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Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation $γ$ rays

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Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation $γ$ rays. / T2K Collaboration.
In: Physical Review D, Vol. 90, No. 7, 072012, 31.10.2014.

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T2K Collaboration. Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation $γ$ rays. Physical Review D. 2014 Oct 31;90(7):072012. doi: 10.1103/PhysRevD.90.072012

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@article{4c05f8e5ae084e58bd5cd1ce678a558f,
title = "Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation $γ$ rays",
abstract = "We report the first measurement of the neutrino-oxygen neutral-current quasielastic (NCQE) cross section. It is obtained by observing nuclear deexcitation $\gamma$-rays which follow neutrino-oxygen interactions at the Super-Kamiokande water Cherenkov detector. We use T2K data corresponding to $3.01 \times 10^{20}$ protons on target. By selecting only events during the T2K beam window and with well-reconstructed vertices in the fiducial volume, the large background rate from natural radioactivity is dramatically reduced. We observe 43 events in the $4-30$ MeV reconstructed energy window, compared with an expectation of 51.0, which includes an estimated 16.2 background events. The background is primarily nonquasielastic neutral-current interactions and has only 1.2 events from natural radioactivity. The flux-averaged NCQE cross section we measure is $1.55 \times 10^{-38}$ cm$^2$ with a 68\% confidence interval of $(1.22, 2.20) \times 10^{-38}$ cm$^2$ at a median neutrino energy of 630 MeV, compared with the theoretical prediction of $2.01 \times 10^{-38}$ cm$^2$.",
keywords = "hep-ex",
author = "K. Abe and J. Adam and H. Aihara and T. Akiri and C. Andreopoulos and S. Aoki and A. Ariga and T. Ariga and S. Assylbekov and D. Autiero and M. Barbi and Barker, {G. J.} and G. Barr and M. Bass and M. Batkiewicz and F. Bay and Bentham, {S. W.} and V. Berardi and Berger, {B. E.} and S. Berkman and I. Bertram and S. Bhadra and Blaszczyk, {F. d. M.} and A. Blondel and C. Bojechko and S. Bordoni and Boyd, {S. B.} and D. Brailsford and A. Bravar and C. Bronner and N. Buchanan and Calland, {R. G.} and Rodr{\'i}guez, {J. Caravaca} and Cartwright, {S. L.} and R. Castillo and Catanesi, {M. G.} and A. Cervera and D. Cherdack and G. Christodoulou and T. Dealtry and Finch, {A. J.} and N. Grant and Kormos, {L. L.} and I. Lamont and M. Lawe and J. Nowak and O'Keeffe, {H. M.} and Ratoff, {P. N.} and M. Reeves and L. Southwell and {T2K Collaboration}",
note = "10 pages, 6 figures {\textcopyright} 2014 American Physical Society",
year = "2014",
month = oct,
day = "31",
doi = "10.1103/PhysRevD.90.072012",
language = "English",
volume = "90",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "7",

}

RIS

TY - JOUR

T1 - Measurement of the neutrino-oxygen neutral-current interaction cross section by observing nuclear deexcitation $γ$ rays

AU - Abe, K.

AU - Adam, J.

AU - Aihara, H.

AU - Akiri, T.

AU - Andreopoulos, C.

AU - Aoki, S.

AU - Ariga, A.

AU - Ariga, T.

AU - Assylbekov, S.

AU - Autiero, D.

AU - Barbi, M.

AU - Barker, G. J.

AU - Barr, G.

AU - Bass, M.

AU - Batkiewicz, M.

AU - Bay, F.

AU - Bentham, S. W.

AU - Berardi, V.

AU - Berger, B. E.

AU - Berkman, S.

AU - Bertram, I.

AU - Bhadra, S.

AU - Blaszczyk, F. d. M.

AU - Blondel, A.

AU - Bojechko, C.

AU - Bordoni, S.

AU - Boyd, S. B.

AU - Brailsford, D.

AU - Bravar, A.

AU - Bronner, C.

AU - Buchanan, N.

AU - Calland, R. G.

AU - Rodríguez, J. Caravaca

AU - Cartwright, S. L.

AU - Castillo, R.

AU - Catanesi, M. G.

AU - Cervera, A.

AU - Cherdack, D.

AU - Christodoulou, G.

AU - Dealtry, T.

AU - Finch, A. J.

AU - Grant, N.

AU - Kormos, L. L.

AU - Lamont, I.

AU - Lawe, M.

AU - Nowak, J.

AU - O'Keeffe, H. M.

AU - Ratoff, P. N.

AU - Reeves, M.

AU - Southwell, L.

AU - T2K Collaboration

N1 - 10 pages, 6 figures © 2014 American Physical Society

PY - 2014/10/31

Y1 - 2014/10/31

N2 - We report the first measurement of the neutrino-oxygen neutral-current quasielastic (NCQE) cross section. It is obtained by observing nuclear deexcitation $\gamma$-rays which follow neutrino-oxygen interactions at the Super-Kamiokande water Cherenkov detector. We use T2K data corresponding to $3.01 \times 10^{20}$ protons on target. By selecting only events during the T2K beam window and with well-reconstructed vertices in the fiducial volume, the large background rate from natural radioactivity is dramatically reduced. We observe 43 events in the $4-30$ MeV reconstructed energy window, compared with an expectation of 51.0, which includes an estimated 16.2 background events. The background is primarily nonquasielastic neutral-current interactions and has only 1.2 events from natural radioactivity. The flux-averaged NCQE cross section we measure is $1.55 \times 10^{-38}$ cm$^2$ with a 68\% confidence interval of $(1.22, 2.20) \times 10^{-38}$ cm$^2$ at a median neutrino energy of 630 MeV, compared with the theoretical prediction of $2.01 \times 10^{-38}$ cm$^2$.

AB - We report the first measurement of the neutrino-oxygen neutral-current quasielastic (NCQE) cross section. It is obtained by observing nuclear deexcitation $\gamma$-rays which follow neutrino-oxygen interactions at the Super-Kamiokande water Cherenkov detector. We use T2K data corresponding to $3.01 \times 10^{20}$ protons on target. By selecting only events during the T2K beam window and with well-reconstructed vertices in the fiducial volume, the large background rate from natural radioactivity is dramatically reduced. We observe 43 events in the $4-30$ MeV reconstructed energy window, compared with an expectation of 51.0, which includes an estimated 16.2 background events. The background is primarily nonquasielastic neutral-current interactions and has only 1.2 events from natural radioactivity. The flux-averaged NCQE cross section we measure is $1.55 \times 10^{-38}$ cm$^2$ with a 68\% confidence interval of $(1.22, 2.20) \times 10^{-38}$ cm$^2$ at a median neutrino energy of 630 MeV, compared with the theoretical prediction of $2.01 \times 10^{-38}$ cm$^2$.

KW - hep-ex

U2 - 10.1103/PhysRevD.90.072012

DO - 10.1103/PhysRevD.90.072012

M3 - Journal article

VL - 90

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 7

M1 - 072012

ER -