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First measurement of the muon neutrino charged current single pion production cross section on water with the T2K near detector

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First measurement of the muon neutrino charged current single pion production cross section on water with the T2K near detector. / T2K Collaboration.
In: Physical Review D, Vol. 95, No. 1, 012010, 01.2017.

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T2K Collaboration. First measurement of the muon neutrino charged current single pion production cross section on water with the T2K near detector. Physical Review D. 2017 Jan;95(1):012010. Epub 2017 Jan 26. doi: 10.1103/PhysRevD.95.012010

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@article{cb40b1a4adb745248acda3a8cbc05cb5,
title = "First measurement of the muon neutrino charged current single pion production cross section on water with the T2K near detector",
abstract = "The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$~GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+}>200$MeV/c, $p_{\mu^-}>200$MeV/c, $\cos \theta_{\pi^+}>0.3$ and $\cos \theta_{\mu^-}>0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$. The total cross section is consistent with the NEUT prediction ($5.03\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$) and 2$\sigma$ lower than the GENIE prediction ($7.68\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$). The differential cross sections are in good agreement with the NEUT generator. The GENIE simulation reproduces well the shapes of the distributions, but over-estimates the overall cross section normalization.",
keywords = "hep-ex",
author = "K. Abe and C. Andreopoulos and M. Antonova and S. Aoki and A. Ariga and S. Assylbekov and D. Autiero and S. Ban and M. Barbi and Barker, {G. J.} and G. Barr and P. Bartet-Friburg and M. Batkiewicz and F. Bay and V. Berardi and S. Berkman and S. Bhadra and S. Bienstock and A. Blondel and S. Bolognesi and S. Bordoni and D. Brailsford and A. Bravar and C. Bronner and Avanzini, {M. Buizza} and Calland, {R. G.} and T. Campbell and S. Cao and Rodr{\'i}guez, {J. Caravaca} and R. Castillo and Catanesi, {M. G.} and A. Cervera and D. Cherdack and N. Chikuma and G. Christodoulou and J. Coleman and G. Collazuol and D. Coplowe and T. Dealtry and Finch, {A. J.} and N. Grant and A. Knox and Kormos, {L. L.} and I. Lamont and M. Lawe and J. Nowak and O'Keeffe, {H. M.} and Ratoff, {P. N.} and D. Shaw and L. Southwell and {T2K Collaboration}",
year = "2017",
month = jan,
doi = "10.1103/PhysRevD.95.012010",
language = "English",
volume = "95",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "1",

}

RIS

TY - JOUR

T1 - First measurement of the muon neutrino charged current single pion production cross section on water with the T2K near detector

AU - Abe, K.

AU - Andreopoulos, C.

AU - Antonova, M.

AU - Aoki, S.

AU - Ariga, A.

AU - Assylbekov, S.

AU - Autiero, D.

AU - Ban, S.

AU - Barbi, M.

AU - Barker, G. J.

AU - Barr, G.

AU - Bartet-Friburg, P.

AU - Batkiewicz, M.

AU - Bay, F.

AU - Berardi, V.

AU - Berkman, S.

AU - Bhadra, S.

AU - Bienstock, S.

AU - Blondel, A.

AU - Bolognesi, S.

AU - Bordoni, S.

AU - Brailsford, D.

AU - Bravar, A.

AU - Bronner, C.

AU - Avanzini, M. Buizza

AU - Calland, R. G.

AU - Campbell, T.

AU - Cao, S.

AU - Rodríguez, J. Caravaca

AU - Castillo, R.

AU - Catanesi, M. G.

AU - Cervera, A.

AU - Cherdack, D.

AU - Chikuma, N.

AU - Christodoulou, G.

AU - Coleman, J.

AU - Collazuol, G.

AU - Coplowe, D.

AU - Dealtry, T.

AU - Finch, A. J.

AU - Grant, N.

AU - Knox, A.

AU - Kormos, L. L.

AU - Lamont, I.

AU - Lawe, M.

AU - Nowak, J.

AU - O'Keeffe, H. M.

AU - Ratoff, P. N.

AU - Shaw, D.

AU - Southwell, L.

AU - T2K Collaboration

PY - 2017/1

Y1 - 2017/1

N2 - The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$~GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+}>200$MeV/c, $p_{\mu^-}>200$MeV/c, $\cos \theta_{\pi^+}>0.3$ and $\cos \theta_{\mu^-}>0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$. The total cross section is consistent with the NEUT prediction ($5.03\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$) and 2$\sigma$ lower than the GENIE prediction ($7.68\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$). The differential cross sections are in good agreement with the NEUT generator. The GENIE simulation reproduces well the shapes of the distributions, but over-estimates the overall cross section normalization.

AB - The T2K off-axis near detector, ND280, is used to make the first differential cross section measurements of muon neutrino charged current single positive pion production on a water target at energies ${\sim}0.8$~GeV. The differential measurements are presented as a function of muon and pion kinematics, in the restricted phase-space defined by $p_{\pi^+}>200$MeV/c, $p_{\mu^-}>200$MeV/c, $\cos \theta_{\pi^+}>0.3$ and $\cos \theta_{\mu^-}>0.3$. The total flux integrated $\nu_\mu$ charged current single positive pion production cross section on water in the restricted phase-space is measured to be $\langle\sigma\rangle_\phi=4.25\pm0.48~(\mathrm{stat})\pm1.56~(\mathrm{syst})\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$. The total cross section is consistent with the NEUT prediction ($5.03\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$) and 2$\sigma$ lower than the GENIE prediction ($7.68\times10^{-40}~\mathrm{cm}^{2}/\mathrm{nucleon}$). The differential cross sections are in good agreement with the NEUT generator. The GENIE simulation reproduces well the shapes of the distributions, but over-estimates the overall cross section normalization.

KW - hep-ex

U2 - 10.1103/PhysRevD.95.012010

DO - 10.1103/PhysRevD.95.012010

M3 - Journal article

VL - 95

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 1

M1 - 012010

ER -