Cross-section measurements of single pion production in charged current neutrino and antineutrino interactions

Grabosch, H. J.; Kaufmann, H. H.; Nahnhauer, R.; Nowak, S.; Schlenstedt, S.; Ammosov, V. V.; Baranov, D.S.; Hleborad, V. I.; Ivanilov, A.; Иванов, П. В.; Konyushko, V.I.; Korablev, V. M.; Коротков, В. А.; Макеев, В. В.; Myagkov, A. G.; Netyaga, N.A.; Polyarush, A. Yu.; Sokolov, A.

doi:10.1007/bf01564697

Cited by 32 publications

(17 citation statements)

References 24 publications

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“…[14] (empty circles) and from Ref. [15] (crosses). Also in this case the agreement between the theoretical results and the data points is reasonably good.…”

Section: B Resultsmentioning

confidence: 99%

Single pion production in neutrino reactions and estimates for charge-exchange effects

Paschos

Pasquali

2000

Nuclear Physics B

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We calculate single pion production by neutrinos in the resonance region. We consider both charged and neutral current reactions on free protons and neutrons. We present differential and total cross sections which can be compared with experiments. Then we use these results to calculate the spectra of the emerging pions including the Pauli suppression factor and rescattering corrections for reactions in heavy nuclei. Our results will be useful for studying single pion production and for investigating neutrino oscillations in future experiments.

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“…[14] (empty circles) and from Ref. [15] (crosses). Also in this case the agreement between the theoretical results and the data points is reasonably good.…”

Section: B Resultsmentioning

confidence: 99%

Single pion production in neutrino reactions and estimates for charge-exchange effects

Paschos

Pasquali

2000

Nuclear Physics B

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“…(A recent reanalysis obtains consistency between these two data sets [43] , however the generator predictions shown here have not been tuned to the results of this reanalysis.) For the channelν µ +p → µ + +π 0 +n there is only one cross-section data point, obtained with antineutrino scattering on a heavy-liquid (freon CF 3 Br) bubble chamber fill [44].…”

Section: Comparison Of the Dashed And Solid-line Histograms Inmentioning

confidence: 99%

Cross sections forνμandν¯μinduced pion production on hydrocarbon in the few-GeV region using MINERvA

McGivern¹,

Le²,

Eberly³

et al. 2016

Phys. Rev. D

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Cross sections for ν_{μ} and ν[over ¯]_{μ} induced pion production on hydrocarbon in the few-GeV region using MINERvA FERMILAB-PUB-16-228-NDCross sections for ν µ andν µ induced pion production on hydrocarbon in the few-GeV region using MINERvA Separate samples of charged-current pion production events representing two semi-inclusive channels νµ-CC(π + ) andνµ-CC(π 0 ) have been obtained using neutrino and antineutrino exposures of the MINERvA detector. Distributions in kinematic variables based upon µ ± -track reconstructions are analyzed and compared for the two samples. The differential cross sections for muon production angle, muon momentum, and four-momentum transfer Q 2 , are reported, and cross sections versus neutrino energy are obtained. Comparisons with predictions of current neutrino event generators are used to clarify the role of the ∆(1232) and higher-mass baryon resonances in CC pion production and to show the importance of pion final-state interactions. For the νµ-CC(π + ) (νµ-CC(π 0 )) sample, the absolute data rate is observed to lie below (above) the predictions of some of the event generators by amounts that are typically 1-to-2 σ. However the generators are able to reproduce the shapes of the differential cross sections for all kinematic variables of either data set.

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“…19 shows a summary of cross section measurements for ν μ P → μ − Δ ++ data on nuclear targets. Shown are the measurements of Gargamelle78 [44] (Propane), SKAT88 [45] (Freon), and SKAT89 [46] (Freon). The bottom panel shows measurements ofν μ N → μ + Δ − cross sections on nuclear targets from Gargamelle78 [47] (Propane) and SKAT89 [46] (Freon).…”

Section: Pion Production With W < 14 Gevmentioning

confidence: 99%

Methods to determine neutrino flux at low energies

et al. 2012

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We investigate the "low-ν" method (developed by the CCFR/NUTEV collaborations) to determine the neutrino flux in a wide band neutrino beam at very low energies, a region of interest to neutrino oscillations experiments. Events with low hadronic final state energy ν < ν cut (of 1, 2 and 5 GeV) were used by the MINOS collaboration to determine the neutrino flux in their measurements of neutrino (ν μ ) and antineutrino (ν μ ) total cross sections. The lowest ν μ energy for which the method was used in MINOS is 3.5 GeV, and the lowestν μ energy is 6 GeV. At these energies, the cross sections are dominated by inelastic processes. We investigate the application of the method to determine the neutrino flux for ν μ ,ν μ energies as low as 0.7 GeV where the cross sections are dominated by quasielastic scattering and Δ(1232) resonance production. We find that the method can be extended to low energies by using ν cut values of 0.25 and 0.50 GeV, which are feasible in fully active neutrino detectors such as MINERvA.

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Cross-section measurements of single pion production in charged current neutrino and antineutrino interactions

Cited by 32 publications

References 24 publications

Single pion production in neutrino reactions and estimates for charge-exchange effects

Single pion production in neutrino reactions and estimates for charge-exchange effects

Cross sections forνμandν¯μinduced pion production on hydrocarbon in the few-GeV region using MINERvA

Methods to determine neutrino flux at low energies

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