Long-baseline neutrino oscillation physics potential of the DUNE experiment

Abi, B.; Acciarri, R.; Acero, M.; Adamov, G.; Adams, D.; Adinolfi, M.; Ahmad, Z.; Ahmed, J.; Alion, T.; Monsalve, S.; 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.; Arroyave, M.; Asaadi, J.; Aurisano, A.; Aushev, V.; Autiero, D.; Azfar, F.; Back, H.; Back, J.; Backhouse, C.; Baesso, P.; Bagby, L.; Bajou, R.; Balasubramanian, S.; Baldi, P.; Bambah, B.; Barao, F.; Barenboim, G.; Barker, G.; Barkhouse, W.; Barnes, C.; Barr, G.; Monarca, J.; Barros, N.; Barrow, J.; Bashyal, A.; Basque, V.; Bay, F.; Alba, J.; Beacom, J.; Bechetoille, E.; Behera, B.; Bellantoni, L.; Bellettini, G.; Bellini, V.; Beltramello, O.; Belver, D.; Benekos, N.; Neves, F.; Berger, J.; Berkman, S.; Bernardini, P.; Berner, R.; 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.; Siffert, B.; Blaszczyk, F.; Blazey, G.; Blucher, E.; Boissevain, J.; Bolognesi, S.; Bolton, T.; Bonesini, M.; Bongrand, M.; Bonini, F.; 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.; Brizzolari, C.; Bromberg, C.; Brooijmans, G.; Brooke, J.; Bross, A.; Brunetti, G.; Buchanan, N.; Budd, H.; Caiulo, D.; Calafiura, P.; Calcutt, J.; Calin, M.; Calvez, S.; Calvo, E.; Camilleri, L.; Caminata, A.; Campanelli, M.; Caratelli, D.; Carini, G.; Carlus, B.; Carniti, P.; Terrazas, I.; Carranza, H.; Castillo, A.; Castromonte, C.; Cattadori, C.; Cavalier, F.; Cavanna, F.; Centro, S.; Cerati, G.; Cervelli, A.; Villanueva, 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.; Cocco, A.; Coelho, J.; Conley, E.; Conrad, J.; Convery, M.; Corwin, L.; Cotte, P.; Cremaldi, L.; Cremonesi, L.; Crespo-Anadón, J.; Cristaldo, E.; Cross, R.; Cuesta, C.; Cui, Y.; Cussans, D.; Dabrowski, M.; Motta, H.; Silva Peres, L.; David, C.; David, Q.; Davies, G.; Davini, S.; Dawson, J.; De, K.; Almeida, R.; Debbins, P.; Bonis, I.; Decowski, M.; Gouvêa, A.; Holanda, P.; Icaza Astiz, I.; Deisting, A.; Jong, P.; Delbart, A.; Delepine, D.; Delgado, M.; Dell’Acqua, A.; Lurgio, P.; Mello Neto, J.; DeMuth, D.; Dennis, S.; Densham, C.; Deptuch, G.; Roeck, A.; Romeri, V.; Vries, J.; Dharmapalan, R.; Dias, M.; Diaz, F.; Díaz, J.; Domizio, S.; Giulio, L.; Ding, P.; Noto, L.; Distefano, C.; Diurba, R.; Diwan, M.; Djurcic, Z.; Dokania, N.; Dolinski, M.; Domine, L.; 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.; 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Gratieri, D.; Green, P.; Green, S.; Greenler, L.; Greenwood, M.; Greer, J.; Griffith, W.; Groh, M.; Grudzinski, J.; Grzelak, K.; Gu, W.; Guarino, V.; Guenette, R.; Guglielmi, A.; Guo, B.; Guthikonda, K.; Gutierrez, R.; Guzowski, P.; Guzzo, 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.; Hartnell, J.; Hasegawa, T.; Hatcher, R.; Hazen, E.; Heavey, A.; Heeger, K.; Heise, J.; Hennessy, K.; Henry, S.; Morquecho, M.; Herner, K.; Hertel, L.; Hesam, A.; Hewes, J.; Higuera, A.; Hill, T.; Hillier, S.; Himmel, A.; Hoff, J.; Hohl, C.; Holin, A.; Hoppe, E.; Horton-Smith, G.; Hostert, M.; Hourlier, A.; Howard, B.; Howell, R.; Huang, J.; Huang, J.; Hugon, J.; Iles, G.; Ilic, N.; Iliescu, A.; Illingworth, R.; Ioannisian, A.; Itay, R.; Izmaylov, A.; James, E.; Jargowsky, B.; Jediny, F.; Jesùs-Valls, C.; Ji, X.; Jiang, L.; Jiménez, S.; Jipa, A.; Joglekar, A.; Johnson, C.; Johnson, R.; Jones, B.; 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doi:10.1140/epjc/s10052-020-08456-z
Long-baseline neutrino oscillation physics potential of the DUNE experiment

B. Abi (University of Oxford, Oxford, OX1 3RH, UK) ; R. Acciarri (Fermi National Accelerator Laboratory, Batavia, IL, 60510, USA) ; M. Acero (Universidad del Atlántico, Atlántico, Colombia) ; G. Adamov (Georgian Technical University, Tbilisi, Georgia) ; D. Adams (Brookhaven National Laboratory, Upton, NY, 11973, USA) ; et al. - Show all 973 authors
The 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 5 $$\sigma $$ $σ$ , for all $$\delta _{\mathrm{CP}}$$ $δ_{CP}$ 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 3 $$\sigma $$ $σ$ (5 $$\sigma $$ $σ$ ) after an exposure of 5 (10) years, for 50% of all $$\delta _{\mathrm{CP}}$$ $δ_{CP}$ 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 $$\sin ^{2} 2\theta _{13}$$ ${sin}^{2} 2 θ_{13}$ to current reactor experiments.
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      "title": "Long-baseline neutrino oscillation physics potential of the DUNE experiment"
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      "source": "Springer", 
      "value": "The 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 5 $$\\sigma $$  <math> <mi>\u03c3</mi> </math>  , for all  $$\\delta _{\\mathrm{CP}}$$  <math> <msub> <mi>\u03b4</mi> <mi>CP</mi> </msub> </math>   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 3 $$\\sigma $$  <math> <mi>\u03c3</mi> </math>   (5 $$\\sigma $$  <math> <mi>\u03c3</mi> </math>  ) after an exposure of 5 (10) years, for 50% of all  $$\\delta _{\\mathrm{CP}}$$  <math> <msub> <mi>\u03b4</mi> <mi>CP</mi> </msub> </math>   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  $$\\sin ^{2} 2\\theta _{13}$$  <math> <mrow> <msup> <mo>sin</mo> <mn>2</mn> </msup> <mn>2</mn> <msub> <mi>\u03b8</mi> <mn>13</mn> </msub> </mrow> </math>   to current reactor experiments."
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Published on:: 22 October 2020
Publisher:: Springer
Published in:: European Physical Journal C , Volume 80 (2020)
Issue 10
Pages 1-34
DOI:: https://doi.org/10.1140/epjc/s10052-020-08456-z
arXiv:: 2006.16043
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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