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Light Stop NLSPs at the Tevatron and LHC
High Energy Physics - Phenomenology · Submitted 31 May 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Focusing on the case of prompt decays, we simulate several existing Tevatron and LHC analyses that would be sensitive to this scenario, and find that they allow the stop to be as light as 150 GeV, mostly due to the large top production background.
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The abstract, sentence by sentence
How light can the stop be given current experimental constraints? Can it still be lighter than the top? In this paper, we study this and related questions in the context of gauge-mediated supersymmetry breaking, where a stop NLSP decays into a W, b and gravitino. Focusing on the case of prompt decays, we simulate several existing Tevatron and LHC analyses that would be sensitive to this scenario, and find that they allow the stop to be as light as 150 GeV, mostly due to the large top production background. With more data, the existing LHC analyses will be able to push the limit up to at least 180 GeV. We hope this work will motivate more dedicated experimental searches for this simple scenario, in which, for most purposes, the only free parameters are the stop mass and lifetime.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | How light can the stop be given current experimental constraints? | background 0.72 | 0.04 | 0.02 | unclear 0.99 |
| s1 | Can it still be lighter than the top? | background 0.71 | 0.04 | 0.02 | unclear 0.76 |
| s2 | In this paper, we study this and related questions in the context of gauge-mediated supersymmetry breaking, where a stop NLSP decays into a W, b and gravitino. | contribution 0.96 | 0.66 | 0.04 | asserted 0.95 |
| s3 | Focusing on the case of prompt decays, we simulate several existing Tevatron and LHC analyses that would be sensitive to this scenario, and find that they allow the stop to be as light as 150 GeV, mostly due to the large top production background. | result 0.99 | 0.94 | 0.77 | asserted 1.00 |
| s4 | With more data, the existing LHC analyses will be able to push the limit up to at least 180 GeV. | result 0.78 | 0.61 | 0.18 | hedged possibility 0.77 |
| s5 | We hope this work will motivate more dedicated experimental searches for this simple scenario, in which, for most purposes, the only free parameters are the stop mass and lifetime. | future work 1.00 | 0.09 | 0.07 | hedged possibility 0.43 |
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The paper
Original abstract
How light can the stop be given current experimental constraints? Can it still be lighter than the top? In this paper, we study this and related questions in the context of gauge-mediated supersymmetry breaking, where a stop NLSP decays into a W, b and gravitino. Focusing on the case of prompt decays, we simulate several existing Tevatron and LHC analyses that would be sensitive to this scenario, and find that they allow the stop to be as light as 150 GeV, mostly due to the large top production background. With more data, the existing LHC analyses will be able to push the limit up to at least 180 GeV. We hope this work will motivate more dedicated experimental searches for this simple scenario, in which, for most purposes, the only free parameters are the stop mass and lifetime.
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References
How the literature uses it
34 arXiv papers cite this in 44 sentences
Papers citing it · 24 sentences without a confident label
Uses its method or tool 1 paper
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We find, using the methods of [ref] , that neither sets the expected limit due to tightened analysis cuts.
The Status of GMSB After 1/fb at the LHC · Stop NLSP (direct production) · 0.80
Uses its data or values 1 paper
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In [ref] , it was estimated that two of the $35$ LHC analyses available at that time would be able to probe stops up to about $180$ GeV, if updated to 1/fb.
The Status of GMSB After 1/fb at the LHC · Stop NLSP (direct production) · 0.88
Cites it as support 2 papers
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Direct searches for third family sparticles allow for stops as light as the top and SUSY can be natural [ref] .
A Non Standard Model Higgs at the LHC as a Sign of Naturalness · Introduction · 0.98
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The existing LHC data do not exclude a light and long-lived stop [ref] .
On low-energy predictions of unification models inspired by F-theory · Discussion · 0.96
Cites it as background 16 papers
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Ref. [ref] investigate a stop NLSP and a gravitino LSP scenario for the Tevatron as well as the LHC.
Probing Minimal Flavor Violation with Long-Lived Stops and Light Gravitinos at Hadron Colliders · Introduction · 0.89
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Hiding stops at low masses has been investigated by many groups in the past [ref] .
Natural SUSY in Plain Sight · Introduction · 0.97
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(In defining GGM, we will not discuss the Higgs sector in detail, but simply assume that $μ$ and $tanβ$ can be set freely.) A number of papers have studied both the Tevatron bounds and LHC projections [ref] , elaborating on and greatly extending the scope of the pioneering Tevatron-era work on gauge mediated phenomenology [ref] .
The Status of GMSB After 1/fb at the LHC · Introduction · 0.80
What it cites · 47 sentences without a confident label
Uses the method or tool of 11 papers
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We have implemented the dilepton stop mass reconstruction algorithm of the CDF analysis [ref] (in a somewhat simplified way described in appendix [ref]).
Search for Pair Production of Supersymmetric Top Quarks in Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV · Stop mass reconstruction · 1.00
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The intermediate step of decaying the stop NLSPs is done according to ([ref]) with our own software.[The authors will be willing to provide copies of the software, or parton-level event files produced with it, to any interested parties.] For the gravity-mediated stops that we use in the process of deriving limits from the CDF stop mass reconstruction procedure of [ref] in section [ref], the decay is performed by Pythia, after the desired spectra are created using SuSpect [ref] .
SuSpect: a Fortran Code for the Supersymmetric and Higgs Particle Spectrum in the MSSM · Simulation details · 0.95
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Here we will only use the simple cuts which precede that procedure (the “selection 1” described in [ref] ).
Search for pair production of the scalar top quark in the electron-muon final state · Constraints from the Tevatron and the LHC · 0.87
Uses data or values from 5 papers
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With these pairs in hand, we can approximately read off the corresponding $95%$ CL exclusion limits from figure 2 of [ref] .
Search for Pair Production of Supersymmetric Top Quarks in Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV · Stop mass reconstruction · 0.86
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NNLO$_approx$+NNLL calculations give the $tt̅$ production cross section at the Tevatron as $σ_tt̅ = 6.30 ±0.19^+0.31_-0.23$ pb [ref] or $7.08^+0.20+0.36_-0.24-0.27$ pb [ref] .
Renormalization-Group Improved Predictions for Top-Quark Pair Production at Hadron Colliders · $tt̅$ and $^∗$ production cross sections · 0.98
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NNLO$_approx$+NNLL calculations give the $tt̅$ production cross section at the Tevatron as $σ_tt̅ = 6.30 ±0.19^+0.31_-0.23$ pb [ref] or $7.08^+0.20+0.36_-0.24-0.27$ pb [ref] .
Next-to-next-to-leading soft-gluon corrections for the top quark cross section and transverse momentum distribution · $tt̅$ and $^∗$ production cross sections · 0.98
Compares with 1 paper
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This is confirmed by table [ref] where we compare our results for stops in gravity-mediated scenarios with those obtained by CDF [ref] (after normalizing our predictions to the stop cross sections used by CDF).[The only exception is the $135$ GeV stop in the $b$-tagged channel where our result is about twice bigger.
Search for Pair Production of Supersymmetric Top Quarks in Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV · Simulation details · 1.00
Cites as background 7 papers
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At the Tevatron, CDF [ref] and D0 [ref] have considered the situation in which the stop decays via a virtual chargino as →bℓ^+ν̃
Search for the lightest scalar top quark in events with two leptons in ppbar collisions at sqrt(s)=1.96 TeV · Searches for new physics · 0.86
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At the Tevatron, CDF [ref] and D0 [ref] have considered the situation in which the stop decays via a virtual chargino as →bℓ^+ν̃
Search for the supersymmetric partner of the top quark in ppbar collisions at sqrt(s) = 1.96 TeV · Searches for new physics · 0.86
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At the Tevatron, CDF [ref] and D0 [ref] have considered the situation in which the stop decays via a virtual chargino as →bℓ^+ν̃
Search for pair production of the scalar top quark in the electron-muon final state · Searches for new physics · 0.86
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