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R-Parity Conservation from a Top Down Perspective
High Energy Physics - Phenomenology · Submitted 19 Mar 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim An experimental observation of R-parity violation would, therefore, disfavor such classes of top-down GUT models.
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The abstract, sentence by sentence
Motivated by results from the LHC and dark matter searches, we study the possibility of phenomenologically viable R-parity violation in $SU(5)$ GUT models from a top-down point of view. We show that in contrast to the more model dependent bounds on the proton lifetime, the limits on neutrino masses provide a robust, stringent and complementary constraint on all $SU(5)$ GUT-based R-parity violating models. Focusing on well-motivated string/$M$ theory GUT frameworks with mechanisms for doublet-triplet splitting and a solution to the $\mu/B\mu$ problems, we show that imposing the neutrino mass bounds implies that R-parity violation is disfavored. The arguments can also be generalized to minimal $SO(10)$ GUTs. An experimental observation of R-parity violation would, therefore, disfavor such classes of top-down GUT models.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Motivated by results from the LHC and dark matter searches, we study the possibility of phenomenologically viable R-parity violation in $SU(5)$ GUT models from a top-down point of view. | contribution 0.72 | 0.50 | 0.04 | hedged possibility 0.74 |
| s1 | We show that in contrast to the more model dependent bounds on the proton lifetime, the limits on neutrino masses provide a robust, stringent and complementary constraint on all $SU(5)$ GUT-based R-parity violating models. | result 0.94 | 0.82 | 0.34 | asserted 1.00 |
| s2 | Focusing on well-motivated string/$M$ theory GUT frameworks with mechanisms for doublet-triplet splitting and a solution to the $\mu/B\mu$ problems, we show that imposing the neutrino mass bounds implies that R-parity violation is disfavored. | result 0.90 | 0.90 | 0.49 | asserted 0.99 |
| s3 | The arguments can also be generalized to minimal $SO(10)$ GUTs. | result 0.55 | 0.62 | 0.04 | asserted 0.66 |
| s4 | An experimental observation of R-parity violation would, therefore, disfavor such classes of top-down GUT models. | interpretation 0.99 | 0.40 | 0.55 | asserted 0.81 |
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The paper
Original abstract
Motivated by results from the LHC and dark matter searches, we study the possibility of phenomenologically viable R-parity violation in $SU(5)$ GUT models from a top-down point of view. We show that in contrast to the more model dependent bounds on the proton lifetime, the limits on neutrino masses provide a robust, stringent and complementary constraint on all $SU(5)$ GUT-based R-parity violating models. Focusing on well-motivated string/$M$ theory GUT frameworks with mechanisms for doublet-triplet splitting and a solution to the $\mu/B\mu$ problems, we show that imposing the neutrino mass bounds implies that R-parity violation is disfavored. The arguments can also be generalized to minimal $SO(10)$ GUTs. An experimental observation of R-parity violation would, therefore, disfavor such classes of top-down GUT models.
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How the literature uses it
3 arXiv papers cite this in 4 sentences
Papers citing it · 3 sentences without a confident label
Cites it as support 1 paper
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If $Z_q$ is completely broken, higher-dimensional Kähler potential operators will generate dangerous lepton-number violating operators which generically violate neutrino mass bounds [ref] .
Superpartners at LHC and Future Colliders: Predictions from Constrained Compactified M-Theory · Obtaining a Benchmark Spectrum · 0.97
What it cites · 93 sentences without a confident label
Uses data or values from 1 paper
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Making the simplifying assumption $|M_1| = |M_2 | = |μ| = M$ and taking the large $tanβ$ limit, we can obtain a limit on $ξ$ from the constraint $m_ν < 0.23$ eV [ref] : [equation] To be consistent with this limit on $ξ$, the four vectors $(μ, κ_i)$ and $(v_d, ṽ_i)$ must be nearly parallel.
Planck 2013 results. XVI. Cosmological parameters · Bilinear R-parity Violation $&$ Neutrino Mass constraints · 0.99
Cites as support 7 papers
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Analyses of the Heterotic $E_8 ×E_8$ string compactified on toroidal orbifolds have demonstrated numerous vacua with realistic MSSM spectra and R-parity conservation [ref] .
The Heterotic Road to the MSSM with R parity · Heterotic Orbifold Compactifications · 0.96
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Analyses of the Heterotic $E_8 ×E_8$ string compactified on toroidal orbifolds have demonstrated numerous vacua with realistic MSSM spectra and R-parity conservation [ref] .
Heterotic mini-landscape (II): completing the search for MSSM vacua in a Z_6 orbifold · Heterotic Orbifold Compactifications · 0.96
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Analyses of the Heterotic $E_8 ×E_8$ string compactified on toroidal orbifolds have demonstrated numerous vacua with realistic MSSM spectra and R-parity conservation [ref] .
A Mini-Landscape of Exact MSSM Spectra in Heterotic Orbifolds · Heterotic Orbifold Compactifications · 0.96
Cites as background 6 papers
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In what follows we briefly review the relevant details of this construction; interested readers should consult [ref] for additional details.
Deconstruction, G_2 Holonomy, and Doublet-Triplet Splitting · $M$ Theory Compactifications on Singular $G_2$-Manifolds · 0.92
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The constraints arising from bilinear R-parity violation have of course been known for quite some time [ref] .
Supersymmetry without R-Parity and without Lepton Number · Introduction and Motivation · 0.96
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The issue of RPV in flipped $SU(5)$ models is qualitatively different and discussed in [ref] .
Comments on Flipped SU(5) (and F-theory) · Minimal $SO(10)$ GUT Models · 0.80
Discussion
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