Home > Research > Publications & Outputs > Measurement of the νμ CCQE cross section on car...

Electronic data

  • 1411 (1).6264v1

    Accepted author manuscript, 377 KB, PDF document

    Available under license: CC BY: Creative Commons Attribution 4.0 International License

  • PhysRevD.92.112003

    Rights statement: © 2015 American Physical Society

    Final published version, 735 KB, PDF document

    Available under license: CC BY: Creative Commons Attribution 4.0 International License

Links

Text available via DOI:

View graph of relations

Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Published

Standard

Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K. / T2K Collaboration.
In: Physical Review D, Vol. 92, No. 11, 112003, 11.12.2015.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

APA

Vancouver

T2K Collaboration. Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K. Physical Review D. 2015 Dec 11;92(11):112003. doi: 10.1103/PhysRevD.92.112003, 10.1103/PhysRevD.92.112003

Author

T2K Collaboration. / Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K. In: Physical Review D. 2015 ; Vol. 92, No. 11.

Bibtex

@article{af05a607836d46a4ac8df97a887c8193,
title = "Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K",
abstract = "The Charged-Current Quasi-Elastic (CCQE) interaction, νl + n → l − + p, is the dominant CC process at Eν ∼ 1 GeV and contributes to the signal in accelerator-based long-baseline neutrino oscillation experiments operating at intermediate neutrino energies. This paper reports a measurement by the T2K experiment of the νµ CCQE cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum (pµ) and angle with respect to the incident neutrino beam (θµ). The flux-integrated CCQE cross section was measured to be hσi = (0.83 ± 0.12) × 10−38 cm2 . The energy dependence of the CCQE cross section is also reported. The axial mass, MQE A , of the dipole axial form factor was extracted assuming the Smith-Moniz CCQE model with a relativistic Fermi gas nuclear model. Using the absolute (shapeonly) pµ-cosθµ distribution, the effective M QE A parameter was measured to be 1.26+0.21 −0.18 GeV/c2 (1.43+0.28 −0.22 GeV/c2 ).",
keywords = "SINGLE PION-PRODUCTION, RESONANCE REGION, DELTA-RESONANCE, TRUE ABSORPTION, NUCLEAR TARGETS, GEV-C, SCATTERING, EXCHANGE, EXCITATION",
author = "K. Abe and J. Adam and H. Aihara and T. Akiri and C. Andreopoulos and S. Aoki and A. 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 V. Berardi and Berger, {B. E.} and S. Berkman and S. Bhadra and Blaszczyk, {F. d. M.} and A. Blondel and C. Bojechko and S. Bolognesi 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 A. Clifton 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 D. Shaw and L. Southwell and {T2K Collaboration}",
note = "{\textcopyright} 2015 American Physical Society",
year = "2015",
month = dec,
day = "11",
doi = "10.1103/PhysRevD.92.112003",
language = "English",
volume = "92",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "11",

}

RIS

TY - JOUR

T1 - Measurement of the νμ CCQE cross section on carbon with the ND280 detector at T2K

AU - Abe, K.

AU - Adam, J.

AU - Aihara, H.

AU - Akiri, T.

AU - Andreopoulos, C.

AU - Aoki, S.

AU - Ariga, A.

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 - Berardi, V.

AU - Berger, B. E.

AU - Berkman, S.

AU - Bhadra, S.

AU - Blaszczyk, F. d. M.

AU - Blondel, A.

AU - Bojechko, C.

AU - Bolognesi, S.

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 - Clifton, A.

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 - Shaw, D.

AU - Southwell, L.

AU - T2K Collaboration

N1 - © 2015 American Physical Society

PY - 2015/12/11

Y1 - 2015/12/11

N2 - The Charged-Current Quasi-Elastic (CCQE) interaction, νl + n → l − + p, is the dominant CC process at Eν ∼ 1 GeV and contributes to the signal in accelerator-based long-baseline neutrino oscillation experiments operating at intermediate neutrino energies. This paper reports a measurement by the T2K experiment of the νµ CCQE cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum (pµ) and angle with respect to the incident neutrino beam (θµ). The flux-integrated CCQE cross section was measured to be hσi = (0.83 ± 0.12) × 10−38 cm2 . The energy dependence of the CCQE cross section is also reported. The axial mass, MQE A , of the dipole axial form factor was extracted assuming the Smith-Moniz CCQE model with a relativistic Fermi gas nuclear model. Using the absolute (shapeonly) pµ-cosθµ distribution, the effective M QE A parameter was measured to be 1.26+0.21 −0.18 GeV/c2 (1.43+0.28 −0.22 GeV/c2 ).

AB - The Charged-Current Quasi-Elastic (CCQE) interaction, νl + n → l − + p, is the dominant CC process at Eν ∼ 1 GeV and contributes to the signal in accelerator-based long-baseline neutrino oscillation experiments operating at intermediate neutrino energies. This paper reports a measurement by the T2K experiment of the νµ CCQE cross section on a carbon target with the off-axis detector based on the observed distribution of muon momentum (pµ) and angle with respect to the incident neutrino beam (θµ). The flux-integrated CCQE cross section was measured to be hσi = (0.83 ± 0.12) × 10−38 cm2 . The energy dependence of the CCQE cross section is also reported. The axial mass, MQE A , of the dipole axial form factor was extracted assuming the Smith-Moniz CCQE model with a relativistic Fermi gas nuclear model. Using the absolute (shapeonly) pµ-cosθµ distribution, the effective M QE A parameter was measured to be 1.26+0.21 −0.18 GeV/c2 (1.43+0.28 −0.22 GeV/c2 ).

KW - SINGLE PION-PRODUCTION

KW - RESONANCE REGION

KW - DELTA-RESONANCE

KW - TRUE ABSORPTION

KW - NUCLEAR TARGETS

KW - GEV-C

KW - SCATTERING

KW - EXCHANGE

KW - EXCITATION

U2 - 10.1103/PhysRevD.92.112003

DO - 10.1103/PhysRevD.92.112003

M3 - Journal article

VL - 92

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 11

M1 - 112003

ER -