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Fermion dark matter from SO(10)
High Energy Physics - Phenomenology · Submitted 21 Sep 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We construct and analyze nonsupersymmetric SO(10) standard model extensions which explain dark matter (DM) through the fermionic Higgs portal.
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The abstract, sentence by sentence
We construct and analyze nonsupersymmetric SO(10) standard model extensions which explain dark matter (DM) through the fermionic Higgs portal. In these SO(10)-based models the DM particle is naturally stable since a $Z_2$ discrete symmetry, the matter parity, is left at the end of the symmetry breaking chain to the standard model. Potentially realistic models contain the $\bf{10}$ and $\bf{45}$ fermionic representations from which a neutralino-like mass matrix with arbitrary mixings can be obtained. Two different SO(10) breaking chains will be analyzed in light of gauge coupling unification: the standard path $\text{SU}(5)\times U(1)_{X}$ and the left-right symmetry intermediate chain. The former opens the possibility of a split supersymmetric-like spectrum with an additional (inert) scalar doublet, while the later requires additional exotic scalar representations associated to the breaking of the left-right symmetry.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We construct and analyze nonsupersymmetric SO(10) standard model extensions which explain dark matter (DM) through the fermionic Higgs portal. | contribution 1.00 | 0.94 | 0.40 | asserted 1.00 |
| s1 | In these SO(10)-based models the DM particle is naturally stable since a $Z_2$ discrete symmetry, the matter parity, is left at the end of the symmetry breaking chain to the standard model. | result 0.51 | 0.52 | 0.15 | asserted 0.99 |
| s2 | Potentially realistic models contain the $\bf{10}$ and $\bf{45}$ fermionic representations from which a neutralino-like mass matrix with arbitrary mixings can be obtained. | contribution 0.59 | 0.54 | 0.08 | hedged possibility 0.70 |
| s3 | Two different SO(10) breaking chains will be analyzed in light of gauge coupling unification: the standard path $\text{SU}(5)\times U(1)_{X}$ and the left-right symmetry intermediate chain. | method 0.64 | 0.76 | 0.05 | asserted 0.95 |
| s4 | The former opens the possibility of a split supersymmetric-like spectrum with an additional (inert) scalar doublet, while the later requires additional exotic scalar representations associated to the breaking of the left-right symmetry. | result 0.58 | 0.46 | 0.08 | asserted 0.57 |
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The paper
Original abstract
We construct and analyze nonsupersymmetric SO(10) standard model extensions which explain dark matter (DM) through the fermionic Higgs portal. In these SO(10)-based models the DM particle is naturally stable since a $Z_2$ discrete symmetry, the matter parity, is left at the end of the symmetry breaking chain to the standard model. Potentially realistic models contain the $\bf{10}$ and $\bf{45}$ fermionic representations from which a neutralino-like mass matrix with arbitrary mixings can be obtained. Two different SO(10) breaking chains will be analyzed in light of gauge coupling unification: the standard path $\text{SU}(5)\times U(1)_{X}$ and the left-right symmetry intermediate chain. The former opens the possibility of a split supersymmetric-like spectrum with an additional (inert) scalar doublet, while the later requires additional exotic scalar representations associated to the breaking of the left-right symmetry.
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References
How the literature uses it
17 arXiv papers cite this in 21 sentences
Papers citing it · 11 sentences without a confident label
Cites it as background 9 papers
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For the aforementioned reasons, we consider the doublet-triplet fermionic model (DTF) [ref] , which is one of the ultraviolet realizations of the fermionic Higgs portal [ref] , and is part of the minimal setup expected when the SM is extended by new physics which is, to some extent, related to lepton and baryon number conservation [ref] .
Phenomenology of doublet-triplet fermionic dark matter in nonstandard cosmology and multicomponent dark sectors · Introduction · 0.89
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Various proposals for $SO(10)$ DM candidates that are stabilized by the $2$ parity of gauge origin have been put forth in the recent literature: a dedicated analysis of scalar DM in the $$ was carried out in [ref] , while the possibility of fermionic DM in the $45$ was addressed in [ref] (see also [ref] where the $45$ is allowed to mix with a $$).
Dark Matter from the vector of SO(10) · Motivations and general considerations · 0.93
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Potentially realistic models containing the $SO(10)$ $10$ and $45$ fermionic representations, from which a neutralino-like mass matrix with arbitrary mixings can be obtained, was discussed in [ref] .
Fermionic triplet dark matter in an $SO(10)$-inspired left right model · Introduction · 0.96
What it cites · 73 sentences without a confident label
Builds on 5 papers
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In particular, we formulate $SO(10)$ realizations of the singlet-doublet fermion dark matter (SDFDM) model [ref] and the doublet-triplet fermion dark matter (DTFDM) model [ref] .
Dark matter and Higgs boson physics · Introduction · 0.82
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In particular, we formulate $SO(10)$ realizations of the singlet-doublet fermion dark matter (SDFDM) model [ref] and the doublet-triplet fermion dark matter (DTFDM) model [ref] .
LHC and Dark Matter Signals of Improved Naturalness · Introduction · 0.82
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In particular, we formulate $SO(10)$ realizations of the singlet-doublet fermion dark matter (SDFDM) model [ref] and the doublet-triplet fermion dark matter (DTFDM) model [ref] .
Doublet-Triplet Fermionic Dark Matter · Introduction · 0.82
Cites as support 4 papers
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The required colored octet has been shown in [ref] , to have an abundance and lifetime sufficiently small to satisfy all experimental constraints [ref] .
Dark matter stability and unification without supersymmetry · Partial split supersymmetry-like model · 0.98
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The required colored octet has been shown in [ref] , to have an abundance and lifetime sufficiently small to satisfy all experimental constraints [ref] .
Radiative Seesaw in SO(10) with Dark Matter · Partial split supersymmetry-like model · 0.98
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The required colored octet has been shown in [ref] , to have an abundance and lifetime sufficiently small to satisfy all experimental constraints [ref] .
Supersymmetric Unification Without Low Energy Supersymmetry And Signatures for Fine-Tuning at the LHC · Partial split supersymmetry-like model · 0.98
Cites as background 32 papers
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On the other hand, the phenomenology of the DTFDM has been studied in [ref] .
Discrimination of dark matter models in future experiments · Fermion DM from $SO(10)$ · 0.93
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On the other hand, the phenomenology of the DTFDM has been studied in [ref] .
Doublet-Triplet Fermionic Dark Matter · Fermion DM from $SO(10)$ · 0.93
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On the other hand, the phenomenology of the DTFDM has been studied in [ref] .
Integrating in the Higgs Portal to Fermion Dark Matter · Fermion DM from $SO(10)$ · 0.93
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