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Accurate modeling of the absorption of tens-of-MeV $\nu_e$ on $^{40}$Ar is needed to enable measurements of astrophysical neutrinos using large liquid argon time projection chamber (LArTPC) detectors, such as those planned for the Deep…

High Energy Physics - Phenomenology · Physics 2026-04-30 Steven Gardiner , Pablo Barham Alzás , Alexis Nikolakopoulos , Luca H. Abu El-Haj , Natalie Jachowicz , Vishvas Pandey

In view of the great interest in liquid argon neutrino detectors, the $^{40}$Ar($\gamma,\gamma'$)$^{40}$Ar$^{*}$ reaction was revisited to guide a calculation of the neutral current neutrino cross section at supernova energies. Using the…

Nuclear Experiment · Physics 2022-12-14 W. Tornow , A. P. Tonchev , S. W. Finch , Krishichayan , X. B. Wang , A. C. Hayes , H. G. D. Yeomans , D. A. Newmark

The charged-current quasi-elastic scattering of muon neutrinos on calcium and argon targets is calculated for neutrino energy up to 2.8 GeV. The calculations are done within the framework of the relativistic distorted-wave impulse…

Nuclear Theory · Physics 2013-05-30 A. V. Butkevich

Superscaling analyses of few-GeV inclusive electron scattering from nuclei are extended to include not only quasielastic processes, but now also into the region where $\Delta$-excitation dominates. It is shown that, with reasonable…

Nuclear Theory · Physics 2008-11-26 J. E. Amaro , M. B. Barbaro , J. A. Caballero , T. W. Donnelly , A. Molinari , I. Sick

Background: 12C has been and is still widely used in neutrino-nucleus scattering and oscillation experiments. More recently, 40Ar has emerged as an important nuclear target for current and future experiments. Liquid argon time projection…

Electron-neutrino charged-current interactions with xenon nuclei were modeled in the nEXO neutrinoless double-$\beta$ decay detector (~5 metric ton, 90% ${}^{136}$Xe, 10% ${}^{134}$Xe) to evaluate its sensitivity to supernova neutrinos.…

High Energy Physics - Phenomenology · Physics 2024-12-02 nEXO Collaboration , S. Hedges , S. Al Kharusi , E. Angelico , J. P. Brodsky , G. Richardson , S. Wilde , A. Amy , A. Anker , I. J. Arnquist , P. Arsenault , A. Atencio , I. Badhrees , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Q. Cao , D. Cesmecioglu , E. Chambers , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , R. Collister , M. Cvitan , J. Dalmasson , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , Y. Y. Ding , M. J. Dolinski , B. Eckert , M. Elbeltagi , R. Elmansali , L. Fabris , W. Fairbank , J. Farine , N. Fatemighomi , B. Foust , Y. S. Fu , D. Gallacher , N. Gallice , W. Gillis , D. Goeldi , A. Gorham , R. Gornea , G. Gratta , Y. D. Guan , C. A. Hardy , M. Heffner , E. Hein , J. D. Holt , E. W. Hoppe , A. House , W. Hunt , A. Iverson , P. Kachru , A. Karelin , D. Keblbeck , A. Kuchenkov , K. S. Kumar , A. Larson , M. B. Latif , K. G. Leach , B. G. Lenardo , D. S. Leonard , H. Lewis , G. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , P. Martel-Dion , J. Masbou , K. McMichael , M. Medina-Peregrina , B. Mong , D. C. Moore , J. Nattress , C. R. Natzke , X. E. Ngwadla , K. Ni , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , J. L. Orrell , G. S. Ortega , C. T. Overman , L. Pagani , H. Peltz Smalley , A. Peña-Perez , A. Perna , A. Piepke , T. Pinto Franco , A. Pocar , J. -F. Pratte , H. Rasiwala , D. Ray , K. Raymond , S. Rescia , V. Riot , R. Ross , R. Saldanha , S. Sangiorgio , S. Schwartz , S. Sekula , J. Soderstrom , A. K. Soma , F. Spadoni , X. L. Sun , S. Thibado , A. Tidball , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , E. van Bruggen , M. Vidal , S. Viel , M. Walent , Q. D. Wang , W. Wang , Y. G. Wang , M. Watts , M. Wehrfritz , W. Wei , L. J. Wen , U. Wichoski , X. M. Wu , H. Xu , H. B. Yang , L. Yang , M. Yu , M. Yvaine , O. Zeldovich , J. Zhao

Present and next generation of long-baseline accelerator experiments are bringing the measurement of neutrino oscillations into the precision era with ever-increasing statistics. One of the most challenging aspects of achieving such…

Neutrino-nucleus interactions play an important role in present and future neutrino experiments. The accurate simulation of these interactions at low energies ($<$100 MeV) is crucial for the detection and study of supernova, solar and…

High Energy Physics - Experiment · Physics 2024-04-02 Pablo Barham Alzás , Radi Radev

Background: Neutrino-nucleus quasi-elastic scattering is crucial to interpret the neutrino oscillation results in long baseline neutrino experiments. There are rather large uncertainties in the cross section, due to insufficient knowledge…

Nuclear Theory · Physics 2012-09-13 G. Shen , L. E. Marcucci , J. Carlson , S. Gandolfi , R. Schiavilla

We present a model for weak CC induced nuclear reactions at energies of interest for current and future neutrino oscillation experiments. This model is a natural extension of the work of Refs.[1,2], where the QE contribution to the…

High Energy Physics - Phenomenology · Physics 2013-05-29 J. Nieves , I. Ruiz Simo , M. J. Vicente Vacas

[Background] Meticulous modeling of neutrino-nucleus interactions is essential to achieve the unprecedented precision goals of present and future accelerator-based neutrino-oscillation experiments. [Purpose] Confront our calculations of…

The cross sections for the \nu-d and \bar{\nu}-d reactions are calculated for the incident energy up to E_\nu = 170 MeV, with the use of a phenomenological Lagrangian approach. We assess and improve the reliability of the employed…

Nuclear Theory · Physics 2014-11-18 S. Nakamura , T. Sato , V. Gudkov , K. Kubodera

The cross sections for neutrino scattering off the 12C and 16O nuclei are calculated within the framework of the continuum Random Phase Approximation. A model to consider also the final state interactions is developed. Total…

Nuclear Theory · Physics 2009-11-11 Antonio Botrugno , Giampaolo Co'

The neutrino energy reconstruction is crucial for reducing systematic uncertainties in neutrino oscillation experiments and improving cross-section measurements. Kaon-Decays-At-Rest (KDAR) neutrinos provide a unique opportunity to probe…

High Energy Physics - Phenomenology · Physics 2025-09-04 Ritesh Kumar Pradhan , Ralte Lalnuntluanga , Anjan Giri

The MINER$\nu$A experiment investigates neutrino interactions with nucleons needed for an understanding of electroweak interactions of hadrons. Since nuclear targets are being used many-body effects may affect the extracted cross sections…

Nuclear Theory · Physics 2014-06-13 U. Mosel , O. Lalakulich , K. Gallmeister

We examine a potential role of the neutrino deuteron reactions in the mechanism of supernova explosion by evaluating the energy transfer cross section for the neutrino heating. We calculate the energy loss rate due to the neutrino…

Nuclear Theory · Physics 2009-11-06 S. X. Nakamura , K. Sumiyoshi , T. Sato

This study quantifies the impact of nuclear de-excitation on correlations in multi-nucleon transfer (MNT) reactions. To bridge the gap between initial collision dynamics and final experimental observables, we introduce a hybrid…

Nuclear Theory · Physics 2026-04-14 Y. C. Yang , D. D. Zhang , D. Vretenar , B. Li , T. Nikšić , P. W. Zhao , J. Meng

We study the impact of neutrino-pair production from the de-excitation of highly excited heavy nuclei on core-collapse supernova simulations, following the evolution up to several 100 ms after core bounce. Our study is based on the…

High Energy Astrophysical Phenomena · Physics 2015-06-17 Tobias Fischer , Karlheinz Langanke , Gabriel Martinez-Pinedo

In ultraperipheral heavy-ion collisions (UPCs) at the Large Hadron Collider (LHC) Pb nuclei are excited through interactions induced by strong electromagnetic fields. The expected excitation energy could reach hundreds MeV, which leads to…

High Energy Physics - Phenomenology · Physics 2025-02-13 P. Jucha , K. Mazurek , M. Klusek-Gawenda , M. Ciemala , A. Szczurek , Yuliia Shevchuk , S. Słotwiński

High intensity monoenergetic muon neutrinos of energy 236 MeV from kaon decay at rest (KDAR) at the medium energy proton accelerator facilities like J-PARC and Fermilab are proposed to be used for making precision measurements of…

Nuclear Theory · Physics 2017-12-06 F Akbar , M. Sajjad Athar , S. K. Singh
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