Study of the reaction

Barish, S.J.; Brock, R.; Engler, A.; Kikuchi, T.; Kraemer, R. W.; Messing, F.; Stacey, B.J.; Tabak, M.; Derrick, M.; Gregory, P.; LoPinto, F.; Musgrave, B.; Schlereth, J.; Schreiner, P.; Singer, R.; Barnes, V. E.; Carmony, D.D.; Fernández, E.; Garfinkel, A. F.; Laasanen, A. T.

doi:10.1016/0370-2693(80)90684-x

Cited by 25 publications

(14 citation statements)

References 10 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…It is nevertheless of interest to investigate whether cross sections measured in a hydrocarbon medium can be related to the underlying initial antineutrino-nucleon interactions. The CC(π) cross sections reported by the bubble chamber experiments of the 1970s and 80s, including those using propane-freon as well as deuterium or hydrogen fills, are entirely of the (anti)-neutrino plus quasi-free nucleon kind [14][15][16][17][18][19][20]. Such measurements require fine-grained event imaging and rely upon certain aspects of neutrino-interaction modeling, e.g.…”

Section: Estimation Ofνµ-nucleon Cross Sections In Hydrocarbonmentioning

confidence: 99%

“…Cross sections for reactions (2) and (3) taking place in propane + freon mixtures were obtained in the few-GeV region (< Eν > = 1.5 GeV) using Gargamelle [14,15] and over the range 3 to 30 GeV using SKAT [16]. Investigations of both reactions for incidentν µ energies exceeding 5 GeV were carried out using large deuterium-filled bubble chambers [17][18][19], and reaction (3) was studied over the range 5 < Eν < 120 GeV using BEBC with a hydrogen fill [20]. The relative contributions from baryon resonances was found to be rather different in the two exclusive reactions: Reaction (2) is an I = 3/2 channel in which production of the ∆ − (1232) resonance plays a major role, while (3) contains I = 1/2 as well as I = 3/2 amplitudes.…”

mentioning

confidence: 99%

See 1 more Smart Citation

Measurement of ν¯μ charged-current single π− production on hydrocarbon in the few-GeV region using MINERvA

Le¹,

Cai²,

Sultana³

et al. 2019

Phys. Rev. D

View full text Add to dashboard Cite

The antineutrino scattering channelνµ CH → µ + π − X(nucleon(s)) is analyzed in the incident energy range 1.5 to 10 GeV using the MINERvA detector at Fermilab. Differential cross sections are reported as functions of µ + momentum and production angle, π − kinetic energy and production angle, and antineutrino energy and squared four-momentum transfer. Distribution shapes are generally reproduced by simulations based on the GENIE, NuWro, and GiBUU event generators, however GENIE (GiBUU) overestimates (underestimates) the cross-section normalizations by 8% (10%). Comparisons of data with the GENIE-based reference simulation probe conventional treatments of cross sections and pion intranuclear rescattering. The distribution of non-track vertex energy is used to decompose the signal sample into reaction categories, and cross sections are determined for the exclusive reactions µ + π − n and µ + π − p. A similar treatment applied to the published MINERvA sampleνµ CH → µ + π 0 X(nucleon(s)) has determined the µ + π 0 n cross section, and the latter is used with σ(π − n) and σ(π − p) to carry out an isospin decomposition ofνµ-induced CC(π). The ratio of magnitudes and relative phase for isospin amplitudes A3 and A1 thereby obtained are: Rν = 0.99 ± 0.19 and φν = 93 • ± 7 • . Our results are in agreement with bubble chamber measurements made four decades ago.

show abstract

Section: Estimation Ofνµ-nucleon Cross Sections In Hydrocarbonmentioning

confidence: 99%

mentioning

confidence: 99%

Measurement of ν¯μ charged-current single π− production on hydrocarbon in the few-GeV region using MINERvA

Le¹,

Cai²,

Sultana³

et al. 2019

Phys. Rev. D

View full text Add to dashboard Cite

show abstract

“…We analyzed and classified all available 1π-production experimental data, presented as the ν µ and ν µ scattering cross sections on hydrogen and deuterium targets measured in ANL [43][44][45][46][47][48][49][50][51][52][53], BNL [54][55][56][57][58], FNAL [59][60][61][62], and CERN [63][64][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80] accelerator experiments from the beginning of the 70s to 90s with energy ranges from about hundreds of MeV (ANL) to tens of GeV (CERN).…”

Section: Experimental Datasetmentioning

confidence: 99%

“…The datasets of ANL 1982 [53] and BNL 1986 [58] include the original data and the data recalculated by Furuno et al [81][82][83] and Rodrigues et al [84]. In the statistical analysis we use the experimental data on measuring the ratio of the total cross section of the res- [43], 1975 [46], 1976 [47], 1978 [49], 1979 [50], 1982 [53], BNL 1986 [58], FNAL 1978 [59,60], 1980 [62], and CERN BEBC 1980 [74], 1984 [76], 1986 [77], 1989 [78], 1990 [80]. The original data of ANL 1982 [53] and BNL 1986 [58] are recalculated by Rodrigues et al [84].…”

Section: Experimental Datasetmentioning

confidence: 99%

Resonance axial-vector mass from experiments on neutrino-hydrogen and neutrino-deuterium scattering

Kakorin,

Kuzmin

2021

Preprint

View full text Add to dashboard Cite

We analyze all available experimental data on the νµ and νµ total and differential cross sections of charged-current single pion production through the decay of intermediate nucleon and baryon resonances measured on hydrogen and deuterium targets in the accelerator experiments at ANL, BNL, FNAL, and CERN. These data are used to determine the current "resonance" axial-vector mass of the nucleon and to fine-tune the nonresonance non-interfering background contribution which described within the Rein-Sehgal approach. For this analysis, we revise the phenomenological model and the experimental dataset for the fits, modify the method of likelihood analysis compared to the previous study. The obtained model parameters coming in combination with a revised strategy for the normalization of the BW distributions are slightly different from the values used by default.

show abstract

“…Also experimental input to the ratio between NC and CC cross section must be taken Channel Experiment Target No. Events Table 2.4: Measurements of antineutrino CCν single pion production from BEBC ( [37], [38], [39]), FNAL ( [40]), Gargamelle ( [41]), and Sepukhov heavy liquid chamber (SKAT) ( [42]).…”

Section: Resonant Single Pion Productionmentioning

confidence: 99%

First Measurement of $\nu_{\mu}$ Induced Charged-Current $\pi^0$ Production Cross Sections on Polystyrene at $E_{\bar{\nu}_{\mu}}$ 2-10 GeV

Gallo¹,

Luís²

2012

View full text Add to dashboard Cite

is an great advisor. He usually let me work things out for myself instead of giving me something already done. Special thanks to Dr. Jorge Morn, he was very supportive to the Latino group. Many thanks to our spokespersons, Dr. Deborah Harris and Dr. Kevin McFarland, who have been very nice. To CAPES and CNPQ for the scholarship (2008-2012), the University of Pittsburgh, Department Physics of and Astronomy for my appointment as a Visiting Scholar (2012). Thanks to CBPF administrative sta José de Almeida Ricardo and Elisabete Vicente. To FERMI-LAB administrative sta

show abstract

Study of the reaction

Cited by 25 publications

References 10 publications

Measurement of ν¯μ charged-current single π− production on hydrocarbon in the few-GeV region using MINERvA

Measurement of ν¯μ charged-current single π− production on hydrocarbon in the few-GeV region using MINERvA

Resonance axial-vector mass from experiments on neutrino-hydrogen and neutrino-deuterium scattering

First Measurement of $\nu_{\mu}$ Induced Charged-Current $\pi^0$ Production Cross Sections on Polystyrene at $E_{\bar{\nu}_{\mu}}$ 2-10 GeV

Contact Info

Product

Resources

About