- Miranda O.G.
- Miryala S.
- Mishra C.
- Mishra S.
- Mislivec A.
- Mladenov D.
- Mocioiu I.
- Moffat K.
- Moggi N.
- Mohanta R.
- Mohayai T.A.
- Mokhov N.
- Molina J.A.
- Monarca J. Barranco
- Monsalve S. Alonso
- Montanari A.
- Montanari C.
- Montanari D.
- Moon J.
- Mooney M.
- Moor A.
- Moreno D.
- Morgan B.
- Morquecho M. Hernandez
- Morris C.
- Mossey C.
- Motta H. Da
- Motuk E.
- Moura C.A.
- Mousseau J.
- Mu W.
- Mualem L.
- Mueller J.
- Muether M.
- Mufson S.
- Muheim F.
- Muir A.
- Mulhearn M.
- Muramatsu H.
- Murphy S.
- Musser J.
- Nachtman J.
- Nagu S.
- Nalbandyan M.
- Nandakumar R.
- Naples D.
- Narita S.
- Navas-Nicolas D.
- Nayak N.
- Nebot-Guinot M.
- Necib L.
- Negishi K.
- Nelson J.K.
- Nesbit J.
- Nessi M.
- Neto J.R. De Mello
- Neves F. Bento
- Newbold D.
- Newcomer M.
- Newhart D.
- Nichol R.
- Niner E.
- Nishimura K.
- Norman A.
- Northrop R.
- Noto L. Di
- Novella P.
- Nowak J.A.
- Nunes M. Soares
- Oberling M.
- Olivier A.
- Onel Y.
- Onishchuk Y.
- Oregui B. Tapia
- Ott J.
- Pagani L.
- Pakvasa S.
- Palamara O.
- Palestini S.
- Paley J.M.
- Pallavicini M.
- Palomares C.
- Pantic E.
- Paolone V.
- Papadimitriou V.
- Papaleo R.
- Papanestis A.
- Paramesvaran S.
- Parke S.
- Parsa Z.
- Parvu M.
- Pascoli S.
- Pasqualini L.
- Pasternak J.
- Pater J.
- Patrick C.
- Patrizii L.
- Patterson R.B.
- Patton S.
- Patzak T.
- Paudel A.
- Paulos B.
- Paulucci L.
- Pavlovic Z.
- Pawloski G.
- Payne D.
- Pec V.
- Peeters S.J.
- Penichot Y.
- Pennacchio E.
- Penzo A.
- Peres L. Da Silva
- Peres O.L.
- Perry J.
- Pershey D.
- Pessina G.
- Petrillo G.
- Petta C.
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- Pichardo A. Higuera
- Pickering L.
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- Pillow J.
- Plata M. Manrique
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- Poling R.
- Pons X.
- Poonthottathil N.
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- Potekhin M.
- Potenza R.
- Potukuchi B.V.
- Pozimski J.
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- Prakash S.
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- Prince S.
- Prior G.
- Pugnere D.
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- Raaf J.
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- Radics B.
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- Ratoff P.
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- Roeth A.
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- Rondon J. Rodriguez
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- Rossella M.
- Rout J.
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- Russell J.
- Ruterbories D.
- Saakyan R.
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- Safford T.
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- Sala P.
- Salinas C.J. Solano
- Samios N.
- Sanchez L. Escudero
- Sanchez M.
- Sanders D.A.
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- Santana S.
- Santos-Maldonado M.
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- Sapienza P.
- Sarasty C.
- Sarcevic I.
- Savage G.
- Savinov V.
- Scaramelli A.
- Scarff A.
- Scarpelli A.
- Schaffer T.
- Schellman H.
- Schlabach P.
- Schmitz D.
- Scholberg K.
- Schukraft A.
- Segreto E.
- Sensenig J.
- Seong I.
- Sergi A.
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- Shaevitz M.
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- Sharma H.R.
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- Talaga R.
- Tanaka H.
- Tapper A.
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- Vermeulen M.A.
- Verzocchi M.
- Vignoli C.
- Vilela C.
- Villanueva A. Cervera
- Viren B.
- Vrba T.
- Vries J. De
- Wachala T.
- Waldron A.V.
- Wallbank M.
- Wang H.
- Wang J.
- Wang Y.
- Wang Y.
- Warburton K.
- Warner D.
- Wascko M.
- Waters D.
- Watson A.
- Weatherly P.
- Weber A.
- Weber M.
- Wei H.
- Weinstein A.
- Wenman D.
- Wetstein M.
- While M.R.
- White A.
- Whitehead L.H.
- Whittington D.
- Wilking M.J.
- Wilkinson C.
- Williams Z.
- Wilson F.
- Wilson R.J.
- Wolcott J.
- Wongjirad T.
- Wood K.
- Wood L.
- Worcester E.
- Worcester M.
- Wret C.
- Wu W.
- Wu W.
- Xiao Y.
- Yang G.
- Yang T.
- Yershov N.
- Yonehara K.
- Young Tim
- Yu B.
- Yu J.
- Zalesak J.
- Zambelli L.
- Zamorano B.
- Zani A.
- Zazueta L.
- Zeller G.
- Zennamo J.
- Zetina L.M. Montano
- Zeug K.
- Zhang C.
- Zhao M.
- Zhivun E.
- Zhu G.
- Zimmerman E.D.
- Zito M.
- Zucchelli S.
- Zuklin J.
- Zutshi V.
- Zwaska R.
- Publication venue
- UND Scholarly Commons
- Publication date
- 01/08/2020
- Field of study
Get PDFThe preponderance of matter over antimatter in the early universe, the dynamics of the supernovae that produced the heavy elements necessary for life, and whether protons eventually decay—these mysteries at the forefront of particle physics and astrophysics are key to understanding the early evolution of our universe, its current state, and its eventual fate. The Deep Underground Neutrino Experiment (DUNE) is an international world-class experiment dedicated to addressing these questions as it searches for leptonic charge-parity symmetry violation, stands ready to capture supernova neutrino bursts, and seeks to observe nucleon decay as a signature of a grand unified theory underlying the standard model. The DUNE far detector technical design report (TDR) describes the DUNE physics program and the technical designs of the single- and dual-phase DUNE liquid argon TPC far detector modules. This TDR is intended to justify the technical choices for the far detector that flow down from the high-level physics goals through requirements at all levels of the Project. Volume I contains an executive summary that introduces the DUNE science program, the far detector and the strategy for its modular designs, and the organization and management of the Project. The remainder of Volume I provides more detail on the science program that drives the choice of detector technologies and on the technologies themselves. It also introduces the designs for the DUNE near detector and the DUNE computing model, for which DUNE is planning design reports. Volume II of this TDR describes DUNE\u27s physics program in detail. Volume III describes the technical coordination required for the far detector design, construction, installation, and integration, and its organizational structure. Volume IV describes the single-phase far detector technology. A planned Volume V will describe the dual-phase technology
Deep Underground Neutrino Experiment (DUNE), far detector technical design report, volume III: DUNE far detector technical coordination
- Author
- A. Ankowski
- A. Aranda-Fernandez
- A. Ariga
- A. Aurisano
- A. Bashyal
- A. Bitadze
- A. Blake
- A. Booth
- A. Borkum
- A. Brandt
- A. Bross
- A. Caminata
- A. Castillo
- A. Cervelli
- A. Cervera Villanueva
- A. Cervera Villanueva
- A. Chatterjee
- A. Chiriacescu
- A. Christensen
- A. De Gouvea
- A. De Roeck
- A. Deisting
- A. Delbart
- A. Dell'Acqua
- A. Dyshkant
- A. Ereditato
- A. Falcone
- A. Filkins
- A. Friedland
- A. Gago
- A. Gallego-Ros
- A. Gendotti
- A. Giri
- A. Grant
- A. Guglielmi
- A. Habig
- A. Hackenburg
- A. Hahn
- A. Heavey
- A. Higuera Pichardo
- A. Himmel
- A. Holin
- A. Hourlier
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- W. Ketchum
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- W. Metcalf
- W. Miller
- W. Mu
- W. Wu
- W. Wu
- W.C. Louis
- W.E. Sondheim
- W.H. Trzaska
- X. Ji
- X. Luo
- X. Pons
- X. Qian
- Y. Bezawada
- Y. Chen
- Y. Cui
- Y. Farzan
- Y. Jwa
- Y. Karyotakis
- Y. Kudenko
- Y. Li
- Y. Onel
- Y. Onishchuk
- Y. Penichot
- Y. Ramachers
- Y. Rigaut
- Y. Wang
- Y. Wang
- Y. Xiao
- Y.T. Tsai
- Z. Ahmad
- Z. Djurcic
- Z. Ghorbani-Moghaddam
- Z. Parsa
- Z. Pavlovic
- Z. Tsamalaidze
- Z. Vallari
- Z. Williams
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
Get PDFThe preponderance of matter over antimatter in the early universe, the dynamics of the supernovae that produced the heavy elements necessary for life, and whether protons eventually decay—these mysteries at the forefront of particle physics and astrophysics are key to understanding the early evolution of our universe, its current state, and its eventual fate. The Deep Underground Neutrino Experiment (DUNE) is an international world-class experiment dedicated to addressing these questions as it searches for leptonic charge-parity symmetry violation, stands ready to capture supernova neutrino bursts, and seeks to observe nucleon decay as a signature of a grand unified theory underlying the standard model. The DUNE far detector technical design report (TDR) describes the DUNE physics program and the technical designs of the single- and dual-phase DUNE liquid argon TPC far detector modules. Volume III of this TDR describes how the activities required to design, construct, fabricate, install, and commission the DUNE far detector modules are organized and managed. This volume details the organizational structures that will carry out and/or oversee the planned far detector activities safely, successfully, on time, and on budget. It presents overviews of the facilities, supporting infrastructure, and detectors for context, and it outlines the project-related functions and methodologies used by the DUNE technical coordination organization, focusing on the areas of integration engineering, technical reviews, quality assurance and control, and safety oversight. Because of its more advanced stage of development, functional examples presented in this volume focus primarily on the single-phase (SP) detector module
Highly-parallelized simulation of a pixelated LArTPC on a GPU
- Author
- Abed Abud A.
- Abi B.
- Acciarri R.
- Acero M.A.
- Adames M.R.
- Adamov G.
- Adamowski M.
- Adams D.
- Adinolfi M.
- Adriano C.
- Aduszkiewicz A.
- Aguilar J.
- Ahmad Z.
- Ahmed J.
- Aimard B.
- Akbar F.
- Allison K.
- Alonso Monsalve S.
- Alrashed M.
- Alt C.
- Alton A.
- Alvarez R.
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- Tennessen P.
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- Thorn C.
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- Todorović N.
- Tomassetti L.
- Tonazzo A.
- Torbunov D.
- Torti M.
- Tortola M.
- Tortorici F.
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- Totani D.
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- Touramanis C.
- Travaglini R.
- Trevor J.
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- Tsai Y.
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- Tsang K.V.
- Tsverava N.
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- Tufanli S.
- Tull C.
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- Tyley E.
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- Utaegbulam H.
- Uzunyan S.
- V. G.C.
- Vagins M.R.
- Vahle P.
- Valder S.
- Valdiviesso G.A.
- Valencia E.
- Valentim R.
- Vallari Z.
- Vallazza E.
- Valle J.W.F.
- Vallecorsa S.
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- Van de Water R.G.
- Vanegas Forero D.
- Vannerom D.
- Varanini F.
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- Varner G.
- Vasina S.
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- Vega J.
- Ventura S.
- Verdugo A.
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- Vermeulen M.A.
- Verzocchi M.
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- Vignoli C.
- Vilela C.
- Viren B.
- Vizcaya-Hernandez A.
- Vrba T.
- Vuong Q.
- Wachala T.
- Waldron A.V.
- Wallbank M.
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- Wang H.
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- Warburton K.
- Warner D.
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- Waters D.
- Watson A.
- Wawrowska K.
- Weatherly P.
- Weber A.
- Weber M.
- Wei H.
- Weinstein A.
- Wenman D.
- Wetstein M.
- Whilhelmi J.
- White A.
- White A.
- Whitehead L.H.
- Whittington D.
- Wilking M.J.
- Wilkinson A.
- Wilkinson C.
- Williams Z.
- Wilson F.
- Wilson R.J.
- Wisniewski W.
- Wolcott J.
- Wolfs J.
- Wongjirad T.
- Wood A.
- Wood K.
- Worcester E.
- Worcester M.
- Wospakrik M.
- Wresilo K.
- Wret C.
- Wu S.
- Wu W.
- Wu W.
- Wurm M.
- Wyenberg J.
- Xiao Y.
- Xiotidis I.
- Yaeggy B.
- Yahlali N.
- Yandel E.
- Yang G.
- Yang K.
- Yang T.
- Yankelevich A.
- Yershov N.
- Yonehara K.
- Yoon Y.S.
- Young T.
- Yu B.
- Yu H.
- Yu H.
- Yu J.
- Yu Y.
- Yuan W.
- Zaki R.
- Zalesak J.
- Zambelli L.
- Zamorano B.
- Zani A.
- Zazueta L.
- Zeller G.P.
- Zennamo J.
- Zeug K.
- Zhang C.
- Zhang S.
- Zhang Y.
- Zhao M.
- Zhivun E.
- Zimmerman E.D.
- Zucchelli S.
- Zuklin J.
- Zutshi V.
- Zwaska R.
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2023
- Field of study
Get PDFThe rapid development of general-purpose computing on graphics processing units (GPGPU) is allowing the implementation of highly-parallelized Monte Carlo simulation chains for particle physics experiments. This technique is particularly suitable for the simulation of a pixelated charge readout for time projection chambers, given the large number of channels that this technology employs. Here we present the first implementation of a full microphysical simulator of a liquid argon time projection chamber (LArTPC) equipped with light readout and pixelated charge readout, developed for the DUNE Near Detector. The software is implemented with an end-to-end set of GPU-optimized algorithms. The algorithms have been written in Python and translated into CUDA kernels using Numba, a just-in-time compiler for a subset of Python and NumPy instructions. The GPU implementation achieves a speed up of four orders of magnitude compared with the equivalent CPU version. The simulation of the current induced on 10^3 pixels takes around 1 ms on the GPU, compared with approximately 10 s on the CPU. The results of the simulation are compared against data from a pixel-readout LArTPC prototype
Transverse Emittance Reduction in Muon Beams by Ionization Cooling
- Author
- Adams D.
- Adey D.
- Asfandiyarov R.
- Bayes R.
- Bayliss V.
- Bertoni R.
- Blackmore V.J.
- Blondel A.
- Boehm J.
- Bogomilov M.
- Bonesini M.
- Booth C.N.
- Bowring D.
- Boyd S.
- Bradshaw T.W.
- Bross A.D.
- Brown C.
- Charnley G.
- Chatzitheodoridis G.T.
- Chignoli F.
- Chung M.
- Cobb J.H.
- Colling D.
- Collomb N.
- Coney L.R.
- Cooke P.
- Courthold M.
- Cremaldi L.M.
- de Bari A.
- DeMello A.
- Dick A.J.
- Dobbs A.
- Dornan P.
- Drielsma F.
- Dumbell K.
- Ellis M.
- Fedorov M.
- Filthaut F.
- Franchini P.
- Freemire B.
- Gallagher A.
- Gamet R.
- Gardener R.B.S.
- Gourlay S.
- Govans J.
- Grant A.
- Greis J.R.
- Griffiths S.
- Hanlet P.
- Hanson G.G.
- Hartnett T.
- Hayler T.
- Heidt C.
- Hills M.
- Hodgson P.
- Hunt C.
- Ishimoto S.
- Jokovic D.
- Jovancevic N.
- Jurj P.B.
- Kaplan D.M.
- Karadzhov Y.
- Kuno Y.
- Kurup A.
- Kyberd P.
- Lagrange J.B.
- Lambert A.
- Langlands J.
- Li D.
- Li Z.H.
- Liu A.
- Long K.
- Lord T.
- Luo T.
- Macwaters C.
- Maletic D.
- Martlew B.
- Martyniak J.
- Mazza R.
- Middleton S.
- Mohayai T.A.
- Moss A.
- Muir A.
- Mullacrane I.
- Nebrensky J.J.
- Neuffer D.
- Nichols A.
- Nikolov J.
- Nugent J.C.
- Oates A.
- Orestano D.
- Overton E.
- Owens P.
- Palmer M.
- Pasternak J.
- Pec V.
- Pidcott C.
- Popovic M.
- Preece R.
- Prestemon S.
- Rajaram D.
- Ramberger S.
- Ricciardi S.
- Rogers C.
- Ronald K.
- Rubinov P.
- Sakamoto H.
- Sanders D.A.
- Sato A.
- Savic M.
- Smith P.J.
- Snopok P.
- Soler F.J.P.
- Song Y.P.
- Stanley T.
- Stokes G.
- Sung C.K.
- Tang J.Y.
- Tarrant J.
- Taylor I.
- Tortora L.
- Torun Y.
- Tsenov R.
- Tucker M.
- Uchida M.A.
- Vankova-Kirilova G.
- Virostek S.
- Vretenar M.
- Warburton P.
- Watson S.
- White C.
- Whyte C.G.
- Wilbur S.
- Wilson A.
- Witte H.
- Young A.R.
- Publication venue
- Publication date
- 09/10/2023
- Field of study
No full textAccelerated muon beams have been considered for next-generation studies of high-energy lepton-antilepton collisions and neutrino oscillations. However, high-brightness muon beams have not yet been produced. The main challenge for muon acceleration and storage stems from the large phase-space volume occupied by the beam, derived from the muon production mechanism through the decay of pions from proton collisions. Ionization cooling is the technique proposed to decrease the muon beam phase-space volume. Here we demonstrate a clear signal of ionization cooling through the observation of transverse emittance reduction in beams that traverse lithium hydride or liquid hydrogen absorbers in the Muon Ionization Cooling Experiment (MICE). The measurement is well reproduced by the simulation of the experiment and the theoretical model. The results shown here represent a substantial advance towards the realization of muon-based facilities that could operate at the energy and intensity frontiers
Doping Liquid Argon with Xenon in ProtoDUNE Single-Phase: Effects on Scintillation Light
- Author
- Abed Abud A
- Abi B
- Acciarri R
- Acero M.A
- Adames M.R
- Adamov G
- Adamowski M
- Adams D
- Adinolfi M
- Adriano C
- Aduszkiewicz A
- Aguilar J
- Aimard B
- Akbar F
- Allison K
- Alonso Monsalve S
- Alonso M.J. Rodriguez
- Alrashed M
- Alton A
- Alvarez R
- Amedo P
- Anderson J
- Andrade D.A
- Andreopoulos C
- Andreotti M
- Andrews M.P
- Andrianala F
- Andringa S
- Anfimov N
- Ankowski A
- Antoniassi M
- Antonova M
- Antoshkin A
- Aranda-Fernandez A
- Arellano L
- Arroyave M.A
- Asaadi J
- Ashkenazi A
- Asquith L
- Atkin E
- Auguste D
- Aurisano A
- Aushev V
- Autiero D
- Azfar F
- Back A
- Back H
- Back J.J
- Bagaturia I
- Bagby L
- Balashov N
- Balasubramanian S
- Baldi P
- Baldini W
- Baller B
- Bambah B
- Banerjee R
- Barao F
- Barenboim G
- Barham Alzás P
- Barker G.J
- Barkhouse W
- Barr G
- Barros A
- Barros N
- Barrow D
- Barrow J.L
- Basharina-Freshville A
- Bashyal A
- Basque V
- Batchelor C
- Bathe-Peters L
- Battat J.B.R
- Battisti F
- Bay F
- Bazetto M.C.Q
- Bazo Alba J.L.L
- Beacom J.F
- Bechetoille E
- Behera B
- Belchior E
- Bell G
- Bellantoni L
- Bellettini G
- Bellini V
- Beltramello O
- Benekos N
- Benitez A. Campos
- Benjamin D
- Bento Neves F
- Berger J
- Berkman S
- Bermeo L.V. Gomez
- Bernardini P
- Bersani A
- Bertolucci S
- Betancourt M
- Bevan A
- Bezawada Y
- Bezerra A.T
- Bezerra T.J
- Bhat A
- Bhatnagar V
- Bhatt J
- Bhattacharjee M
- Bhattacharya M
- Bhuller S
- Bhuyan B
- Biagi S
- Bian J
- Biery K
- Bilki B
- Bishai M
- Bitadze A
- Blake A
- Blaszczyk F.D
- Blazey G.C
- Blucher E
- Boissevain J
- Bolognesi S
- Bolton T
- Bomben L
- Bonesini M
- Bonilla-Diaz C
- Bonini F
- Booth A
- Boran F
- Bordoni S
- Borkum A
- Bostan N
- Bracinik J
- Braga D
- Brahma B
- Brailsford D
- Bramati F
- Branca A
- Brandt A
- Bravo A. Sánchez
- Bremer J
- Brew C
- Brice S.J
- Brio V
- Brizzolari C
- Bromberg C
- Brooke J
- Bross A
- Brunetti G
- Brunetti M
- Buchanan N
- Budd H
- Bueno L. Molina
- Buergi J
- Burgardt D
- Butchart S
- Caceres V.G
- Cagnoli I
- Cai T
- Calabrese R
- Calcutt J
- Calin M
- Calivers L
- Calvo E
- Caminata A
- Campanelli W
- Canci N
- Capó J
- Caracas I
- Caratelli D
- Carber D
- Carceller J.M
- Carini G
- Carlus B
- Carneiro M.F
- Carniti P
- Caro Terrazas I
- Carranza H
- Carrara N
- Carroll L
- Carroll T
- Carter A
- Casanova A.M. Tapia
- Casazza D
- Castaño F.A
- Castillo A
- Castromonte C
- Catano-Mur E
- Cattadori C
- Cavalier F
- Cavanna F
- Centro S
- Cerati G
- Cervelli A
- Chakraborty K
- Chalifour M
- Chappell A
- Charitonidis N
- Chatterjee A
- Chauhan S. Singh
- Chen H
- Chen M
- Chen W.C
- Chen Y
- Chen-Wishart Z
- Cherdack D
- Chi C
- Chirco R
- Chitirasreemadam N
- Cho K
- Choate S
- Chokheli D
- Chong P.S
- Chowdhury B
- Christian D
- Chukanov A
- Chung M
- Church E
- Cicala M.F
- Cicerchia M
- Cicero V
- Ciolini R
- Clair J
- Clarke P
- Cline G
- Coan T.E
- Cocco A.G
- Coelho J.A.B
- Cohen A
- Collot J
- Conley E
- Conrad J.M
- Convery M
- Cooke P
- Copello S
- Cova P
- Cox C
- Cremaldi L
- Cremonesi L
- Crespo-Anadón J.I
- Crisler M
- Cristaldo E
- Crnkovic J
- Crone G
- Cross R
- Cudd A
- Cuesta C
- Cui Y
- Cussans D
- da Motta H
- da Silva Peres L
- Dai J
- Dalager O
- Dallavalle R
- Dar Z.A
- Darby R
- David Q
- Davies G.S
- Davini S
- Dawson J
- de Aguiar R
- de Almeida P
- de Bonis I
- de Gouvêa A
- de Holanda P.C
- de Icaza Astiz I.L
- de Jong P
- de la Torre A
- de Lurgio P
- de Mello Neto J.R.T
- de Oliveira M.A. Leigui
- de Rego I. López
- de Roeck A
- de Romeri V
- de Souza H. Vieira
- Debbins P
- Decowski M.P
- Delbart A
- Delepine D
- Delgado M
- Delgado M.A. Ramirez
- Dell'Acqua A
- Delle Monache G
- Delmonte N
- Demario R
- Demuth D.M
- Dennis S
- Densham C
- Denton P
- Deptuch G.W
- Detje J.P
- Devine J
- Dharmapalan R
- Di Capua F
- Di Domenico A
- Di Domizio S
- Di Falco S
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- Dias M
- Diaz E. Arrieta
- Ding P
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- Distefano C
- Diurba R
- Diwan M
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- Doering D
- Dolan S
- Dolek F
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- Domenici D
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- Duyang H
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- Dwyer D.A
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- Dytman S
- Díaz F
- Díaz J.S
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- Edayath S
- Edmunds D
- Eisch J
- Englezos P
- Ereditato A
- Erjavec T
- Es-Sghir H. Amar
- Escobar C.O
- Evans J.J
- Ewart E
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- Fajardo L.S. Gomez
- Fajt L
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- Fani M
- Farnese C
- Farzan Y
- Fedoseev D
- Felix J
- Feng Y
- Fernandez-Martinez E
- Ferraro F
- Ferreira G. Ruiz
- Ferry G
- Fields L
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- Filkins A
- Filthaut F
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- Fiorillo G
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- Fogarty S
- Foreman W
- Forero D.V
- Forero J.F. Castaño
- Fowler J
- Franc J
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- Franco D
- Franklin J
- Freeman J
- Fried J
- Friedland A
- Fuess S
- Furic I.K
- Furman K
- Furmanski A.P
- Gabrielli A
- Gago A.M
- Galizzi F
- Gallagher H
- Gallas A
- Gallice N
- Galymov V
- Gamberini E
- Gamble T
- Ganacim F
- Gandhi R
- Ganguly S
- Gao F
- Gao S
- Garcia-Gamez D
- García-Peris M.Á
- Gardim F
- Gardiner S
- Gastler D
- Gauch A
- Gauvreau J
- Gauzzi P
- Ge G
- Geffroy N
- Gelli B
- Gent S
- Gerlach L
- Ghorbani-Moghaddam Z
- Giammaria P
- Giammaria T
- Gibin D
- Gil-Botella I
- Gilligan S
- Gioiosa A
- Giovannella S
- Girerd C
- Giri A.K
- Giugliano C
- Giusti V
- Gnani D
- Gogota O
- Gollapinni S
- Gollwitzer K
- Gomes R.A
- Gonnella F
- Gonzalez-Diaz D
- Gonzalez-Lopez M
- González J. Ureña
- Goodman M.C
- Goswami S
- Gotti C
- Goudeau J
- Goudzovski E
- Grace C
- Gramellini E
- Gran R
- Granados E
- Granger P
- Grant C
- Gratieri D.R
- Grauso G
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- Greenberg S
- Greer J
- Griffith W.C
- Groetschla F.T
- Grzelak K
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- Guarino V
- Guarise M
- Guenette R
- Guerard E
- Guerzoni M
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- Gutierrez D
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- Hagaman L
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- Hazen E
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- Heise J
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- Hilgenberg C
- Hillier S.J
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- Hirsch L.R
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- Holvey T
- Hoppe E
- Horton-Smith G.A
- Hostert M
- Houdy T
- Howard B
- Howell R
- Hristova I
- Hronek M.S
- Huang J
- Huang R.G
- Hulcher Z
- Ibrahim M
- Iles G
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- Illingworth R
- Ingratta G
- Ioannisian A
- Irwin B
- Isenhower L
- Ismerio Oliveira M
- Itay R
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- Jain V
- James E
- Jang W
- Jargowsky B
- Jena D
- Ji X
- Jiang C
- Jiang J
- Jiang L
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- Joaquim F.R
- Johnson W
- Jones B
- Jones R
- Joséfernández D
- Jovancevic N
- Judah M
- Jung C.K
- Junk T
- Jwa Y
- Kabirnezhad M
- Kaboth A.C
- Kadenko I
- Kakorin I
- Kalitkina A
- Kalra D
- Kamiya F
- Kandemir M
- Kaplan D.M
- Karagiorgi G
- Karaman G
- Karcher A
- Karyotakis Y
- Kasai S
- Kasetti S.P
- Kashur L
- Katsioulas I
- Kauther A
- Kazaryan N
- Ke L
- Kearns E
- Keener P.T
- Kelly K.J
- Kemp E
- Kemularia O
- Kermaidic Y
- Ketchum W
- Kettell S.H
- Khabibullin M
- Khan N
- Khotjantsev A
- Khvedelidze A
- Kim D
- Kim J
- King B
- Kirby B
- Kirby M
- Klein J
- Kleykamp J
- Klustova A
- Kobilarcik T
- Koch L
- Koehler K
- Koerner L.W
- Koh D.H
- Kolupaeva L
- Korablev D
- Kordosky M
- Kosc T
- Kose U
- Kostelecký V.A
- Kothekar K
- Kotler I
- Kovalcuk M
- Kozhukalov V
- Krah W
- Kralik R
- Kramer M
- Kreczko L
- Krennrich F
- Kreslo I
- Kroupova T
- Kubota S
- Kubu M
- Kudenko Y
- Kudryavtsev V.A
- Kuhlmann S
- Kulagin S
- Kumar J
- Kumar P
- Kumar R
- Kumaran S
- Kunze P
- Kunzmann J
- Kuravi R
- Kurita N
- Kuruppu C
- Kus V
- Kutter T
- Kvasnicka J
- Labree T
- Lackey T
- Lambert A
- Land B.J
- Lane C.E
- Lane N
- Lang K
- Langford T
- Langstaff M
- Lanni F
- Lantwin O
- Larkin J
- Lasorak P
- Last D
- Laudrain A
- Laundrie A
- Laurenti G
- Lavaut E
- Lawrence A
- Laycock P
- Lazanu I
- Lazzaroni M
- Le T
- Leardini S
- Learned J
- Lecompte T
- Lee C
- Legin V
- Lehmann Miotto G
- Lehnert R
- Leitner M
- Lepin L.M
- Li J. -Y
- Li S.W
- Li Y
- Liao H
- Lin C.S
- Lindebaum D
- Lineros R.A
- Ling J
- Lister A
- Littlejohn B.R
- Liu H
- Liu J
- Liu Y
- Lockwitz S
- Lokajicek M
- Lomidze I
- Long K
- Lopes T.V
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- Publication venue
- HAL CCSD
- Publication date
- 08/02/2024
- Field of study
No full textInternational audienceDoping of liquid argon TPCs (LArTPCs) with a small concentration of xenon is a technique for light-shifting and facilitates the detection of the liquid argon scintillation light. In this paper, we present the results of the first doping test ever performed in a kiloton-scale LArTPC. From February to May 2020, we carried out this special run in the single-phase DUNE Far Detector prototype (ProtoDUNE-SP) at CERN, featuring 770 t of total liquid argon mass with 410 t of fiducial mass. The goal of the run was to measure the light and charge response of the detector to the addition of xenon, up to a concentration of 18.8 ppm. The main purpose was to test the possibility for reduction of non-uniformities in light collection, caused by deployment of photon detectors only within the anode planes. Light collection was analysed as a function of the xenon concentration, by using the pre-existing photon detection system (PDS) of ProtoDUNE-SP and an additional smaller set-up installed specifically for this run. In this paper we first summarize our current understanding of the argon-xenon energy transfer process and the impact of the presence of nitrogen in argon with and without xenon dopant. We then describe the key elements of ProtoDUNE-SP and the injection method deployed. Two dedicated photon detectors were able to collect the light produced by xenon and the total light. The ratio of these components was measured to be about 0.65 as 18.8 ppm of xenon were injected. We performed studies of the collection efficiency as a function of the distance between tracks and light detectors, demonstrating enhanced uniformity of response for the anode-mounted PDS. We also show that xenon doping can substantially recover light losses due to contamination of the liquid argon by nitrogen
Doping Liquid Argon with Xenon in ProtoDUNE Single-Phase: Effects on Scintillation Light
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- Publication venue
- HAL CCSD
- Publication date
- 08/02/2024
- Field of study
No full textInternational audienceDoping of liquid argon TPCs (LArTPCs) with a small concentration of xenon is a technique for light-shifting and facilitates the detection of the liquid argon scintillation light. In this paper, we present the results of the first doping test ever performed in a kiloton-scale LArTPC. From February to May 2020, we carried out this special run in the single-phase DUNE Far Detector prototype (ProtoDUNE-SP) at CERN, featuring 770 t of total liquid argon mass with 410 t of fiducial mass. The goal of the run was to measure the light and charge response of the detector to the addition of xenon, up to a concentration of 18.8 ppm. The main purpose was to test the possibility for reduction of non-uniformities in light collection, caused by deployment of photon detectors only within the anode planes. Light collection was analysed as a function of the xenon concentration, by using the pre-existing photon detection system (PDS) of ProtoDUNE-SP and an additional smaller set-up installed specifically for this run. In this paper we first summarize our current understanding of the argon-xenon energy transfer process and the impact of the presence of nitrogen in argon with and without xenon dopant. We then describe the key elements of ProtoDUNE-SP and the injection method deployed. Two dedicated photon detectors were able to collect the light produced by xenon and the total light. The ratio of these components was measured to be about 0.65 as 18.8 ppm of xenon were injected. We performed studies of the collection efficiency as a function of the distance between tracks and light detectors, demonstrating enhanced uniformity of response for the anode-mounted PDS. We also show that xenon doping can substantially recover light losses due to contamination of the liquid argon by nitrogen
Doping Liquid Argon with Xenon in ProtoDUNE Single-Phase: Effects on Scintillation Light
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- Zutshi V
- Publication venue
- HAL CCSD
- Publication date
- 08/02/2024
- Field of study
No full textInternational audienceDoping of liquid argon TPCs (LArTPCs) with a small concentration of xenon is a technique for light-shifting and facilitates the detection of the liquid argon scintillation light. In this paper, we present the results of the first doping test ever performed in a kiloton-scale LArTPC. From February to May 2020, we carried out this special run in the single-phase DUNE Far Detector prototype (ProtoDUNE-SP) at CERN, featuring 770 t of total liquid argon mass with 410 t of fiducial mass. The goal of the run was to measure the light and charge response of the detector to the addition of xenon, up to a concentration of 18.8 ppm. The main purpose was to test the possibility for reduction of non-uniformities in light collection, caused by deployment of photon detectors only within the anode planes. Light collection was analysed as a function of the xenon concentration, by using the pre-existing photon detection system (PDS) of ProtoDUNE-SP and an additional smaller set-up installed specifically for this run. In this paper we first summarize our current understanding of the argon-xenon energy transfer process and the impact of the presence of nitrogen in argon with and without xenon dopant. We then describe the key elements of ProtoDUNE-SP and the injection method deployed. Two dedicated photon detectors were able to collect the light produced by xenon and the total light. The ratio of these components was measured to be about 0.65 as 18.8 ppm of xenon were injected. We performed studies of the collection efficiency as a function of the distance between tracks and light detectors, demonstrating enhanced uniformity of response for the anode-mounted PDS. We also show that xenon doping can substantially recover light losses due to contamination of the liquid argon by nitrogen
Long-baseline neutrino oscillation physics potential of the DUNE experiment: DUNE Collaboration
- Publication venue
- Publication date
- 01/01/2020
- Field of study
No full textThe sensitivity of the Deep Underground Neutrino Experiment (DUNE) to neutrino oscillation is determined, based on a full simulation, reconstruction, and event selection of the far detector and a full simulation and parameterized analysis of the near detector. Detailed uncertainties due to the flux prediction, neutrino interaction model, and detector effects are included. DUNE will resolve the neutrino mass ordering to a precision of 5σ, for all δCP values, after 2 years of running with the nominal detector design and beam configuration. It has the potential to observe charge-parity violation in the neutrino sector to a precision of 3σ (5σ) after an exposure of 5 (10) years, for 50% of all δCP values. It will also make precise measurements of other parameters governing long-baseline neutrino oscillation, and after an exposure of 15 years will achieve a similar sensitivity to sin 22 θ13 to current reactor experiments. © 2020, The Author(s)
Supernova neutrino burst detection with the deep underground neutrino experiment: DUNE Collaboration
- Publication venue
- Publication date
- 01/01/2021
- Field of study
No full textThe deep underground neutrino experiment (DUNE), a 40-kton underground liquid argon time projection chamber experiment, will be sensitive to the electron-neutrino flavor component of the burst of neutrinos expected from the next Galactic core-collapse supernova. Such an observation will bring unique insight into the astrophysics of core collapse as well as into the properties of neutrinos. The general capabilities of DUNE for neutrino detection in the relevant few- to few-tens-of-MeV neutrino energy range will be described. As an example, DUNE’s ability to constrain the νe spectral parameters of the neutrino burst will be considered. © 2021, The Author(s)
First results on ProtoDUNE-SP liquid argon time projection chamber performance from a beam test at the CERN Neutrino Platform
- Author
- Abed Abud A.
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- Zuklin J.
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- Zwaska R.
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2020
- Field of study
Get PDFInternational audienceThe ProtoDUNE-SP detector is a single-phase liquid argon time projection chamber with an active volume of 7.2× 6.1× 7.0 m3. It is installed at the CERN Neutrino Platform in a specially-constructed beam that delivers charged pions, kaons, protons, muons and electrons with momenta in the range 0.3 GeV/c to 7 GeV/c. Beam line instrumentation provides accurate momentum measurements and particle identification. The ProtoDUNE-SP detector is a prototype for the first far detector module of the Deep Underground Neutrino Experiment, and it incorporates full-size components as designed for that module. This paper describes the beam line, the time projection chamber, the photon detectors, the cosmic-ray tagger, the signal processing and particle reconstruction. It presents the first results on ProtoDUNE-SP's performance, including noise and gain measurements, dE/dx calibration for muons, protons, pions and electrons, drift electron lifetime measurements, and photon detector noise, signal sensitivity and time resolution measurements. The measured values meet or exceed the specifications for the DUNE far detector, in several cases by large margins. ProtoDUNE-SP's successful operation starting in 2018 and its production of large samples of high-quality data demonstrate the effectiveness of the single-phase far detector design
