{"arxiv_id":"1207.4846","incoming":{"papers":27,"sentences":33,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1307.3383","title":"Determination of the CMSSM Parameters using Neural Networks","url":"/paper/1307.3383","section":"Summary and Conclusions","sentence":"The cuts could then be optimized for each benchmark point separately, as e.g. done in [ref] .","intent_p":0.91,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1210.2395","title":"Spread Supersymmetry with Wino LSP: Gluino and Dark Matter Signals","url":"/paper/1210.2395","section":"Future prospects","sentence":"For $√(s) = 14 TeV$ and very heavy squarks, the LHC has a discovery reach of $m_g̃$ up to about $2.0 TeV$ ($2.3 TeV$) with an integrated luminosity of $300 fb^-1$ ($3000 fb^-1$) [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"1509.02929","title":"Upper bounds on sparticle masses from naturalness or how to disprove weak scale supersymmetry","url":"/paper/1509.02929","section":"Conclusions:","sentence":"However, if we require a more stringent naturalness condition of $Δ_EW10$ then $m_2$ TeV and the most natural region of parameter space should be accessible to LHC13 (LHC13 has a projected $5σ$ discovery reach to $m_∼2$ TeV for 300-1000 fb$^-1$ of data [ref] ).","intent_p":0.83,"contests_p":null},{"arxiv_id":"1301.6085","title":"Supersymmetric SO(10) GUTs with sliding scales","url":"/paper/1301.6085","section":"Leading-Log RGE Invariants","sentence":"According to [ref] the LHC at $√(s)=14$ TeV will be able to explore SUSY masses up to $m_g̃∼3.2$ TeV ($3.6$ TeV) for $m_q̃ ≃m_g̃$ and of $m_g̃∼1.8$ TeV ($2.3$ TeV) for $m_q̃ ≫m_g̃$ with 300 fb$^-1$ (3000 fb$^-1$).","intent_p":0.96,"contests_p":null},{"arxiv_id":"1303.4256","title":"Muon g-2 vs LHC in Supersymmetric Models","url":"/paper/1303.4256","section":"Future prospects","sentence":"According to the future sensitivity in Ref. [ref] based on the minimal supergravity models, the gluino lighter than $1.8$ and $2.3$ can be discovered at the $14$ LHC with $∫ℒ = 300$ and $3000$, respectively.","intent_p":0.83,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1912.04079","title":"GAMBIT and its Application in the Search for Physics Beyond the Standard Model","url":"/paper/1912.04079","section":"Supersymmetry","sentence":"The has been studied in global fits for over a decade [ref] , most recently in the analysis in [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1303.5776","title":"Stop and sbottom search using dileptonic $M_{T2}$ variable and boosted top technique at the LHC","url":"/paper/1303.5776","section":"Introduction and motivation","sentence":"There have been quite a few phenomenological analysis to investigate cMSSM signatures at the LHC using different techniques to suppress SM background [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1308.6484","title":"Probing the flavor violating scalar top quark signal at the LHC","url":"/paper/1308.6484","section":"Introduction","sentence":"The early searches in SUSY, the most popular model among all the BSM options, have focussed, both phenomenologically [ref] and experimentally [ref] , on the constrained minimal supersymmetric standard model(CMSSM)/minimal supergravity(mSUGRA) [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1410.4999","title":"Sparticle Mass Hierarchies, Simplified Models from SUGRA Unification, and Benchmarks for LHC Run-II SUSY Searches","url":"/paper/1410.4999","section":"Model Signatures","sentence":"For recent analyses relating to sparticle signature identification at the upgraded LHC see [ref] .","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":24},"outgoing":{"papers":2,"sentences":5,"groups":[{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1202.4937","title":"Higgs signal in Chargino-Neutralino production at the LHC","url":"/paper/1202.4937","section":"LHC14 reach for SUSY with 300 fb$^-1$ and 3000 fb$^-1$","sentence":"Although these numbers superficially seem lower than our earlier projections [ref] , we should keep in mind that here we have not included any signal K-factors and have also included the $Ztt̅$ background.","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":4},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/1207.4846"}}