Deep Underground Neutrino Experiment (DUNE), Far Detector Technical Design Report, Volume IV: Far Detector Single-phase Technology

Abi, B.; Acciarri, R.; Acero, M. A.; Adamov, G.; Adams, D. L.; Adinolfi, M.; Ahmad, Zahid; Ahmed, Jamal; Alion, T.; Monsalve, S. Alonso; Alt, C.; Anderson, J.; Andreopoulos, C.; Andrews, M.; Andrianala, F.; Andringa, S.; Ankowski, A.; Anthony, J.; Antonova, M.; Antusch, Stefan; Fernandez, A. Aranda; Ariga, A.; Arnold, L.; Arroyave, M. A.; Asaadi, J.; Aurisano, A.; Aushev, V.; Autiero, D.; Azfar, F.; Back, H. O.; Back, J. J.; Backhouse, C.; Baesso, P.; Bagby, L.; Bajou, R.; Balasubramanian, S.; Baldi, Pierre; Bambah, Bindu A.; Barão, F.; Barenboim, Gabriela; Barker, G. J.; Barkhouse, W. A.; Barnes, C.; Barr, G.; Monarca, J. Barranco; Barros, N.; Barrow, J. L.; Bashyal, A.; Basque, V.; Bay, F.; Alba, J. L. Bazo; Beacom, J. F.; Bechetoille, E.; Behera, B. R.; Bellantoni, L.; Bellettini, G.; Bellini, Vincenzo; Beltramello, O.; Belver, D.; Benekos, N.; Neves, F.; Berger, Joshua; Berkman, S.; Bernardini, P.; Berner, R. M.; Berns, H.; Bertolucci, S.; Betancourt, M.; Bezawada, Y.; Bhattacharjee, M.; Bhuyan, B.; Biagi, S.; Bian, J. G.; Biassoni, M.; Biery, K.; Bilki, B.; Bishai, M.; Bitadze, A.; Blake, A.; Siffert, B. Blanco; Blaszczyk, F. d. M.; Blazey, G.; Blucher, E.; Boissevain, J.; Bolognesi, S.; Bolton, T.; Bonesini, M.; Bongrand, M.; Bonini, F.; Booth, Alexander; Booth, C.N.; Bordoni, S.; Borkum, A.; Boschi, T.; Bostan, N.; Bour, P.; Boyd, S. B.; Boyden, D.; Braciník, J.; Braga, D.; Brailsford, D.; Brandt, A.; Bremer, J.; Brew, C.; Brianne, Eldwan; Brice, S. J.; Brizzolari, C.; Bromberg, C.; Brooijmans, G.; Brooke, J. J.; Bross, A.; Brunetti, G.; Buchanan, N. J.; Budd, H. S.; Caiulo, D.; Calafiura, P.; Calcutt, J.; Călin, M.; Calvez, S.; Calvo, E.; Camilleri, L.; Caminata, A.; Campanelli, M.; Caratelli, D.; Carini, G.; Carlus, B.; Carniti, P.; Terrazas, I. Caro; Carranza, H.; Castillo, A.; Castromonte, C.; Cattadori, C.; Cavalier, F.; Cavanna, F.; Centro, S.; Cerati, G. B.; Cervelli, A.; Villanueva, A. Cervera; Chalifour, M.; Chang, C.; Chardonnet, Etienne; Chatterjee, A.; Chattopadhyay, S.; Chaves, J.; Chen, H.; Chen, M.; Chen, Y.; Cherdack, D.; Chi, C.Y.; Childress, S.; Chiriacescu, A.; Cho, K.; Choubey, Sandhya; Christensen, A.; Christian, David; Christodoulou, G.; Church, E.; Clarke, P. E. L.; Coan, T. E.; Cocco, A. G.; Coelho, J. A. B.; Conley, E.; Conrad, J. M.; Convery, M. R.; Corwin, L.; Cotte, P.; Cremaldi, L.; Cremonesi, L.; Crespo-Anadón, J. I.; Cristaldo, E.; Cross, R.; Cuesta, C.; Cui, Yanou; Cussans, D.; Dabrowski, M.; Motta, H. da; Peres, L. Da Silva; David, Q.; Davies, G. S.; Davini, S.; Dawson, Jim; De, K.; Almeida, R. M. de; Debbins, P.; Bonis, I. De; Decowski, M. P.; Gouvêa, A. de; Holanda, P. C. de; Astiz, I. L. De Icaza; Deisting, A.; Jong, P. de; Delbart, A.; Delépine, D.; Delgado, M.; Dell’Acqua, A.; Lurgio, P. De; Neto, J. R. T. de Mello; DeMuth, D. M.; Dennis, S. R.; Densham, C.; Deptuch, G.; Roeck, A. 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doi:10.48550/arxiv.2002.03010

Cited by 18 publications

(38 citation statements)

References 0 publications

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“…Sub-percent energy resolution could be achieved with light collection efficiency above 20%. However, this is more than two orders of magnitude greater than the current DUNE specification of 0.06% [42], and well beyond the percent-level light yields potentially attainable via design options with 10-20% effective photon sensor coverage. The isotropic nature of the scintillation light signal combined with the photon detector coverage in large detectors, and the intrinsic efficiency of photon detectors, present a challenge to increasing light collection efficiency that would require significant detector design changes to be overcome.…”

Section: Energy Resolutionmentioning

confidence: 82%

“…Sec. IV details the dominant backgrounds and mitigation strategies for MeV-scale radiogenic and neutron backgrounds, including the likely necessity of argon depleted in 42 Ar. Sec.…”

Section: A Experimental Conceptmentioning

confidence: 99%

“…Anthropogenic 42 Ar presents a significant background challenge for a doped 0νββ search in a large LArTPC. This synthetic isotope is present in trace quantities in argon extracted from the Earth's atmosphere, having been produced via nuclear fission.…”

Section: B Argon-42mentioning

confidence: 99%

“…This synthetic isotope is present in trace quantities in argon extracted from the Earth's atmosphere, having been produced via nuclear fission. The 42 Ar itself has a Q value of 599 keV, but the daughter 42 K decays to 42 Ca with Q = 3.53 MeV, directly to the ground state in 82% of cases. The 12-hour half-life of 42 K makes spatial coincidence tagging impractical, in light of ion drift and argon flow.…”

Section: B Argon-42mentioning

confidence: 99%

See 3 more Smart Citations

Xenon-Doped Liquid Argon TPCs as a Neutrinoless Double Beta Decay Platform

Mastbaum,

Psihas,

Zennamo

2022

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Section: Energy Resolutionmentioning

confidence: 82%

“…Sec. IV details the dominant backgrounds and mitigation strategies for MeV-scale radiogenic and neutron backgrounds, including the likely necessity of argon depleted in 42 Ar. Sec.…”

Section: A Experimental Conceptmentioning

confidence: 99%

Section: B Argon-42mentioning

confidence: 99%

Section: B Argon-42mentioning

confidence: 99%

See 2 more Smart Citations

Xenon-Doped Liquid Argon TPCs as a Neutrinoless Double Beta Decay Platform

Mastbaum,

Psihas,

Zennamo

2022

Preprint

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“…The study of scalar NSI has been a growing field to explore the possibility of new interactions in various neutrino experiments. In this paper, we explore the impact of a general scalar NSI on the neutrino mixing and for the first time, we have thoroughly studied its effects on the CP-violation sensitivity at the proposed long baseline neutrino experiment, DUNE [2].…”

mentioning

confidence: 99%

Exploring the effects of Scalar Non Standard Interactions on the CP violation sensitivity at DUNE

Medhi,

Dutta,

Devi

2021

Preprint

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Neutrino oscillations have provided an excellent opportunity to study new physics beyond the Standard Model or popularly known as BSM. The unknown couplings involving neutrinos, termed as Non Standard Interactions (NSIs), may appear as 'new physics' in different neutrino experiments. The neutrino NSIs offer significant effects in neutrino oscillations and CP sensitivity, which may be probed in various neutrino experiments. The idea of neutrinos coupling with a scalar has evolved recently and looks promising. The effects of scalar NSI may appear as a perturbation to the neutrino mass matrix in the neutrino Hamiltonian. Also, as it modifies the neutrino mass matrix, it may provide a direct possibility of probing neutrino mass models. As the scalar NSI affects the neutrino mass matrix in the Hamiltonian, its effect is energy independent. Moreover, the matter effects due to scalar NSI scales linearly with the matter density.In this work, we have performed a model independent study of the effects of scalar NSI at long baseline neutrino experiments, taking DUNE as a case study. We have done such a thorough study for the first time for DUNE. Various neutrino parameters may get affected due to the inclusion of scalar NSI as it modifies the effective mass matrix of neutrinos. We have explored the impact of scalar NSI in neutrino oscillations and its impact on the measurements of various mixing parameters. Also, we have probed the effects of scalar NSI on different oscillation channels relevant to the experiment. We have also explored the impact of various possible elements in the scalar NSI term at DUNE.

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