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$\theta_{13}$ and the Higgs mass from high scale supersymmetry
High Energy Physics - Phenomenology · Submitted 17 May 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A relatively large $\sin{\theta_{13}}$ is the natural result.
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The abstract, sentence by sentence
In the framework in which supersymmetry is used for understanding fermion masses rather than stabilizing the electroweak scale, we elaborate the phenomenological analysis for the neutrino physics. A relatively large $\sin{\theta_{13}}$ is the natural result. The model further predicts vanishingly small CP violation in neutrino oscillations. And $\theta_{23}$ is not necessarily maximal. While the high scale supersymmetry generically results in a Higgs mass of about 141 GeV, our model reduces this mass via introducing SU(2)$_L$ triplet fields which also contribute to neutrino masses.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In the framework in which supersymmetry is used for understanding fermion masses rather than stabilizing the electroweak scale, we elaborate the phenomenological analysis for the neutrino physics. | contribution 0.75 | 0.78 | 0.06 | asserted 0.90 |
| s1 | A relatively large $\sin{\theta_{13}}$ is the natural result. | result 1.00 | 0.79 | 0.35 | asserted 0.99 |
| s2 | The model further predicts vanishingly small CP violation in neutrino oscillations. | result 1.00 | 0.80 | 0.15 | asserted 1.00 |
| s3 | And $\theta_{23}$ is not necessarily maximal. | result 1.00 | 0.74 | 0.06 | hedged possibility 0.61 |
| s4 | While the high scale supersymmetry generically results in a Higgs mass of about 141 GeV, our model reduces this mass via introducing SU(2)$_L$ triplet fields which also contribute to neutrino masses. | contribution 0.45 | 0.84 | 0.29 | asserted 0.96 |
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The paper
Original abstract
In the framework in which supersymmetry is used for understanding fermion masses rather than stabilizing the electroweak scale, we elaborate the phenomenological analysis for the neutrino physics. A relatively large $\sin{\theta_{13}}$ is the natural result. The model further predicts vanishingly small CP violation in neutrino oscillations. And $\theta_{23}$ is not necessarily maximal. While the high scale supersymmetry generically results in a Higgs mass of about 141 GeV, our model reduces this mass via introducing SU(2)$_L$ triplet fields which also contribute to neutrino masses.
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References
How the literature uses it
10 arXiv papers cite this in 23 sentences
Papers citing it · 13 sentences without a confident label
Contests it 1 paper
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In addition, in [ref] it was wrong to say CP violation is small in the lepton sector.
Neutrino phenomenology of a high scale supersymmetry model · Discussions · contest 0.94
Compares with it 1 paper
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The physics analysis including $λ_1^ν$ is different from our previous one [ref] .
Neutrino phenomenology of a high scale supersymmetry model · Neutrino masses · 0.93
Cites it as background 5 papers
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This includes models which some authors call `Intermediate Scale SUSY'.] [ref] , following the work of Ibanez, Marchesano, Regalado and Valenzuela [ref] .
Precision Unification and Proton Decay in F-Theory GUTs with High Scale Supersymmetry · Introduction · 0.80
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Models based on this approach have been discussed extensively (see, e.g., [ref] for some recent works) and they often lead to intriguing mixing patterns, including the well-known tribimaximal mixing (TBM) [ref] and bimaximal mixing (BM) [ref] .
Neutrino Mixing and Discrete Symmetries · Introduction · 0.97
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With this view point, we revisit extensions of the Standard Model with vector-like fermions which lead to precision gauge coupling unification (for earlier works in this direction, please see [ref] ).
Unification with Vector-like fermions and signals at LHC · Introduction · 0.90
What it cites · 9 sentences without a confident label
Contests 1 paper
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More importantly, the high scale SUSY generically predicts the SM Higgs mass to be $141$ GeV (for a large $tanβ$ as in our case) [ref] , while recent LHC experiments have ruled out this mass, and discovered that the Higgs mass is $126$ GeV [ref] .
A sharp 141 GeV Higgs prediction from environmental selection · Introduction · contest 0.75
Uses data or values from 3 papers
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Experimental neutrino oscillation parameters are measured as follows [ref] , $Δm^2_21=(7.59 ±0.21)×10^-5 eV^2$, $Δm^2_32=(2.43 ±0.13)×10^-3 eV^2$ and $sin^2(2θ_12) = 0.861^+0.026_-0.022$, $sin^2(2θ_23) > 0.92$, $sin^2(2θ_13) = 0.088 ±0.008$.
Observation of electron-antineutrino disappearance at Daya Bay · Neutrino mixing and CP violation · 1.00
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In the case of a large $tanβ$, the Higgs mass of ($141 ±2$) GeV was predicted [ref] .
A sharp 141 GeV Higgs prediction from environmental selection · Higgs mass · 0.84
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With appropriate negative quartic coupling (about $-0.02$ as shown in [ref] ) at the high scale, a Higgs mass of about $126$ GeV compatible with the recent experimental results can be obtained.
Higgs mass implications on the stability of the electroweak vacuum · Higgs mass · 0.82
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