12 research outputs found
Fiabilidad de los test de diagnóstico de disfunción sacroilíaca y de las pruebas exploratorias de la pelvis
- Author
- Arab
- Buckup
- C. Lozano-Quijada
- Chaitow
- Cleland
- Cohen
- Dreyfuss
- E.J. Poveda-Pagán
- Fernandez-de-las-Penas
- Forst
- Greenman
- J.J. Miralles-Bueno
- J.V. Toledo-Marhuenda
- Jurado
- Kapandji
- Khruakhorn
- Kissling
- Lozano-Quijada
- M. Peral-Berná
- Manchikanti
- Meijne
- Petty
- Poveda-Pagán
- Ricard
- Riddle
- Robinson
- Salvans
- Timm
- Tixa
- Tong
- Toussaint
- Van der Wurff
- Vincent-Smith
- Wilke
- Publication venue
- 'Elsevier BV'
- Publication date
- Field of study
Factores que contribuyen a la infección relacionada con la asistencia sanitaria: cómo evitarlos
- Author
- Anderson
- Aranaz
- Aranaz
- Aranaz-Andres
- Baker
- Bonnal
- Brennan
- Burke
- Corrales
- Davis
- De Vries
- Haley
- Harbarth
- J. Requena-Puche
- J.J. Miralles-Bueno
- J.M. Aranaz-Andrés
- Kanerva
- Klevens
- Leape
- M.J. Corrales-Fernández
- M.T. Gea-Velázquez de Castro
- McKibben
- Michel
- Mielke
- Pittet
- Pittet
- Pratt
- Pronovost
- R. Limón-Ramírez
- Requena
- Rosenthal
- Rosenthal
- Rosselló-Urgell
- Schioler
- Scott
- Thomas
- Thomas
- Valls
- Vincent
- Warren
- Wilson
- Woloshynowych
- Zegers
- Publication venue
- 'Elsevier BV'
- Publication date
- Field of study
Identificación de eventos adversos en pacientes hospitalizados por gripe
- Author
- A.I. Balbuena-Segura
- Abad
- Aibar
- Aranaz
- Aranaz
- Aranaz
- Aranaz
- Aranaz-Andrés
- Aranaz-Andrés
- Aranaz-Andrés
- Aranaz-Andrés
- Aranaz-Andrés
- B. Obón-Azuara
- Braz Pavao
- Brennan
- Brennan
- C. Aibar-Remón
- Camacho
- F. Jiménez-Pericás
- Gea-Velázquez de Castro
- Guggenmoos-Holzmann
- J. Moliner-Lahoz
- J.J. Miralles-Bueno
- J.M. Aranaz-Andrés
- M.C. Meyer-García
- M.T. Gea-Velázquez de Castro
- Mattsson
- Michel
- Morgan
- N. López-Fresneña
- Naessens
- Pujol
- Requena
- Sharek
- Silver
- Thomas
- Vaqué
- Weingart
- Zarb
- Publication venue
- 'Elsevier BV'
- Publication date
- Field of study
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
- Di Giulio L
- Di Noto L
- Dias M
- Diaz E. Arrieta
- Ding P
- Diociaiuti E
- Distefano C
- Diurba R
- Diwan M
- Djurcic Z
- Doering D
- Dolan S
- Dolek F
- Dolinski M.J
- Domenici D
- Domine L
- Donati S
- Donon Y
- Doran S
- Douglas D
- Doyle T.A
- Dragone A
- Drielsma F
- Duarte L
- Duchesneau D
- Duffy K
- Dugas K
- Dunne P
- Dutta B
- Duyang H
- Dvornikov O
- Dwyer D.A
- Dyshkant A.S
- Dytman S
- Díaz F
- Díaz J.S
- Eads M
- Earle A
- Edayath S
- Edmunds D
- Eisch J
- Englezos P
- Ereditato A
- Erjavec T
- Es-Sghir H. Amar
- Escobar C.O
- Evans J.J
- Ewart E
- Ezeribe A.C
- Fahey K
- Fajardo L.S. Gomez
- Fajt L
- Falcone A
- Fani M
- Farnese C
- Farzan Y
- Fedoseev D
- Felix J
- Feng Y
- Fernandez-Martinez E
- Ferraro F
- Ferreira G. Ruiz
- Ferry G
- Fields L
- Filip P
- Filkins A
- Filthaut F
- Fine R
- Fiorillo G
- Fiorini M
- Fogarty S
- Foreman W
- Forero D.V
- Forero J.F. Castaño
- Fowler J
- Franc J
- Francis K
- 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
- Green P
- Greenberg S
- Greer J
- Griffith W.C
- Groetschla F.T
- Grzelak K
- Gu W
- Guarino V
- Guarise M
- Guenette R
- Guerard E
- Guerzoni M
- Guffanti D
- Guglielmi A
- Guo B
- Guo Y
- Gupta A
- Gupta V
- Gurung G
- Gutierrez D
- Guzowski P
- Guzzo M.M
- Gwon S
- Haaf K
- Habig A
- Hadavand H
- Haenni R
- Hagaman L
- Hahn A
- Haiston J
- Hakenmueller J
- Hamernik T
- Hamilton P
- Hancock J
- Happacher F
- Harris D.A
- Hartnell J
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- Harton J
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- Kalitkina A
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- Laurenti G
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- Lopez J
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- Losecco J.M
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- Publication venue
- HAL CCSD
- Publication date
- 08/02/2024
- Field of study
International 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
International 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
- 01/01/2024
- Field of study
International 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
International 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
DUNE Phase II: Scientific Opportunities, Detector Concepts, Technological Solutions
- 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
- Akbar F
- Allison K
- Alonso Monsalve S
- Alonso M.J. Rodriguez
- Alrashed M
- Alton A
- Alvarez R
- Alves T
- Amar H
- Amedo P
- Anderson J
- Andreopoulos C
- Andreotti M
- Andrews M.P
- Andrianala F
- Andringa S
- Anfimov N
- Ankowski A
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- Ashkenazi A
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- Auguste D
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- Zucchelli S
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- Zwaska R
- Publication venue
- HAL CCSD
- Publication date
- 04/09/2024
- Field of study
International audienceThe international collaboration designing and constructing the Deep Underground Neutrino Experiment (DUNE) at the Long-Baseline Neutrino Facility (LBNF) has developed a two-phase strategy toward the implementation of this leading-edge, large-scale science project. The 2023 report of the US Particle Physics Project Prioritization Panel (P5) reaffirmed this vision and strongly endorsed DUNE Phase I and Phase II, as did the European Strategy for Particle Physics. While the construction of the DUNE Phase I is well underway, this White Paper focuses on DUNE Phase II planning. DUNE Phase-II consists of a third and fourth far detector (FD) module, an upgraded near detector complex, and an enhanced 2.1 MW beam. The fourth FD module is conceived as a "Module of Opportunity", aimed at expanding the physics opportunities, in addition to supporting the core DUNE science program, with more advanced technologies. This document highlights the increased science opportunities offered by the DUNE Phase II near and far detectors, including long-baseline neutrino oscillation physics, neutrino astrophysics, and physics beyond the standard model. It describes the DUNE Phase II near and far detector technologies and detector design concepts that are currently under consideration. A summary of key R&D goals and prototyping phases needed to realize the Phase II detector technical designs is also provided. DUNE's Phase II detectors, along with the increased beam power, will complete the full scope of DUNE, enabling a multi-decadal program of groundbreaking science with neutrinos
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The DUNE Far Detector Vertical Drift Technology. Technical Design Report
- Author
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- Ratoff P.
- Ray R.
- Razafinime H.
- Rea E.M.
- Real J.S.
- Rebel B.
- Rechenmacher R.
- Reggiani-Guzzo M.
- Reichenbacher J.
- Reitzner S.D.
- Rejeb Sfar H.
- Renner E.
- Renshaw A.
- Rescia S.
- Resnati F.
- Restrepo Diego
- Reynolds C.
- Ribas M.
- Riboldi S.
- Riccio C.
- Riccobene G.
- Ricol J.S.
- Rigan M.
- Rincón E.V.
- Ritchie-Yates A.
- Ritter S.
- Rivera D.
- Rivera R.
- Robert A.
- Rocabado Rocha J.L.
- Rochester L.
- Roda M.
- Rodrigues P.
- Rodriguez Alonso M.J.
- Rodriguez Rondon J.
- Rosauro-Alcaraz S.
- Rosier P.
- Ross D.
- Ross-Lonergan M.
- Rossella M.
- Rossi M.
- Roy N.
- Roy P.
- Rubbia C.
- Ruggeri A.
- Ruiz Ferreira G.
- Russell B.
- Ruterbories D.
- Rybnikov A.
- Saakyan R.
- Sacerdoti S.
- Sahoo S.K.
- Sahu N.
- Sala P.
- Samios N.
- Samoylov O.
- Sanchez M.C.
- Sanchez-Lucas P.
- Sandberg V.
- Sanders D.A.
- Sanfilippo S.
- Sankey D.
- Santoro D.
- Saoulidou N.
- Sapienza P.
- Sarasty C.
- Sarcevic I.
- Sarra I.
- Savage G.
- Savinov V.
- Scanavini G.
- Scaramelli A.
- Scarff A.
- Schefke T.
- Schellman H.
- Schifano S.
- Schlabach P.
- Schmitz D.
- Schneider A.W.
- Scholberg K.
- Schukraft A.
- Schuld B.
- Segade A.
- Segreto E.
- Selyunin A.
- Senise C.R.
- Sensenig J.
- Shaevitz M.H.
- Shanahan P.
- Sharma P.
- Shaw K.
- Shaw T.
- Shchablo K.
- Shen J.
- Shepherd-Themistocleous C.
- Sheshukov A.
- Shi W.
- Shin S.
- Shivakoti S.
- Shoemaker I.
- Shooltz D.
- Shrock R.
- Siddi B.
- Siden M.
- Silber J.
- Simard L.
- Sinclair J.
- Sinev G.
- Singh Chauhan S.
- Singh J.
- Singh Jaydip
- Singh L.
- Singh P.
- Singh V.
- Sipos R.
- Sironneau C.
- Sirri G.
- Siyeon K.
- Skarpaas K.
- Smedley J.
- Smith E.
- Smith J.
- Smith P.
- Smolik J.
- Smy M.
- Snape M.
- Snider E.L.
- Snopok P.
- Snowden-Ifft D.
- Soares Nunes M.
- Sobel H.
- Soderberg M.
- Sokolov S.
- Solano Salinas C.J.
- Soleti S.R.
- Solomey N.
- Solovov V.
- Sondheim W.E.
- Sorel M.
- Sotnikov A.
- Soto-Oton J.
- Sousa A.
- Soustruznik K.
- Spinella F.
- Spitz J.
- Spooner N.J.C.
- Spurgeon K.
- Stalder D.
- Stancari M.
- Stanco L.
- Steenis J.
- Stein R.
- Steiner H.M.
- Steklain Lisbôa A.F.
- Stepanova A.
- Stewart J.
- Stillwell B.
- Stock J.
- Stocker F.
- Stokes T.
- Strait M.
- Strauss T.
- Strigari L.
- Stuart A.
- Suarez J.G.
- Subash J.
- Surdo A.
- Suter L.
- Sutera C.M.
- Sutton K.
- Suvorov Y.
- Svoboda R.
- Swain S.K.
- Szczerbinska B.
- Szelc A.M.
- Sztuc A.
- Sánchez Bravo A.
- Söldner-Rembold S.
- Taffara A.
- Talukdar N.
- Tamara J.
- Tanaka H.A.
- Tang S.
- Taniuchi N.
- Tapia Casanova A.M.
- Tapia Oregui B.
- Tapper A.
- Tariq S.
- Tarpara E.
- Tatar E.
- Tayloe R.
- Tedeschi D.
- Teklu A.M.
- Tena Vidal J.
- Tennessen P.
- Tenti M.
- Terao K.
- Terranova F.
- Testera G.
- Thakore T.
- The DUNE collaboration
- Thea A.
- Thomas S.
- Thompson A.
- Thorn C.
- Timm S.C.
- Tiras E.
- Tishchenko V.
- Todorović N.
- Tomassetti L.
- Tonazzo A.
- Torbunov D.
- Torti M.
- Tortola M.
- Tortorici F.
- Tosi N.
- Totani D.
- Toups M.
- Touramanis C.
- Tran D.
- Travaglini R.
- Trevor J.
- Triller E.
- Trilov S.
- Truchon J.
- Truncali D.
- Trzaska W.H.
- Tsai Y.
- Tsai Y.-T.
- Tsamalaidze Z.
- Tsang K.V.
- Tsverava N.
- Tu S.Z.
- Tufanli S.
- Tunnell C.
- Turner J.
- Tuzi M.
- Tyler J.
- Tyley E.
- Tzanov M.
- Uchida M.A.
- Ureña González J.
- Urheim J.
- Usher T.
- Utaegbulam H.
- Uzunyan S.
- V. G.Caceres
- Vagins M.R.
- Vahle P.
- Valder S.
- Valdiviesso G.A.
- Valencia E.
- Valentim R.
- Vallari Z.
- Vallazza E.
- Valle J.W.F.
- Van Berg R.
- Van de Water R.G.
- Van Nuland-Troost M.
- Vannozzi A.
- Varanini F.
- Vargas Oliva D.
- Vasina S.
- Vaughan N.
- Vaziri K.
- Vega J.
- Ventura S.
- Verdugo A.
- Vergani S.
- Verzocchi M.
- Vetter K.
- Vicenzi M.
- Vieira de Souza H.
- Vignoli C.
- Vilela C.
- Villa E.
- Viola S.
- Viren B.
- Vizcaya-Hernandez A.
- Vuong Q.
- Vázquez-Ramos A.
- Waldron A.V.
- Wallbank M.
- Walsh J.
- Walton T.
- Wang H.
- Wang J.
- Wang L.
- Wang M.H.L.S.
- Wang X.
- Wang Y.
- Warburton K.
- Warner D.
- Warsame L.
- Wascko M.O.
- Waters D.
- Watson A.
- Wawrowska K.
- Weber A.
- Weber C.M.
- Weber M.
- Wei H.
- Weinstein A.
- Wenzel H.
- Westerdale S.
- Wetstein M.
- Whalen K.
- Whilhelmi J.
- White A.
- Whitehead L.H.
- Whittington D.
- Wilking M.J.
- Wilkinson A.
- Wilkinson C.
- Wilson F.
- Wilson R.J.
- Winter P.
- 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.
- Wurm M.
- Wyenberg J.
- Xiao Y.
- Xiotidis I.
- Yaeggy B.
- Yahlali N.
- Yandel E.
- Yang K.
- Yang T.
- Yankelevich A.
- Yershov N.
- Yonehara K.
- Young T.
- Yu B.
- Yu H.
- Yu J.
- Yu Y.
- Yuan W.
- Zaki R.
- Zalesak J.
- Zambelli L.
- Zamorano B.
- Zani A.
- Zapata O.
- Zazueta L.
- Zeller G.P.
- Zennamo J.
- Zeug K.
- Zhang C.
- Zhang S.
- Zhao M.
- Zhivun E.
- Zimmerman E.D.
- Zucchelli S.
- Zuklin J.
- Zutshi V.
- Zwaska R.
- Publication venue
- Journal of Instrumentation
- Publication date
- 21/08/2024
- Field of study
DUNE is an international experiment dedicated to addressing some of the questions at the forefront of particle physics and astrophysics, including the mystifying preponderance of matter over antimatter in the early universe. The dual-site experiment will employ an intense neutrino beam focused on a near and a far detector as it aims to determine the neutrino mass hierarchy and to make high-precision measurements of the PMNS matrix parameters, including the CP-violating phase. It will also stand ready to observe 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 implements liquid argon time-projection chamber (LArTPC) technology, and combines the many tens-of-kiloton fiducial mass necessary for rare event searches with the sub-centimeter spatial resolution required to image those events with high precision. The addition of a photon detection system enhances physics capabilities for all DUNE physics drivers and opens prospects for further physics explorations. Given its size, the far detector will be implemented as a set of modules, with LArTPC designs that differ from one another as newer technologies arise. In the vertical drift LArTPC design, a horizontal cathode bisects the detector, creating two stacked drift volumes in which ionization charges drift towards anodes at either the top or bottom. The anodes are composed of perforated PCB layers with conductive strips, enabling reconstruction in 3D. Light-trap-style photon detection modules are placed both on the cryostat's side walls and on the central cathode where they are optically powered. This Technical Design Report describes in detail the technical implementations of each subsystem of this LArTPC that, together with the other far detector modules and the near detector, will enable DUNE to achieve its physics goals
DUNE Phase II: Scientific Opportunities, Detector Concepts, Technological Solutions
- 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
- Akbar F
- Allison K
- Alonso Monsalve S
- Alonso M.J. Rodriguez
- Alrashed M
- Alton A
- Alvarez R
- Alves T
- Amar H
- Amedo P
- Anderson J
- Andreopoulos C
- Andreotti M
- Andrews M.P
- Andrianala F
- Andringa S
- Anfimov N
- Ankowski A
- Antic D
- Antoniassi M
- Antonova M
- Antoshkin A
- Aranda-Fernandez A
- Arellano L
- Arroyave M.A
- Asaadi J
- Ashkenazi A
- Asner D.M
- Asquith L
- Atkin E
- Auguste D
- Aurisano A
- Aushev V
- Autiero D
- Azam M.B
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- Back A
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- Back J.J
- Bagaturia I
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- Baldonedo J
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- Barker G.J
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- Bazo Alba J.L.L
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- Benitez A. Campos
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- Bermeo L.V. Gomez
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- Bersani A
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- Bromberg C
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- Caceres V.G
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- Caminata A
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- Carneiro M.F
- Carniti P
- Caro Terrazas I
- Carranza H
- Carrara N
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- Casarejos E
- Casazza D
- Castaño F.A
- Castillo A
- Castromonte C
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- Chappell A
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- Chatterjee A
- Chauhan S. Singh
- Chen H
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- de Mello Neto J.R.T
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- de Rego I. López
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- de Souza H. Vieira
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- Dyshkant A.S
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- Eisch J
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- Ereditato A
- Erjavec T
- Escobar C.O
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- Fedoseev D
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- Fernández-Posada D
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- Publication venue
- HAL CCSD
- Publication date
- 04/09/2024
- Field of study
International audienceThe international collaboration designing and constructing the Deep Underground Neutrino Experiment (DUNE) at the Long-Baseline Neutrino Facility (LBNF) has developed a two-phase strategy toward the implementation of this leading-edge, large-scale science project. The 2023 report of the US Particle Physics Project Prioritization Panel (P5) reaffirmed this vision and strongly endorsed DUNE Phase I and Phase II, as did the European Strategy for Particle Physics. While the construction of the DUNE Phase I is well underway, this White Paper focuses on DUNE Phase II planning. DUNE Phase-II consists of a third and fourth far detector (FD) module, an upgraded near detector complex, and an enhanced 2.1 MW beam. The fourth FD module is conceived as a "Module of Opportunity", aimed at expanding the physics opportunities, in addition to supporting the core DUNE science program, with more advanced technologies. This document highlights the increased science opportunities offered by the DUNE Phase II near and far detectors, including long-baseline neutrino oscillation physics, neutrino astrophysics, and physics beyond the standard model. It describes the DUNE Phase II near and far detector technologies and detector design concepts that are currently under consideration. A summary of key R&D goals and prototyping phases needed to realize the Phase II detector technical designs is also provided. DUNE's Phase II detectors, along with the increased beam power, will complete the full scope of DUNE, enabling a multi-decadal program of groundbreaking science with neutrinos