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Muon g-2 and 125 GeV Higgs in Split-Family Supersymmetry
High Energy Physics - Phenomenology · Submitted 27 Mar 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim With the split-family spectrum, the deviation of the muon g-2 and the observed Higgs boson mass are explained simultaneously.
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The abstract, sentence by sentence
We discuss the minimal supersymmetric standard model with "split-family" spectrum where the sfermions in the first two generations are in the hundreds GeV to a TeV range while the sfermions in the third generation are in the range of tens TeV. With the split-family spectrum, the deviation of the muon g-2 and the observed Higgs boson mass are explained simultaneously. It is predicted that the gluino and the squarks in the first two generations are within the reach of the LHC experiments in most favored parameter space for the universal gaugino mass, which can be tested by searching for events with missing transverse energy or events with stable charged massive particles. We also point out that the split-family scenario can be consistent with the focus point scenario for the non-universal gaugino masses where the required mu-term is in the hundreds GeV range.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the minimal supersymmetric standard model with "split-family" spectrum where the sfermions in the first two generations are in the hundreds GeV to a TeV range while the sfermions in the third generation are in the range of tens TeV. | contribution 0.54 | 0.23 | 0.07 | asserted 0.95 |
| s1 | With the split-family spectrum, the deviation of the muon g-2 and the observed Higgs boson mass are explained simultaneously. | result 0.97 | 0.71 | 0.76 | asserted 1.00 |
| s2 | It is predicted that the gluino and the squarks in the first two generations are within the reach of the LHC experiments in most favored parameter space for the universal gaugino mass, which can be tested by searching for events with missing transverse energy or events with stable charged massive particles. | result 0.75 | 0.76 | 0.16 | asserted 0.72 |
| s3 | We also point out that the split-family scenario can be consistent with the focus point scenario for the non-universal gaugino masses where the required mu-term is in the hundreds GeV range. | result 0.64 | 0.72 | 0.07 | hedged possibility 0.99 |
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The paper
Original abstract
We discuss the minimal supersymmetric standard model with "split-family" spectrum where the sfermions in the first two generations are in the hundreds GeV to a TeV range while the sfermions in the third generation are in the range of tens TeV. With the split-family spectrum, the deviation of the muon g-2 and the observed Higgs boson mass are explained simultaneously. It is predicted that the gluino and the squarks in the first two generations are within the reach of the LHC experiments in most favored parameter space for the universal gaugino mass, which can be tested by searching for events with missing transverse energy or events with stable charged massive particles. We also point out that the split-family scenario can be consistent with the focus point scenario for the non-universal gaugino masses where the required mu-term is in the hundreds GeV range.
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References
How the literature uses it
30 arXiv papers cite this in 38 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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With the splitting mass spectrum, the muon g-2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV.
Splitting Mass Spectra and Muon g-2 in Higgs-Anomaly Mediation · 0.97
Papers citing it · 28 sentences without a confident label
Builds on it 1 paper
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In this section, we update the favored region for the muon $g-2$ and the Higgs boson mass in Ref. [ref] in light of the current LHC data.
Muon $g-2$ in Split-Family SUSY in light of LHC Run II · Phenomenology of Split-Family SUSY model · 0.87
Compares with it 1 paper
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A similar direction was previously addressed in [ref] , though our arguments have the unique reasoning for them.
Sparticle spectroscopy of the minimal SO(10) model · Introduction · 0.86
Cites it as support 1 paper
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[We also assume that the hierarchy of the soft masses and the Yukawa couplings are aligned.] These assumptions are implicitly made, for example, in the models [ref] to avoid too large FCNC.
Muon $g-2$ in Split-Family SUSY in light of LHC Run II · Split-Family SUSY Model · 0.96
Cites it as background 7 papers
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The authors in Ref. [ref] assume MSSM Higgs fields ($H_u$ and $H_d$) with a common SSB mass either with the first two generation sfermions or with the third generation squarks and sleptons.
Reconciling Muon g-2, 125 GeV Higgs and Dark Matter in Gauge Mediation Models · Introduction · 0.80
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This standard MSSM case is well known (for reviews see [ref] ; recent works are [ref] ), and it requires SUSY masses in the few-hundred GeV range in order to explain the deviation [ref]; the LHC experiments, however, start to exclude parts of the relevant parameter space [ref] .
Large muon $(g-2)$ with TeV-scale SUSY masses for $\tan\beta\to\infty$ · Introduction · 0.94
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Therefore recently many new physics scenarios have been explored in this context, for an incomplete list of which one may refer [ref] .
Neutrino mass, mixing and muon $g-2$ explanation in $U(1)_{L_\mu-L_\tau}$ extension of left-right theory · Introduction · 0.99
What it cites · 14 sentences without a confident label
Uses the method or tool of 2 papers
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These corrections are included by solving one-loop renormalization group equations below the decoupling scale of the third generation SUSY particles [ref] .
Threshold and Flavour Effects in the Renormalization Group Equations of the MSSM II: Dimensionful couplings · Split-family SUSY · 0.95
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The calculation is performed using micOMEGAs [ref] .
Dark matter direct detection rate in a generic model with micrOMEGAs2.2 · Case II : Large Higgs soft mass squared · 1.00
Uses data or values from 2 papers
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The prediction of the Standard Model prediction is, on the other hand, given by [ref] ; [equation] in which the updated data from $e^+e^-→$ hadrons and the latest evaluation of the hadronic light-by-light scattering contributions are included.
(g-2)_mu and alpha(M_Z^2) re-evaluated using new precise data · The muon anomalous magnetic moment · 0.95
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In Fig. [ref], we used the strange quark content of the nucleon, $f_s≃0.26$, which is the default value used in micOMEGAs, while the smaller value suggested by the recent lattice calculation [ref] , $f_s=0.009$, is used in Fig. [ref].
Nucleon strange quark content from N_f=2+1 lattice QCD with exact chiral symmetry · Case II : Large Higgs soft mass squared · 0.83
Cites as background 3 papers
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[ The later possibilities have been widely discussed in the models of pure gravity mediation [ref] , the models with strong moduli stabilization [ref] , the minimal split supersymmetry [ref] , where the gauginos (and Higgsinos) are in the TeV range.
Chaotic inflation and supersymmetry breaking · Introduction · 0.84
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[ The later possibilities have been widely discussed in the models of pure gravity mediation [ref] , the models with strong moduli stabilization [ref] , the minimal split supersymmetry [ref] , where the gauginos (and Higgsinos) are in the TeV range.
The Lightest Higgs Boson Mass in Pure Gravity Mediation Model · Introduction · 0.84
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[ The later possibilities have been widely discussed in the models of pure gravity mediation [ref] , the models with strong moduli stabilization [ref] , the minimal split supersymmetry [ref] , where the gauginos (and Higgsinos) are in the TeV range.
Simply Unnatural Supersymmetry · Introduction · 0.84
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