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Barish, S.J.; Campbell, John Henry; Charlton, G.; Cho, Y.; Derrick, M.; Engelmann, R.; Hyman, L.; Jankowski, D.J.; Mann, A. K.; Musgrave, B.; Schreiner, P.; Schultz, P. F.; Singer, R.; Szczekowski, M.; Wangler, T.P.; Yuta, H.; Barnes, V. E.; Carmony, D.D.; Garfinkel, A. F.; Radecky, G.M.

doi:10.1103/physrevd.16.3103

Cited by 156 publications

(181 citation statements)

References 41 publications

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“…Incoming neutrino energy distributions can be found in Figure 8 of Ref. [37] and in Figure 7 of Ref. [38] for the ANL and BNL experiments, respectively 13 .…”

Section: A CC Pion Production Cross Sectionsmentioning

confidence: 99%

Weak pion production off the nucleon

2007

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We develop a model for the weak pion production off the nucleon, which besides the Delta pole mechanism (weak excitation of the ∆(1232) resonance and its subsequent decay into N π), includes also some background terms required by chiral symmetry. We re-fit the C A 5 (q 2 ) form factor to the flux averaged νµp → µ − pπ + ANL q 2 −differential cross section data, finding a substantially smaller contribution of the Delta pole mechanism than traditionally assumed in the literature. Within this scheme, we calculate several differential and integrated cross sections, including pion angular distributions, induced by neutrinos and antineutrinos and driven both by charged and neutral currents. In all cases we find that the background terms produce quite significant effects and that they lead to an overall improved description of the data, as compared to the case where only the Delta pole mechanism is considered. We also show that the interference between the Delta pole and the background terms produces parity-violating contributions to the pion angular differential cross section, which are intimately linked to T −odd correlations in the contraction between the leptonic and hadronic tensors. However, these latter correlations do not imply a genuine violation of time reversal invariance because of the existence of strong final state interaction effects.

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“…Incoming neutrino energy distributions can be found in Figure 8 of Ref. [37] and in Figure 7 of Ref. [38] for the ANL and BNL experiments, respectively 13 .…”

Section: A CC Pion Production Cross Sectionsmentioning

confidence: 99%

Weak pion production off the nucleon

2007

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“…The first category, quasi-elastic (QE) CC events, is the primary source of untagged Michel electrons and originates from neutrinos in the energy range 150 Y250 MeV. The uncertainty on the cross section in this energy region is 25% (Barish et al 1977). These Michel electrons comprise 80% of the DSNB background.…”

Section: Backgroundsmentioning

confidence: 99%

A Search for Neutrinos from the SolarhepReaction and the Diffuse Supernova Neutrino Background with the Sudbury Neutrino Observatory

Aharmim

Ahmed

Anthony

et al. 2006

ApJ

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A search has been made for neutrinos from the hep reaction in the Sun and from the diffuse supernova neutrino background ( DSNB) using data collected during the first operational phase of the Sudbury Neutrino Observatory, with an exposure of 0.65 ktons yr. For the hep neutrino search, two events are observed in the effective electron energy range of 14:3 MeV < T eA < 20 MeV, where 3.1 background events are expected. After accounting for neutrino oscillations, an upper limit of 2:3 ; 10 4 cm À2 s À1 at the 90% confidence level is inferred on the integral total flux of hep neutrinos. For DSNB neutrinos, no events are observed in the effective electron energy range of 21 MeV < T eA < 35 MeV, and, consequently, an upper limit on the e component of the DSNB flux in the neutrino energy range of 22:9 MeV < E < 36:9 MeVof 70 cm À2 s À1 is inferred at the 90% confidence level. This is an improvement by a factor of 6.5 on the previous best upper limit on the hep neutrino flux and by 2 orders of magnitude on the previous upper limit on the e component of the DSNB flux.

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“…The dashed, dot and dash-dotted lines show the calculated quasi-elastic, single-meson and deep-inelastic scatterings, respectively. The data points are taken from the following experiments: ( )ANL [54], ( )GGM77 [55], (•)GGM79(a) [56],(b) [57], ( * )Serpukhov [58], (♦)ANL82 [59], ( )BNL86 [60], ( )CCFR90 [61], ( )CDHSW87 [62], (×)IHEP-JINR96 [63], (+)IHEP-ITEP79 [64], ( )CCFRR84 [65], and ( )BNL82 [53].…”

Section: Benefits To the Measurements Of Exclusive Channelsmentioning

confidence: 99%

A Measurement of Neutrino Charged Current Interactions and a Search for Muon Neutrino Disappearance with the Fermilab Booster Neutrino Beam

Nakajima

2011

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In this thesis, we report on a measurement of muon neutrino inclusive charged current interactions on carbon in the few GeV region, using the Fermilab Booster Neutrino Beam. The all neutrino mode data collected in the SciBooNE experiment is used for this analysis.We collected high-statistics CC interaction sample at SciBooNE, and extracted energy dependent inclusive charged current interaction rates and cross sections for a wide energy range from 0.25 GeV to ∼3 GeV. We measure the interaction rates with 6-15% precision, and the cross sections with 10-30% precision. We also made an energy integrated measurements, with the precisions of 3% for the rate, and 8% for the cross section measurements. This is the first measurement of the CC inclusive cross section on carbon around 1 GeV.This inclusive interaction measurement is nearly free from effects of hadron re-interactions in the nucleus. Hence, it is complementary to other exclusive cross section measurements, and essential to understand the neutrino interaction cross sections in the few GeV region, which is relevant to ongoing and future neutrino oscillation experiments. This analysis also provides the normalization for SciBooNE's previous cross section ratio measurements for charged current coherent pion production and neutral current neutral pion production. Then, a precise comparison between our previous measurements and the model predictions becomes possible.The result of the interaction rate measurement is used to constrain the product of the neutrino flux and the cross section at the other experiment on the Fermilab Booster Neutrino Beam: MiniBooNE. We conducted a search for short-baseline muon neutrino disappearance using data both from SciBooNE and MiniBooNE, to test a possible neutrino oscillation with sterile neutrinos which is suggested by the LSND experiment. With this constraint by SciBooNE, we significantly reduced the flux and the cross section uncertainties at MiniBooNE, and achieved the world best sensitivity for the ν µ disappearance at 0.5 < ∆m 2 < 30 (eV 2 ). We found no significant oscillation signal, and set one of the world strongest limits for the sterile neutrino models.ii

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Study of neutrino interactions in hydrogen and deuterium: Description of the experiment and study of the reactionν+d→μ−+p+ps

Cited by 156 publications

References 41 publications

Weak pion production off the nucleon

Weak pion production off the nucleon

A Search for Neutrinos from the SolarhepReaction and the Diffuse Supernova Neutrino Background with the Sudbury Neutrino Observatory

A Measurement of Neutrino Charged Current Interactions and a Search for Muon Neutrino Disappearance with the Fermilab Booster Neutrino Beam

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