# Higgs Parity, Strong CP, and Dark Matter

**Authors:** David Dunsky, Lawrence J. Hall, Keisuke Harigaya

arXiv: 1902.07726 · 2019-07-12

## TL;DR

This paper proposes a model where Higgs Parity explains the Standard Model, solves the strong CP problem, and predicts mirror electron dark matter, with testable implications for future experiments and measurements.

## Contribution

It introduces a Higgs Parity framework that unifies electroweak symmetry breaking, addresses the strong CP problem, and predicts mirror electron dark matter with specific detection signatures.

## Key findings

- Higgs Parity leads to a vanishing quartic coupling at scale v'
- Mirror electrons are viable dark matter candidates stabilized by mirror electromagnetism
- Future measurements of fundamental parameters will test the model's predictions

## Abstract

An exact spacetime parity replicates the $SU(2) \times U(1)$ electroweak interaction, the Higgs boson $H$, and the matter of the Standard Model. This "Higgs Parity" and the mirror electroweak symmetry are spontaneously broken at scale $v' = \left\langle{H'} \right\rangle \gg \left\langle{H}\right\rangle$, yielding the Standard Model below $v'$ with a quartic coupling that essentially vanishes at $v'$: $\lambda_{SM}(v') \sim 10^{-3}$. The strong CP problem is solved as Higgs parity forces the masses of mirror quarks and ordinary quarks to have opposite phases. Dark matter is composed of mirror electrons, $e'$, stabilized by unbroken mirror electromagnetism. These interact with Standard Model particles via kinetic mixing between the photon and the mirror photon, which arises at four-loop level and is a firm prediction of the theory. Physics below $v'$, including the mass and interaction of $e'$ dark matter, is described by $\textit{one fewer parameter}$ than in the Standard Model. The allowed range of $m_{e'}$ is determined by uncertainties in $(\alpha_s, m_t, m_h)$, so that future precision measurements of these will be correlated with the direct detection rate of $e'$ dark matter, which, together with the neutron electric dipole moment, will probe the entire parameter space.

## Full text

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## Figures

7 figures with captions in the complete paper: https://tomesphere.com/paper/1902.07726/full.md

## References

87 references — full list in the complete paper: https://tomesphere.com/paper/1902.07726/full.md

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Source: https://tomesphere.com/paper/1902.07726