SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter
We propose a grand unified SU(5)×U(1)X model, where the standard SU(5) grand unified theory is supplemented by minimal seesaw and a right-handed neutrino dark matter with an introduction of a global Z2-parity. In the presence of three right-handed neutrinos (RHNs), the model is free from all gauge a...
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doaj-45b26cbbc11442749a3747fb680db1fd2020-11-24T22:47:35ZengElsevierPhysics Letters B0370-26932018-05-01780422426SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matterNobuchika Okada0Satomi Okada1Digesh Raut2Department of Physics and Astronomy, University of Alabama, Tuscaloosa, AL 35487, USAGraduate School of Science and Engineering, Yamagata University, Yamagata 990-8560, JapanDepartment of Physics and Astronomy, University of Alabama, Tuscaloosa, AL 35487, USA; Corresponding author.We propose a grand unified SU(5)×U(1)X model, where the standard SU(5) grand unified theory is supplemented by minimal seesaw and a right-handed neutrino dark matter with an introduction of a global Z2-parity. In the presence of three right-handed neutrinos (RHNs), the model is free from all gauge and mixed-gravitational anomalies. The SU(5) symmetry is broken into the Standard Model (SM) gauge group at MGUT≃4×1016GeV in the standard manner, while the U(1)X symmetry breaking occurs at the TeV scale, which generates the TeV-scale mass of the U(1)X gauge boson (Z′ boson) and the three Majorana RHNs. A unique Z2-odd RHN is stable and serves as the dark matter (DM) in the present Universe, while the remaining two RHNs work to generate the SM neutrino masses through the minimal seesaw. We investigate the Z′-portal RHN DM scenario in this model context. We find that the constraints from the DM relic abundance, and the Z′ boson search at the Large Hadron Collider (LHC), and the perturbativity bound on the U(1)X gauge coupling are complementary to narrow down the allowed parameter region in the range of 3.0≤mZ′[TeV]≤9.2 for the Z′ boson mass. The allowed region for mZ′≤5TeV will be fully covered by the future LHC experiments. We also briefly discuss the successful implementation of Baryogenesis and cosmological inflation scenarios in the present model.http://www.sciencedirect.com/science/article/pii/S037026931830220X |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Nobuchika Okada Satomi Okada Digesh Raut |
spellingShingle |
Nobuchika Okada Satomi Okada Digesh Raut SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter Physics Letters B |
author_facet |
Nobuchika Okada Satomi Okada Digesh Raut |
author_sort |
Nobuchika Okada |
title |
SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter |
title_short |
SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter |
title_full |
SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter |
title_fullStr |
SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter |
title_full_unstemmed |
SU(5)×U(1)X grand unification with minimal seesaw and Z′-portal dark matter |
title_sort |
su(5)×u(1)x grand unification with minimal seesaw and z′-portal dark matter |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 |
publishDate |
2018-05-01 |
description |
We propose a grand unified SU(5)×U(1)X model, where the standard SU(5) grand unified theory is supplemented by minimal seesaw and a right-handed neutrino dark matter with an introduction of a global Z2-parity. In the presence of three right-handed neutrinos (RHNs), the model is free from all gauge and mixed-gravitational anomalies. The SU(5) symmetry is broken into the Standard Model (SM) gauge group at MGUT≃4×1016GeV in the standard manner, while the U(1)X symmetry breaking occurs at the TeV scale, which generates the TeV-scale mass of the U(1)X gauge boson (Z′ boson) and the three Majorana RHNs. A unique Z2-odd RHN is stable and serves as the dark matter (DM) in the present Universe, while the remaining two RHNs work to generate the SM neutrino masses through the minimal seesaw. We investigate the Z′-portal RHN DM scenario in this model context. We find that the constraints from the DM relic abundance, and the Z′ boson search at the Large Hadron Collider (LHC), and the perturbativity bound on the U(1)X gauge coupling are complementary to narrow down the allowed parameter region in the range of 3.0≤mZ′[TeV]≤9.2 for the Z′ boson mass. The allowed region for mZ′≤5TeV will be fully covered by the future LHC experiments. We also briefly discuss the successful implementation of Baryogenesis and cosmological inflation scenarios in the present model. |
url |
http://www.sciencedirect.com/science/article/pii/S037026931830220X |
work_keys_str_mv |
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