Study of electron-neutrino—electron elastic scattering at LAMPF

Allen, R. C.; Chen, H. H.; Doe, P. J.; Lee, W. P.; Lu, X. Q.; Mahler, H.J.; Potter, M.; Wang, K. C.; Bowles, T. J.; Burman, R. L.; Carlini, R.; Cochran, D. R. F.; Frank, J. S.; Piasetzky, E.; Sandberg, V.; Krakauer, D.; Talaga, R. L.

doi:10.1103/physrevd.47.11

Cited by 122 publications

(109 citation statements)

References 37 publications

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“…7(a)]. This technique is similar to those used in previous experiments [48][49][50][51][52] but the multiple beam configurations allow us to selectively enhance different regions of p z and p T .…”

Section: Study Of Muon Neutrino Disappearance Using mentioning

confidence: 99%

Study of muon neutrino disappearance using the Fermilab Main Injector neutrino beam

Adamson¹,

Andreopoulos²,

Arms³

et al. 2008

Phys. Rev. D

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174

153

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Section: Study Of Muon Neutrino Disappearance Using mentioning

confidence: 99%

Study of muon neutrino disappearance using the Fermilab Main Injector neutrino beam

Adamson¹,

Andreopoulos²,

Arms³

et al. 2008

Phys. Rev. D

Self Cite

174

153

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show abstract

“…This uncertainty can be reduced by using the Near Detector (ND) data to constrain the calculated flux. Several previous experiments used their neutrino data to constrain the yield of hadrons off the target [82,83,84,85], but the variable beam design of NuMI allows this to be accomplished with fewer assumptions, eg. about neutrino interaction cross sections.…”

Section: Constraint On Flux Uncertainties Using Near Detector Datamentioning

confidence: 99%

Observation of Disappearance of Muon Neutrinos in the NuMI Beam

Pavlović¹

2008

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“…The present laboratory limits for the electron neutrino are −5.5 × 10 −32 ≤ r 2 A (ν e ) ≤ 9.8 × 10 −32 cm 2 [21] 5 . In the Dirac case these limits apply to the sum r 2 V + r 2 A as well.…”

Section: Introductionmentioning

confidence: 64%

“…For r 2 A (ν e ) we could not find new experimental results that would imply better constraints than the existing ones [21]. We just mention that the Bugey nuclear reactor data from the detector module closest to the neutrino source (15 meters) [26] should imply independent limits of the same order of magnitude than the existing ones.…”

Section: Introductionmentioning

confidence: 83%

On the Neutrino Vector and Axial Vector Charge Radius

Nardi¹

2003

AIP Conference Proceedings

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Abstract.A Majorana neutrino is characterized by just one flavor diagonal electromagnetic form factor: the anapole moment, that in the static limit corresponds to the axial vector charge radius r 2 A . As is the case for the vector charge radius of a Dirac neutrino, proving that this quantity is a well defined physical quantity is non trivial. I will first describe briefly the origin of the long standing controversy about the physical or non physical nature of the neutrino charge radius. Then I will argue that, in contrast to Dirac neutrino electromagnetic form factors, for Majorana neutrinos cosmological and astrophysical arguments do not provide useful informations on r 2 A . Therefore this quantity has to be studied by means of terrestrial experiment. Finally, I will discuss the constraints that can be derived on r 2 A for the tau neutrino from a comprehensive analysis of the data on single photon production off Z-resonance, and I will conclude with a few comments on ν µ scattering data from the NuTeV, E734, CCFR and CHARM-II collaborations and on the limits implied for r 2 A for the muon neutrino.

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Study of electron-neutrino—electron elastic scattering at LAMPF

Cited by 122 publications

References 37 publications

Study of muon neutrino disappearance using the Fermilab Main Injector neutrino beam

Study of muon neutrino disappearance using the Fermilab Main Injector neutrino beam

Observation of Disappearance of Muon Neutrinos in the NuMI Beam

On the Neutrino Vector and Axial Vector Charge Radius

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