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On hypercharge flux and exotics in F-theory GUTs
High Energy Physics - Phenomenology · Submitted 8 Jul 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If we impose an additional R-parity symmetry by hand we find all the exotics can be lifted while proton decay operators are still forbidden.
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The abstract, sentence by sentence
We study SU(5) Grand Unified Theories within a local framework in F-theory with multiple extra U(1) symmetries arising from a small monodromy group. The use of hypercharge flux for doublet-triplet splitting implies massless exotics in the spectrum that are protected from obtaining a mass by the U(1) symmetries. We find that lifting the exotics by giving vacuum expectation values to some GUT singlets spontaneously breaks all the U(1) symmetries which implies that proton decay operators are induced. If we impose an additional R-parity symmetry by hand we find all the exotics can be lifted while proton decay operators are still forbidden. These models can retain the gauge coupling unification accuracy of the MSSM at 1-loop. For models where the generations are distributed across multiple curves we also present a motivation for the quark-lepton mass splittings at the GUT scale based on a Froggatt-Nielsen approach to flavour.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study SU(5) Grand Unified Theories within a local framework in F-theory with multiple extra U(1) symmetries arising from a small monodromy group. | contribution 0.93 | 0.83 | 0.04 | asserted 0.98 |
| s1 | The use of hypercharge flux for doublet-triplet splitting implies massless exotics in the spectrum that are protected from obtaining a mass by the U(1) symmetries. | background 0.55 | 0.17 | 0.10 | asserted 0.99 |
| s2 | We find that lifting the exotics by giving vacuum expectation values to some GUT singlets spontaneously breaks all the U(1) symmetries which implies that proton decay operators are induced. | result 0.91 | 0.93 | 0.23 | asserted 1.00 |
| s3 | If we impose an additional R-parity symmetry by hand we find all the exotics can be lifted while proton decay operators are still forbidden. | result 0.93 | 0.93 | 0.30 | asserted 0.99 |
| s4 | These models can retain the gauge coupling unification accuracy of the MSSM at 1-loop. | result 1.00 | 0.78 | 0.09 | hedged possibility 0.52 |
| s5 | For models where the generations are distributed across multiple curves we also present a motivation for the quark-lepton mass splittings at the GUT scale based on a Froggatt-Nielsen approach to flavour. | contribution 0.80 | 0.83 | 0.05 | asserted 0.73 |
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The paper
Original abstract
We study SU(5) Grand Unified Theories within a local framework in F-theory with multiple extra U(1) symmetries arising from a small monodromy group. The use of hypercharge flux for doublet-triplet splitting implies massless exotics in the spectrum that are protected from obtaining a mass by the U(1) symmetries. We find that lifting the exotics by giving vacuum expectation values to some GUT singlets spontaneously breaks all the U(1) symmetries which implies that proton decay operators are induced. If we impose an additional R-parity symmetry by hand we find all the exotics can be lifted while proton decay operators are still forbidden. These models can retain the gauge coupling unification accuracy of the MSSM at 1-loop. For models where the generations are distributed across multiple curves we also present a motivation for the quark-lepton mass splittings at the GUT scale based on a Froggatt-Nielsen approach to flavour.
Human review
References
How later papers used it
59 later papers cite it
3 later papers by other authors are listed below: 3 used its method or tool. 1 more paper by the same authors is listed: 1 used its method or tool.
Uses its method or tool 4 of 5 papers with this label · 1 by the same authors
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Followed this paper to derive the relations of b_k(a_i) by equating coefficients of the same powers in s, using a suitable Ansatz for the a_i's to solve the constraint b_1(a_i)=0.
Building SO(10) models from F-theory (2012) · 0.87 · paraphrased: the licence does not allow quoting
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Determined homologies from the known Chern classes of the b_k coefficients through the equations b_k=b_k(a_i) given in this paper, using well known procedures.
Phenomenological implications of a minimal F-theory GUT with discrete symmetry (2015) · 0.87 · paraphrased: the licence does not allow quoting
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Made this paper's Ansatz and substituted it into the b_n's.
Aspects of F-Theory GUTs (2012) · 0.85 · paraphrased: the licence does not allow quoting
By the same authors
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Followed precisely this paper's methodology and notation to start from a fully split spectral cover.
Wavefunctions and the Point of E8 in F-theory (2012) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
How the literature uses it
60 arXiv papers cite this in 129 sentences
Papers citing it · 90 sentences without a confident label
Builds on it 2 papers
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As already stated, if no other conditions are imposed on $a_k$ this model is considered as an $S_3$ variant of the $3+1+1$ example given in [ref] .
Discrete Family Symmetry from F-Theory GUTs · $S_3$ and $Z_3$ models for $(3,1,1)$ factorisation · 0.81
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Remarkably, this model is the $SO(10)$ upgrade of the $3+1+1+1$ example given in [ref] .
Building SO(10) models from F-theory · First example · 0.91
Uses its method or tool 5 papers
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Following precisely the methodology and notation of [ref] we start from a fully split spectral cover C_10 = (a_1 V + a_6 U ) (a_2 V + a_7 U ) (a_3 V + a_8 U) (a_4 V + a_9 U) (a_5 V + a_10 U) = 0 .
Wavefunctions and the Point of E8 in F-theory · Semi-local constraints on matter spectrum · 1.00
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Using the method of [ref] , the possible abelian monodromies are $ℤ_2$, $ℤ_3$, $ℤ_4,$ $ℤ_2×ℤ_3$ and $ℤ_2×ℤ_2$; they lead to factorizations of the $𝒞_5$ spectral cover as [equation] and to the respective identification of the weights ${ t_1,t_2}$, ${ t_1,t_2,t_3}$, ${ t_1,t_2,t_3,t_4}$, ${ t_1,t_2} ∪{ t_3,t_4,t_5}$ and ${ t_1,t_2} ∪{ t_3,t_4}$.The algebraic equations for the matter curves $Σ_t_i$, $Σ_t_i+t_j$, $Σ_t_i-t_j$ in terms of the $t_i$ weights associated with the $SU_5^⊥$ fundamental representation are respectively given by $t_i=0$; $( t_i+t_j) _i<j=0$ and $±( t_i-t_j) _i<j=0$; they are denoted like $10_t_i,$ $5̅_t_i+t_j$ and $1_±( t_i-t_j)$; see eq(<ref>).
MSSM-like from $SU_{5}\times D_{4}$ Models · Abelian monodromy · 0.91
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These are readily determined from the known Chern classes of the $b_k$ coefficients through the equations $b_k=b_k(a_i)$ given in ([ref]), using well known procedures [ref] .
Phenomenological implications of a minimal F-theory GUT with discrete symmetry · The discrete group $D_4$ as a Family Symmetry · 0.87
Uses its data or values 1 paper
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The third column shows the homology classes of the matter curves computed in [ref] .
Neutrino mass textures from F-theory · $SU(5)$ spectrum · 0.80
Compares with it 5 papers
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Unlike the constraints ([ref]) and ([ref]), the constraint ([ref]) does not come out from the type of local geometry or spectral cover analysis presented in [ref] for example.
A Note on Hypercharge Flux, Anomalies, and U(1)s in F-theory GUTs · GUT Anomalies and the Local Geometry · 0.81
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Notice that the latter does not coincide with the parity chosen in [ref] .
Building SO(10) models from F-theory · A $Z_2$ matter parity for a model with $2+3$ spectral cover split · 0.94
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This is in contrast to the example given in [ref] .
Yukawa couplings and fermion mass structure in F-theory GUTs · A simple model for doublet-triplet splitting · 0.99
Cites it as background 21 papers
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To start with, we recall here the basic features of the model [ref] which emerges from the general class [ref] presented in Table [ref].
Unification, KK-thresholds and the top Yukawa coupling in F-theory GUTs · Application to a realistic minimal model · 0.83
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To set the stage, we first present a short review of the basic characteristics of the model following mainly the notation of [ref] .
MSSM from F-theory SU(5) with Klein Monodromy · Analysis of the $Z_2×Z_2$ model · 0.91
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This phenomenon was discovered in [ref] in IIB string theory (see also [ref] ), and was propagated to F-theory in [ref] (see [ref] for a review).
Hypercharge flux in F-theory and the stable Sen limit · Introduction · 0.90
What it cites · 72 sentences without a confident label
Uses data or values from 2 papers
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The highest mass we can give the exotics is around $2×10^14$GEV since $ϵ_1ϵ_2 ∼10^-2$ from the quark masses [ref] .
Froggatt-Nielsen models from E8 in F-theory GUTs · 3-curve models · 0.83
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The dimension 4 operator is constrained for any generation indices to be $λ_ijk<10^-5$ [ref] .
Upper bound on all products of R-parity violating couplings $\lambda'$ and $\lambda''$ from proton decay · Constraints on proton decay operators · 0.81
Compares with 1 paper
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In this sense it is on a similar footing to the single $U(1)$ model of [ref] .
Compact F-theory GUTs with U(1)_PQ · 3-curve models · 0.96
Cites as support 2 papers
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As shown in [ref] 3-curve models can recreate realistic quark and lepton mixing at the GUT level.
Froggatt-Nielsen models from E8 in F-theory GUTs · Froggatt-Nielsen and quark-lepton mass splitting · 0.96
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The second is that it is possible to realise the idea that each MSSM generation comes from a different matter curve which as shown in [ref] can lead to attractive models of flavour.
Family symmetries in F-theory GUTs · Introduction · 0.98
Cites as background 27 papers
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Recently string GUT constructions have been developed in the context of F-theory [ref] (see [ref] for a phenomenological review).
Particle Physics Implications of F-theory · Introduction · 1.00
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Recently string GUT constructions have been developed in the context of F-theory [ref] (see [ref] for a phenomenological review).
Model Building with F-Theory · Introduction · 1.00
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Recently string GUT constructions have been developed in the context of F-theory [ref] (see [ref] for a phenomenological review).
Breaking GUT Groups in F-Theory · Introduction · 1.00
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