Abstract

In the framework of a baryon-number-violating effective Lagrangian, we calculate improved lower bounds on partial lifetimes for proton and bound neutron decays, including $p \to \ell^+ \ell'^+ \ell'^-$, $n \to \bar\nu \ell^+ \ell'^-$, $p \to \ell^+ \nu\bar\nu$, and $n \to \bar\nu \bar\nu \nu$, where $\ell$ and $\ell'$ denote $e$ or $\mu$, with both $\ell = \ell'$ and $\ell \ne \ell'$ cases. Our lower bounds are substantially stronger than the corresponding lower bounds from direct experimental searches. We also present lower bounds on $(\tau/B)_{p \to \ell^+\gamma}$, $(\tau/B)_{n \to \bar\nu \gamma}$, $(\tau/B)_{p \to \ell^+ \gamma\gamma}$, and $(\tau/B)_{n \to \bar\nu \gamma\gamma}$. Our method relies on relating the rates for these decay modes to the rates for decay modes of the form $p \to \ell^+ M$ and $n \to \bar\nu M$, where $M$ is a pseudoscalar or vector meson, and then using the experimental lower bounds on the partial lifetimes for these latter decays.

Highlights

  • The Standard Model (SM) conserves baryon number1 B, this is violated in many of its ultraviolet extensions

  • Our method can be applied to other nucleon decay modes, such as p → lþγγ and n → νγγ, where here the γγ part of the final state are “continuum” photons, i.e., not photons that arise from a cascade decay such as p → lþπ0 followed by π0 → γγ or p → lþη followed by η → γγ

  • If nucleon decays were to be observed with lower partial lifetimes than the bounds derived here, this would be of interest as evidence of baryon-number violation, and as evidence of BNV mass scales lower than the grand unified theories (GUTs)-type scales assumed in the minimal framework used here

Read more

Summary

INTRODUCTION

The Standard Model (SM) conserves baryon number B, this is violated in many of its ultraviolet extensions. A number of dedicated experiments have been carried out since the early 1980s to search for proton decay and the decay of neutrons bound in nuclei. These experiments have obtained null results and have set resultant stringent upper limits for the rates of nucleon decays.. Within the framework of a baryon-numberviolating effective Lagrangian, Leff, we shall calculate improved lower bounds on partial lifetimes for a number of nucleon decays. Our method is to derive an approximate relation between the rate ΓN→f:s: for the decay of a nucleon to a final state f.s., N → f:s: (where N 1⁄4 p or n) and the rate for the decay ΓN→f:s:0 to a different final state, denoted f:s:0. IX and some relevant phase-space formulas are given in the Appendix

EFFECTIVE LAGRANGIAN
THE DECAYS p → l + γ AND n → νγ
VIII. OTHER DECAY MODES
CONCLUSIONS

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

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.