{"arxiv_id":"1303.2985","incoming":{"papers":124,"sentences":199,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":9,"sentences":14,"quotes":[{"arxiv_id":"1305.1313","title":"Natural Supersymmetry and Implications for Higgs physics","url":"/paper/1305.1313","section":"Direct sbottom searches","sentence":"To bound $b̅ b + E_T$ signals, CMS [ref] retains events with 2-3 jets and 1 or 2 $b$-tags.","intent_p":0.91,"contests_p":null},{"arxiv_id":"2104.03302","title":"The Tiny (g-2) Muon Wobble from Small-$\\mu$ Supersymmetry","url":"/paper/2104.03302","section":"Benchmark Points Explaining $Δa_μ$, Dark Matter and Avoiding LHC Constraints","sentence":"In order to solve this problem, we use [ref] , that uses Monte Carlo event generation to compare all production and decay channels for the neutralinos, charginos and sleptons with the current LHC analyses [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1410.0965","title":"Constraining supersymmetry at the LHC with simplified models for squark production","url":"/paper/1410.0965","section":"Event generation and parameter scan","sentence":"We used Delphes 3.0.11 [ref] with Fastjet [ref] for detector simulation using the standard CMS settings included in this version of Delphes, but changed the $b$-tag misidentification rate to 0.01 [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1710.10785","title":"Testing Higgs boson scenarios in the phenomenological NMSSM","url":"/paper/1710.10785","section":"Experimental constraints and fit procedure","sentence":"The “post-processing” means passing the posterior sample points, in SLHA [ref] format, to SModelS and HiggsBounds for imposing the experimental 95% confidence limits from ATLAS and CMS SUSY bounds [ref] and the Tevatron and LHC Higgs physics bounds [ref] respectively.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1504.00927","title":"Signs of Tops from Highly Mixed Stops","url":"/paper/1504.00927","section":"Constraints from LHC8","sentence":"In order to ascertain the viability of our benchmark points we produce samples with , shower them with [ref] , and process them using [ref] , using all the available LHC searches, including jets plus $$ [ref] , searches exploting the $α_T$ variables [ref] , and single-lepton stop searches [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":27,"sentences":37,"quotes":[{"arxiv_id":"1308.2232","title":"Gluino bounds: Simplified Models vs a Particular SO(10) Model (A Snowmass white paper)","url":"/paper/1308.2232","section":"Introduction","sentence":"The lower bound on the gluino mass from CMS [ref] and ATLAS [ref] searches are $M_g̃ ≳1 - 1.2$ TeV, where the actual bound depends on the search strategy.","intent_p":0.81,"contests_p":null},{"arxiv_id":"1505.03479","title":"Long-Lived Particle Searches in R-Parity Violating MSSM","url":"/paper/1505.03479","section":"Relevant LHC Searches","sentence":"CMS also did a R-hadron search [ref] which excluding long-lived gluino (stop) LSP masses of 1322 GeV (820 GeV).","intent_p":0.8,"contests_p":null},{"arxiv_id":"1508.07318","title":"The search for mirror quarks at the LHC","url":"/paper/1508.07318","section":"Phenomenology: new physics at the LHC","sentence":"In our analysis, we have used the bounds from Ref. [ref] to impose constraints on the mirror quark mass and branching ratios to light jets and b-jet.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1405.0737","title":"Framework for Model Independent Analyses of Multiple Extra Quark Scenarios","url":"/paper/1405.0737","section":"Introduction","sentence":"By definition, one would expect that this search is not suited to a re-interpretation when considering coupling to light-flavour quarks and so, in addition, we use a set of four inclusive topological SUSY searches [ref] whose generic jets + 0,1,2 lepton signature should be sensitive to final states with light quarks.","intent_p":0.86,"contests_p":null},{"arxiv_id":"1307.8120","title":"Effective WIMPs","url":"/paper/1307.8120","section":"Limits from Collider Experiments","sentence":"For the $dijet + MET$ signal, we utilize two CMS simplified model searches for light generation squarks based on 11.7 fb$^-1$ [ref] and 19.5 fb$^-1$ [ref] luminosity at 8 TeV which have cross section limits as a function of squark, neutralino mass.","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":6,"sentences":8,"quotes":[{"arxiv_id":"1307.7723","title":"LHC Phenomenology of SO(10) Models with Yukawa Unification","url":"/paper/1307.7723","section":"Conclusions","sentence":"However, the excellent agreement between the gluino bounds from Refs. 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