High-energy quasielastic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>ν</mml:mi></mml:mrow><mml:mrow><mml:mi>μ</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mi>n</mml:mi><mml:mo>→</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi>μ</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow><mml:mi>p</mml:mi></mml:math>scattering in deuterium

Kitagaki, T.; Tanaka, S.; Yuta, H.; Abe, K.; Hasegawa, K.; Yamaguchi, A.; Tamai, K.; Hayashino, T.; Otani, Yoshimi; Hayano, H.; Sagawa, H.; Burnstein, R. A.; Hanlon, J.; Rubin, H. A.; Chang, C. Y.; Kunori, S.; Snow, G. A.; Son, D.; Steinberg, P.; Ziemińska, D.; Engelmann, R.; Kafka, T.; Sommars, S.; Chang, C. C.; Mann, W. A.; Napier, A.; Schneps, J.

doi:10.1103/physrevd.28.436

Cited by 177 publications

(170 citation statements)

References 30 publications

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“…[34]. It is obtained from an analysis of pion electroproduction data [54] and measurements of the reaction ν µ + p → n + µ + [55]. Since here q 2 σ << Λ 2…”

Section: Weak Transition Operatormentioning

confidence: 99%

Muon capture on deuteron andHe3

et al. 2011

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The muon capture reactions 2 H(µ − , νµ)nn and 3 He(µ − , νµ) 3 H are studied with conventional or chiral realistic potentials and consistent weak currents. The initial and final A = 2 and 3 nuclear wave functions are obtained from the Argonne v18 or chiral N3LO two-nucleon potential, in combination with, respectively, the Urbana IX or chiral N2LO three-nucleon potential in the case of A = 3. The weak current consists of polar-and axial-vector components. The former are related to the isovector piece of the electromagnetic current via the conserved-vector-current hypothesis. These and the axial currents are derived either in a meson-exchange or in a chiral effective field theory (χEFT) framework. There is one parameter (either the N -to-∆ axial coupling constant in the meson-exchange model, or the strength of a contact term in the χEFT model) which is fixed by reproducing the Gamow-Teller matrix element in tritium β-decay. The model dependence relative to the adopted interactions and currents (and cutoff sensitivity in the χEFT currents) is weak, resulting in total rates of 392.0 ± 2.3 s −1 for A = 2, and 1484 ± 13 s −1 for A = 3, where the spread accounts for this model dependence.

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“…[34]. It is obtained from an analysis of pion electroproduction data [54] and measurements of the reaction ν µ + p → n + µ + [55]. Since here q 2 σ << Λ 2…”

Section: Weak Transition Operatormentioning

confidence: 99%

Muon capture on deuteron andHe3

et al. 2011

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“…Published results from the relevant experiments with ν µ and ν µ beams from accelerators at ANL [12][13][14][15][16][17][18][19], BNL [20][21][22][23][24][25][26][27][28][29][30][31][32][33], FNAL [34][35][36][37][38][39][40], CERN , and IHEP [65][66][67][68][69][70][71][72][73][74] are included dating from the end of sixties to the present day, covering a variety of nuclear targets, with energies ranging from about 150 MeV (ANL experiments) to about 350 GeV Table 2. Values of M A (given in GeV), extracted by fitting the νµ, νµ, and νµ + νµ data on total and differential QES cross sections, using the BBBA(07) and GKex(05) models for the vector form factors of the nucleon.…”

Section: Statistical Analysis Of the Data 41 Description Of Experimementioning

confidence: 99%

“…In this study, which is in a sense complementary to that by Bodek et al [3], we attempt to extract the axial mass value by a global statistical analysis of all available consistent data on the total and differential QES cross sections measured in accelerator experiments with ν µ and ν µ beams 1 from ANL [12][13][14][15][16][17][18][19], BNL [20][21][22][23][24][25][26][27][28][29][30][31][32][33], FNAL [34][35][36][37][38][39][40], CERN , and IHEP [65][66][67][68][69][70][71][72][73][74]. The detector media used in these experiments are hydrogen, deuterium, carbon, aluminium, argon, iron/steel, propane, freon, and also propane-freon and neon-hydrogen mixtures.…”

Section: Introductionmentioning

confidence: 99%

Quasielastic axial-vector mass from experiments on neutrino–nucleus scattering

2008

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Abstract. We analyse available experimental data on the total and differential charged-current cross sections for quasielastic νµN and νµN scattering, obtained with a variety of nuclear targets in the accelerator experiments at ANL, BNL, FNAL, CERN, and IHEP, dating from the end of sixties to the present day. The data are used to adjust the poorly known value of the axial-vector mass of the nucleon.

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“…Here g A is the nucleon axial coupling constant, g A = 1.2654, and the cutoff mass Λ A is taken to be 1 GeV/c 2 , as obtained from an analysis of pion electroproduction data [28] and measurements of the reaction ν µ p → µ + n [29]. There are relativistic corrections to j 5,1 as well as two-body contributions arising from π-, ρ-, ρπ-exchange mechanisms and ∆ excitation [24].…”

Section: Weak Operatorsmentioning

confidence: 99%

Parity-violating electron-deuteron scattering

2001

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The longitudinal asymmetry due to Z 0 exchange is calculated in quasi-elastic electron-deuteron scattering at momentum transfers |Q 2 | ≃ 0.1 GeV 2 relevant for the SAMPLE experiment. The deuteron and pn scattering-state wave functions are obtained from solutions of a Schrödinger equation with the Argonne v 18 potential. Electromagnetic and weak neutral one-and two-nucleon currents are included in the calculation. The two-nucleon currents of pion range are shown to be identical to those derived in Chiral Perturbation Theory. The results indicate that two-body contributions to the asymmetry are small (≃ 0.2%) around the quasi-elastic peak, but become relatively more significant (≃ 3%) in the high-energy wing of the quasielastic peak.pacs: 13.10.+q, 21.45.+v, 25.30.Fj

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High-energy quasielasticνμn→μ−pscattering in deuterium

Cited by 177 publications

References 30 publications

Muon capture on deuteron andHe3

Muon capture on deuteron andHe3

Quasielastic axial-vector mass from experiments on neutrino–nucleus scattering

Parity-violating electron-deuteron scattering

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