Abstract

Studies of neutrino mixing and oscillations, solar neutrinos as background in dark matter searches involving electron detection, detection of sterile neutrino warm dark matter, and of possible electromagnetic properties of neutrinos, have generated interest in the low energy O(10 keV) scattering of electron neutrinos and antineutrinos by atomic electrons where the binding of the atomic electron cannot be ignored. Of particular interest is the ionization of atoms by neutrinos and antineutrinos. Most existing calculations are based on modifications of the free electron differential cross section, which destroy the relationship between the neutrino helicities and the orbital and spin angular momenta of the atomic electrons. The present calculations maintain the full collision dynamics by formulating the scattering in configuration space using the Bound Interaction Picture, rather than the usual formulation in the Interaction Picture in momentum space as appropriate to scattering by free electrons. Energy spectra of ionization electrons produced by scattering of neutrinos and antineutrinos with energies of 5, 10, 20, and 30 keV by hydrogen, helium and neon have been calculated using Dirac central field eigenfunctions and are presented as ratios to the spectra for scattering by free electrons. Binding effects increase strongly with atomic number, are largest for low neutrino energy and, for each neutrino energy, greatest at the high electron energy end of the spectrum. The most extreme effects of binding are for 5 keV scattering by Ne where the ratios are less than 0.1. The energy spectra are calculated for both a Coulombic final electron state and a free final electron state. The results indicate that the binding effects from the continuum state of the final electron are significant and can be comparable to those arising from the bound initial electron state.

Highlights

  • Studies of neutrino mixing and oscillations [1], solar neutrinos as background in dark matter searches involving electron detection [2], detection of sterile neutrino warm dark matter [3], and of possible electromagnetic properties of neutrinos, such as magnetic and electric dipole moments, using low energy elastic scattering of neutrinos and antineutrinos [4,5], have generated interest in the low energy O(10 keV) scattering of electron neutrinos and antineutrinos by atomic electrons νeðνeÞ þ e− → νeðνeÞ þ e−: ð1ÞThe standard scattering is due to the weak interaction and involves both W-boson charged current and Z-boson neutral current exchange

  • The weak and electromagnetic scatterings are incoherent and their dependences upon the energy transferred T 1⁄4 Eνi − Eνf to the atomic electron for T ≪ Eνi are quite different, with their differential cross sections dσ=dT being approximately constant for the standard scattering and ∝ 1=T for the electromagnetic scattering

  • Neutrino-atom collisions has been reviewed by Kouzakov and Studenikin [6]

Read more

Summary

INTRODUCTION

Studies of neutrino mixing and oscillations [1], solar neutrinos as background in dark matter searches involving electron detection [2], detection of sterile neutrino warm dark matter [3], and of possible electromagnetic properties of neutrinos, such as magnetic and electric dipole moments, using low energy elastic scattering of neutrinos and antineutrinos [4,5], have generated interest in the low energy O(10 keV) scattering of electron neutrinos and antineutrinos by atomic electrons νeðνeÞ þ e− → νeðνeÞ þ e−: ð1Þ. For all these low energy studies the binding of the atomic electron cannot be ignored and one can expect modifications of the free electron scattering formulas. Neutrino-atom collisions has been reviewed by Kouzakov and Studenikin [6] In this present study we consider only the scattering by the standard weak interaction. Details of the derivation of the S-matrix in the Bound Interaction Picture are given in Appendix A, explicit expressions for the electron scattering tensors in Appendix B, and computational details for the evaluation of the radial matrix elements in Appendix C

S-matrix for scattering by bound electrons
Cross section
Atomic electron amplitude
RADIAL MATRIX ELEMENTS
EVALUATION OF CROSS SECTIONS
RESULTS AND DISCUSSION
SUMMARY AND CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call