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Gauge Coupling Unification in E6 F-Theory GUTs with Matter and Bulk Exotics from Flux Breaking
High Energy Physics - Phenomenology · Submitted 17 Jul 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The combination of matter and bulk exotics in these cases can lead to precise gauge coupling unification which would not be possible with either type of exotics considered by themselves.
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The abstract, sentence by sentence
We consider gauge coupling unification in E6 F-Theory Grand Unified Theories (GUTs) where E6 is broken to the Standard Model (SM) gauge group using fluxes. In such models there are two types of exotics that can affect gauge coupling unification, namely matter exotics from the matter curves in the 27 dimensional representation of E6 and the bulk exotics from the adjoint 78 dimensional representation of E6. We explore the conditions required for either the complete or partial removal of bulk exotics from the low energy spectrum. In the latter case we shall show that (miraculously) gauge coupling unification may be possible even if there are bulk exotics at the TeV scale. Indeed in some cases it is necessary for bulk exotics to survive to the TeV scale in order to cancel the effects coming from other TeV scale matter exotics which would by themselves spoil gauge coupling unification. The combination of matter and bulk exotics in these cases can lead to precise gauge coupling unification which would not be possible with either type of exotics considered by themselves. The combination of matter and bulk exotics at the TeV scale represents a unique and striking signature of E6 F-theory GUTs that can be tested at the LHC.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider gauge coupling unification in E6 F-Theory Grand Unified Theories (GUTs) where E6 is broken to the Standard Model (SM) gauge group using fluxes. | contribution 0.59 | 0.40 | 0.04 | asserted 0.78 |
| s1 | In such models there are two types of exotics that can affect gauge coupling unification, namely matter exotics from the matter curves in the 27 dimensional representation of E6 and the bulk exotics from the adjoint 78 dimensional representation of E6. | background 0.99 | 0.10 | 0.03 | hedged possibility 0.51 |
| s2 | We explore the conditions required for either the complete or partial removal of bulk exotics from the low energy spectrum. | contribution 0.98 | 0.75 | 0.04 | asserted 0.60 |
| s3 | In the latter case we shall show that (miraculously) gauge coupling unification may be possible even if there are bulk exotics at the TeV scale. | result 0.96 | 0.76 | 0.27 | hedged possibility 0.99 |
| s4 | Indeed in some cases it is necessary for bulk exotics to survive to the TeV scale in order to cancel the effects coming from other TeV scale matter exotics which would by themselves spoil gauge coupling unification. | result 0.92 | 0.71 | 0.19 | asserted 0.91 |
| s5 | The combination of matter and bulk exotics in these cases can lead to precise gauge coupling unification which would not be possible with either type of exotics considered by themselves. | result 0.91 | 0.76 | 0.45 | asserted 0.57 |
| s6 | The combination of matter and bulk exotics at the TeV scale represents a unique and striking signature of E6 F-theory GUTs that can be tested at the LHC. | interpretation 0.94 | 0.32 | 0.30 | asserted 0.94 |
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The paper
Original abstract
We consider gauge coupling unification in E6 F-Theory Grand Unified Theories (GUTs) where E6 is broken to the Standard Model (SM) gauge group using fluxes. In such models there are two types of exotics that can affect gauge coupling unification, namely matter exotics from the matter curves in the 27 dimensional representation of E6 and the bulk exotics from the adjoint 78 dimensional representation of E6. We explore the conditions required for either the complete or partial removal of bulk exotics from the low energy spectrum. In the latter case we shall show that (miraculously) gauge coupling unification may be possible even if there are bulk exotics at the TeV scale. Indeed in some cases it is necessary for bulk exotics to survive to the TeV scale in order to cancel the effects coming from other TeV scale matter exotics which would by themselves spoil gauge coupling unification. The combination of matter and bulk exotics in these cases can lead to precise gauge coupling unification which would not be possible with either type of exotics considered by themselves. The combination of matter and bulk exotics at the TeV scale represents a unique and striking signature of E6 F-theory GUTs that can be tested at the LHC.
Human review
References
How the literature uses it
16 arXiv papers cite this in 27 sentences
Papers citing it · 13 sentences without a confident label
Uses its method or tool 2 papers
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The calculation below mostly follow [ref] .
Towards natural and realistic $E_7$ GUTs in F-theory · Mass scales and inert vector-like exotics · 0.97
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The calculation below mostly follow [ref] .
Applications of Flux Compactifications in F-Theory · Mass scales and inert vector-like exotics · 0.97
Cites it as background 10 papers
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The detailed derivation of the particular F-theory model we are interested in can be found in reference [ref] .
750 GeV Diphoton excess from $E_6$ in F-theory GUTs · The F-theory model with extra vector-like matter · 0.87
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The early literature, starting from [ref] , focused on the breaking of GUT groups of $(5)$ and its $(1)$ extensions [ref] , while there has also been some study of $(10)$ [ref] and $E_6$ [ref] GUTs.
Applications of Flux Compactifications in F-Theory · Review of previous work · 0.97
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In the context of F-theory, GUT groups $G=SU(5)$ (beginning with [ref] ), $(10)$ [ref] and $E_6$ [ref] have been studied in detail (see also the reviews [ref] for further references).
D-brane and F-theory Model Building · GUT Constructions: Georgi-Glashow GUTs · 0.93
What it cites · 16 sentences without a confident label
Builds on 1 paper
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In the presence of large VEVs for $X_5$ and $X_5$, the F and D flatness equations of [ref] must be modified accordingly.
E6 Models from F-theory · Low scale bulk exotics · 0.90
Uses the method or tool of 2 papers
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However, in [ref] a method has been pointed out for suppressing proton-decay in F-theory SU(5) with hypercharge flux breaking.
The Intermediate Scale MSSM, the Higgs Mass and F-theory Unification · Low scale bulk exotics · 0.86
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[ref] , and then integrating out X,Y.
Massive wavefunctions, proton decay and FCNCs in local F-theory GUTs · Low scale bulk exotics · 0.98
Uses data or values from 1 paper
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Here we make the same choices for the Ms and Ns as in [ref] and these choices are summarised in Table [ref].
Towards a Realistic F-theory GUT · Matter exotics only · 0.91
Compares with 1 paper
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The difference between this case and model 1 [ref] is that in model 1, $θ_34$ also gets a large VEV.
Towards a Realistic F-theory GUT · Matter exotics only · 0.88
Cites as support 1 paper
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It is argued in [ref] that the $U(1)_ψ$ and $U(1)_χ$ fluxes don't lead to any relative splittings of the gauge couplings at unification, although there could be a constant shift in all the couplings at each breaking.
E6 Models from F-theory · The effect of bulk exotics at a single mass scale $M_X$ · 0.96
Cites as background 2 papers
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In the previous section, we have reviewed the spectra of the models presented in [ref] and [ref] .
Towards a Realistic F-theory GUT · The complete spectra of potential models · 0.87
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In the previous section, we have reviewed the spectra of the models presented in [ref] and [ref] .
E6 Models from F-theory · The complete spectra of potential models · 0.87
Discussion
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