Angular distribution in electron-neutrino scattering and the anomalous magnetic moment of the neutrino

Barut, A. O.; Aydin, Z. Z.

doi:10.1007/bf02848090

Cited by 5 publications

(2 citation statements)

References 12 publications

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“…A full derivation of the cross section can be found in Greiner's textbook [61] on weak interactions. The scattering angle θ between the outgoing electron and the incoming neutrino is given by [100], since the Compton formula for scattering angle in final states holds [25].…”

Section: Neutrino Electron Elastic Scatteringmentioning

confidence: 99%

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Muon-Neutrino Electron Elastic Scattering and a Search for the Muon-Neutrino Magnetic Moment in the NOvA Near Detector

Wang

2017

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Section: Neutrino Electron Elastic Scatteringmentioning

confidence: 99%

“…Substitute Eq. 2.6 into dσ dT , the differential cross-section can then be approximately written in terms of θ as well [25] by…”

Section: Neutrino Electron Elastic Scatteringmentioning

confidence: 99%

Muon-Neutrino Electron Elastic Scattering and a Search for the Muon-Neutrino Magnetic Moment in the NOvA Near Detector

Wang

2017

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Reflection, transmission and spin rotation of dirac neutrinos in magnetic fields

Barut

Božić

1990

Z. Physik A - Atomic Nuclei

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Reflection and transmission coefficients of Dirac neutrinos with a magnetic moment through magnetic fields are calculated. The motion is in three dimensions. We find that one spin component can undergo a total reflection, but the other not, this effect being most pronounced at neutrino energies equal to the magnetic energy ~B. We also determine the spin rotation angle (equivalently the helicity rotation angle).

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A nonstandard model

Grandy

1993

Found Phys

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An elementary-particle picture developed primarily by Barut as an alternative to the standard model is re-examined. This model is formulated on the basis of strong short-range magnetic interactions among the stable particles (p, e , v) and at present is able to account qualitatively for most of the known phenomena.For more than three decades high-energy physicists have labored to assemble a wealth of data into a modern picture of elementary particles. The result, described principally in terms of quantum field theory (QFT), is a body of conventional wisdom generally referred to as the standard model. This development has not proceeded without reasoned disagreement, however, and a parallel body of other views exists, which have been less successful in reaching fruition. In particular, the work of Asim Barut and colleagues has aimed to construct a more transparent theory of particles that avoids their instantaneous appearance from, and disappearance into, the vacuum--and which abjures the introduction of new forces in a picture already unified by the electromagnetic field. Guided by a penchant for simplicity and a vision of "the way it ought to be", Barut has provided the skeletal structure for an alternative picture that actually turns out to have a measure of flesh on it. The time seems quite appropriate to gather together and review the essential features of these alternate views, due primarily to one who is very definitely a nonstandard model himself. THE S T A N D A R D M O D E LRegardless of what the future holds, the so-called standard model of particles and fields, consisting of the electroweak theory and quantum

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Angular distribution in electron-neutrino scattering and the anomalous magnetic moment of the neutrino

Cited by 5 publications

References 12 publications

Muon-Neutrino Electron Elastic Scattering and a Search for the Muon-Neutrino Magnetic Moment in the NOvA Near Detector

Muon-Neutrino Electron Elastic Scattering and a Search for the Muon-Neutrino Magnetic Moment in the NOvA Near Detector

Reflection, transmission and spin rotation of dirac neutrinos in magnetic fields

A nonstandard model

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