Abstract

In a recent Letter we presented a systematic way of testing the seesaw origin of neutrino mass in the context of the Minimal Left-Right Symmetric Model. The essence of the program is to exploit lepton number violating decays of doubly charged scalars, particles which lie at the heart of the Higgs-mechanism-based seesaw, to probe the Dirac neutrino mass term which in turn enters directly into a number of physical processes including the decays of right-handed neutrinos into the $W$ boson and left-handed charged leptons. In this longer version we discuss at length these and related processes, and offer some missing technical details. We also carefully analyze the physically appealing possibility of parity conserving Yukawa sector showing that the neutrino Dirac mass matrix can be analytically expressed as a function of light and heavy neutrino masses and mixing, without resorting to any additional discrete symmetries, a context in which the seesaw mechanism can be disentangled completely.When parity does get broken, we show that, in the general case, only the Hermitian part of the Dirac mass term is independent which substantially simplifies the task of testing experimentally the origin of neutrino mass. We illustrate this program through some physical examples that allow simple analytical expressions. Our work shows that the Minimal Left-Right Symmetric Model is a self-contained theory of neutrino mass which can be in principle tested at the LHC or the next hadron collider.

Highlights

  • Understanding the origin of neutrino mass is a central task of the physics beyond the Standard Model

  • The seesaw mechanism has emerged as the main scenario behind the smallness of neutrino mass, but by itself falls short of providing a fullfledged theory

  • The SM seesaw cannot be disentangled, and the heavy RH neutrinos can be produced at the hadron colliders, such as the LHC, only through the Dirac mass terms

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Summary

INTRODUCTION

We have shown how to determine MD in the Hermitian case (unbroken parity in the Dirac Yukawa sector), which in a simple case of the socalled type I seesaw and same left and right leptonic mixing matrices takes the following unique form [9]: MD 1⁄4 iVLpffimffiffiffiνffiffimffiffiffiffiNffiffiV†L: ð6Þ This expression manifestly demonstrates the predictivity of the theory—all ambiguities are gone from the Dirac neutrino mass matrix. It is useful to rewrite the Yukawa interaction of the bidoublet Φ as the function of the physical fields h and H and the charged lepton and neutrino Dirac mass matrices: LΦ

H NR l L
LEPTON MASSES
The tale of unbroken parity
Broken parity
PHENOMENOLOGICAL IMPLICATIONS
Decays and the probe of MD
The limits on particle masses
SUMMARY AND OUTLOOK
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