Measurement of the neutrino component of an antineutrino beam observed by a nonmagnetized detector

Aguilar-Arevalo, A. A.; Anderson, Carl E.; Brice, S. J.; Brown, Bruce; Bugel, L.; Conrad, J. M.; Dharmapalan, R.; Djurcic, Z.; Fleming, B. T.; Ford, R.; García, F.; Garvey, G. T.; Grange, Joseph; Green, J. A.; Imlay, R.; Johnson, R. A.; Karagiorgi, G.; Katori, T.; Kobilarcik, T.; Linden, S. K.; Louis, W. C.; Mahn, Kendall; Marsh, W.; Mauger, C.; Metcalf, W.; Mills, G. B.; Mirabal, J.; Moore, C. D.; Mousseau, J.; Nelson, Robert H.; Nguyen, V.; Nienaber, P.; Nowak, J.; Osmanov, B.; Patch, A.; Pavlović, Ž.; Perevalov, D.; Polly, C. C.; Ray, H.; Roe, B. P.; Russell, A. D.; Shaevitz, M. H.; Sorel, M.; Spitz, J.; Stancu, I.; Stefanski, R. J.; Tayloe, R.; Tzanov, M.; Water, R. G. Van de; Wascko, M. O.; White, D. H.; Wilking, M. J.; Zeller, G. P.; Zimmerman, E. D.

doi:10.1103/physrevd.84.072005

Cited by 33 publications

(36 citation statements)

References 43 publications

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“…The ratios for the predictions of the "Larger M A (M A = 1.3) model" and "Transverse Enhancement model" are shown. The data points are the ratios for the measurements of MiniBooNE [13,14] (gray stars) and NOMAD [30,31] (purple circles). Top (a): The ratio for ν μ total QE cross sections.…”

Section: Resultsmentioning

confidence: 99%

“…Figure 11 shows the total QE cross section as function of energy. The data points are the measurements from MiniBooNE [13,14] and NOMAD [30,31] Figure 12 shows the ratio of the predictions for total QE cross section to the predictions of the "Independent Nucleon (M A = 1.014)" model as a function energy. The blue dashed line is the ratio of the predictions for the "Larger M A (M A = 1.3)" model, and the red line is ratio for the "Transverse Enhancement" model (with error bands shown as dotted red lines).…”

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

“…11 The total QE cross section as function of energy. The data points are measurements of MiniBooNE [13,14] (gray stars) and NO-MAD [30,31] (purple circles). The predictions for the "Independent Nucleon (M A = 1.014)" model, "Larger M A (M A = 1.3) model", and "Transverse Enhancement model" are shown.…”

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

“…The bottom (c) panel shows the predictedν μ /ν μ cross section ratio divided by the predicted ν μ /ν μ ratio for the "Independent Nucleon (M A = 1.014)" model. The data points are measurements from MiniBooNE [13,14] and NOMAD [30,31].…”

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

“…a e-mail: bodek@pas.rochester.edu Models which assume that QE scattering on nuclear targets can be described in terms of scattering from independent nucleons bound in a nuclear potential (e.g. Fermi gas [12] or spectral functions) do not provide an adequate representation of measured differential and total QE cross sections for low energy (≈1 GeV) ν μ scattering on nucleons bound in carbon [13][14][15][16] (MiniBooNE) and oxygen [17,18] (K2K and T2K). The measured QE total cross sections are 20% larger than the model and the differential distributions in Q 2 are also inconsistent.…”

Section: Introductionmentioning

confidence: 99%

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Neutrino quasielastic scattering on nuclear targets

2011

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We present a parametrization of the observed enhancement in the transverse electron quasielastic (QE) response function for nucleons bound in carbon as a function of the square of the four momentum transfer (Q 2 ) in terms of a correction to the magnetic form factors of bound nucleons. The parametrization should also be applicable to the transverse cross section in neutrino scattering. If the transverse enhancement originates from meson exchange currents (MEC), then it is theoretically expected that any enhancement in the longitudinal or axial contributions is small. We present the predictions of the "Transverse Enhancement" model (which is based on electron scattering data only) for the ν μ ,ν μ differential and total QE cross sections for nucleons bound in carbon. The Q 2 dependence of the transverse enhancement is observed to resolve much of the long standing discrepancy in the QE total cross sections and differential distributions between low energy and high energy neutrino experiments on nuclear targets.

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Section: Resultsmentioning

confidence: 99%

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

Section: The "Transverse Enhancement" Modelmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

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Neutrino quasielastic scattering on nuclear targets

2011

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Charged current quasi elastic scattering of muon neutrino with nuclei

Saraswat¹,

Shukla²,

Kumar³

et al. 2017

Indian J Phys

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Abstract. We present a study on the charge current quasi elastic scattering of ν µ from nucleon and nuclei which gives a charged muon in the final state. To describe nuclei, the Fermi Gas model has been used with proposed Pauli suppression factor. The diffuseness parameter of the Fermi distribution has been obtained using experimental data. We also investigate different parametrizations for electric and magnetic Sach's form factors of nucleons. Calculations have been made for CCQES total and differential cross sections for the cases of ν µ − N , ν µ − 12 C and ν µ − 56 F e scatterings and are compared with the data for different values of the axial mass. The present model gives excellent description of measured differential cross section for all the systems.

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Improved statistics in the search for oscillations in MiniBooNE

Polly¹

2013

Nuclear Physics B - Proceedings Supplements

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Measurement of the neutrino component of an antineutrino beam observed by a nonmagnetized detector

Abstract: Phys. Rev. D

Cited by 33 publications

References 43 publications

Neutrino quasielastic scattering on nuclear targets

Neutrino quasielastic scattering on nuclear targets

Charged current quasi elastic scattering of muon neutrino with nuclei

Improved statistics in the search for oscillations in MiniBooNE

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