{"arxiv_id":"2308.02697","incoming":{"papers":6,"sentences":21,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":3,"quotes":[{"arxiv_id":"2310.07532","title":"Slepton searches in the trilinear RPV SUSY scenarios at the HL-LHC and HE-LHC","url":"/paper/2310.07532","section":"Collider analysis","sentence":"The track and calorimeter isolation, $b-$tagging efficiency, generation level cuts, jet matching, etc. are done in a similar way as prescribed in Sec.3 of Ref. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"2405.06040","title":"Searches for the BSM scenarios at the LHC using decision tree based machine learning algorithms: A comparative study and review of Random Forest, Adaboost, XGboost and LightGBM frameworks","url":"/paper/2405.06040","section":"Performance of different Decision Tree based algorithms - a RPC SUSY case study at the HL-LHC","sentence":"Lepton-lepton isolation, lepton-jet isolation, etc, also have been implemented as described in the Refs. [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":4,"sentences":4,"quotes":[{"arxiv_id":"2310.07532","title":"Slepton searches in the trilinear RPV SUSY scenarios at the HL-LHC and HE-LHC","url":"/paper/2310.07532","section":"Collider analysis","sentence":"The cross-sections for the SM backgrounds are taken from Table 11 and Table 13 of Ref. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"2405.06040","title":"Searches for the BSM scenarios at the LHC using decision tree based machine learning algorithms: A comparative study and review of Random Forest, Adaboost, XGboost and LightGBM frameworks","url":"/paper/2405.06040","section":"Searches for RPV SUSY scenarios using BDT","sentence":"It has been shown that an optimized cut-based analysis will be able to exclude $$ upto 2.18 TeV at the HL-LHC from wino like $$ and $$ productions [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2402.04040","title":"Status of R-parity violating SUSY","url":"/paper/2402.04040","section":"Prospect of electroweakino searches at the HL-LHC and HE-LHC","sentence":"The projected discovery and exclusion reaches of the HL-LHC ($√(s) = 13$ TeV and $ℒ = 3000$ fb$^-1$) and HE-LHC ($√(s) = 27$ TeV and $ℒ = 3000$ fb$^-1$) obtained in [ref] are illustrated in the left and right panel of Fig.[ref] respectively.","intent_p":0.99,"contests_p":null},{"arxiv_id":"2411.08112","title":"Markov Chain Monte Carlo analysis to probe trilinear $R$-parity violating SUSY scenarios and possible LHC signatures","url":"/paper/2411.08112","section":"Possible Collider signals to probe allowed region","sentence":"However, using the ATLAS $N_l ≥4l$ analysis [ref] , validated in Refs. [ref] , we observe that the lower bounds on $$ reduce to $∼$ 900 GeV when both the LLE and LQD couplings are nonzero, and as a result, the relevant branching ratios get suppressed.","intent_p":0.92,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2309.12918","title":"Combining Resonant and Tail-based Anomaly Detection","url":"/paper/2309.12918","section":"Introduction","sentence":"Our method should be contrasted with existing ML-based approaches to SUSY in the literature which are fully supervised (see e.g. [ref] ).","intent_p":0.81,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":4,"sentences":5,"quotes":[{"arxiv_id":"2402.04040","title":"Status of R-parity violating SUSY","url":"/paper/2402.04040","section":"Prospect of electroweakino searches at the HL-LHC and HE-LHC","sentence":"The works in Ref. [ref] have considered the $LLE$ type couplings while $UDD$ type coupling has been studied in [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"2310.07532","title":"Slepton searches in the trilinear RPV SUSY scenarios at the HL-LHC and HE-LHC","url":"/paper/2310.07532","section":"Model Definition","sentence":"For more details on the LSP decay modes and charged lepton configurations for various scenarios see Sec. 2 of Ref. [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"2608.21033","title":"The ABC of RPV III: Classification of R-parity Violating Signatures from LQD Couplings and their Coverage at the LHC","url":"/paper/2608.21033","section":"Introduction","sentence":"In particular, the diverse signatures arising from LSP decays in the RPV-MSSM have been explored in a wide range of phenomenological studies; see, e.g., Refs. [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"2411.08112","title":"Markov Chain Monte Carlo analysis to probe trilinear $R$-parity violating SUSY scenarios and possible LHC signatures","url":"/paper/2411.08112","section":"Possible Collider signals to probe allowed region","sentence":"In a recent analysis [ref] , the authors have studied the future prospect of electroweakino searches for different choices of LLE couplings from multilepton final states.","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":8},"outgoing":{"papers":118,"sentences":135,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":10,"sentences":11,"quotes":[{"arxiv_id":"2103.11684","title":"Search for supersymmetry in events with four or more charged leptons in $139\\,\\mbox{fb\\(^{-1}\\)}$ of $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","url":"/paper/2103.11684","section":"Collider Analysis","sentence":"For the reconstruction of leptons (electron, muon), we have followed the isolation, overlap removal procedures etc. according to the ATLAS analysis as mentioned in Sec. 5 of [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1603.02754","title":"XGBoost: A Scalable Tree Boosting System","url":"/paper/1603.02754","section":"Prospect at the HL-LHC using Machine Learning based analysis","sentence":"For our ML-based multi-variate analysis we have used Extreme Gradient Boosted decision tree algorithm through XGBoost machine learning toolkit [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1307.6346","title":"DELPHES 3, A modular framework for fast simulation of a generic collider experiment","url":"/paper/1307.6346","section":"Collider Analysis","sentence":"Then all these events passed through a fast detector simulation in the platform [ref] (version-3.5.0).","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/0603175","title":"PYTHIA 6.4 Physics and Manual","url":"/paper/hep-ph/0603175","section":"Collider Analysis","sentence":"The SUSY signal events have been generated using [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1304.0790","title":"Precision predictions for electroweak superpartner production at hadron colliders with Resummino","url":"/paper/1304.0790","section":"Collider Analysis","sentence":"The next-to-leading order + next-to-leading logarithmic (NLO+NLL) order cross-sections have been computed for the signal events ($$ and $$) by using [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2103.11684","title":"Search for supersymmetry in events with four or more charged leptons in $139\\,\\mbox{fb\\(^{-1}\\)}$ of $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","url":"/paper/2103.11684","section":"Collider Analysis","sentence":"Following the ATLAS analysis [ref] , the b-tagging efficiency has been chosen to be 85$%$ and the light jet mistagging efficiency (as b-jet) 25$%$.","intent_p":0.8,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":43,"sentences":45,"quotes":[{"arxiv_id":"2306.07317","title":"The ABC of RPV: Classification of R-Parity Violating Signatures at the LHC for Small Couplings","url":"/paper/2306.07317","section":"Introduction","sentence":"Depending on the choice of the LSP and non-zero RPV coupling, there can be a plethora of different kinds of final states [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1301.2336","title":"Natural SUSY's Last Hope: R-parity Violation via UDD Operators","url":"/paper/1301.2336","section":"Introduction","sentence":"Depending on the choice of the LSP and non-zero RPV coupling, there can be a plethora of different kinds of final states [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"2003.10920","title":"Electroweakino searches at the HL-LHC in the baryon number violating MSSM","url":"/paper/2003.10920","section":"Introduction","sentence":"Depending on the choice of the LSP and non-zero RPV coupling, there can be a plethora of different kinds of final states [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1510.02660","title":"R-parity violating supersymmetry and neutrino physics: experimental signatures","url":"/paper/1510.02660","section":"Introduction","sentence":"Depending on the choice of the LSP and non-zero RPV coupling, there can be a plethora of different kinds of final states [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1611.03846","title":"Search for bottom squarks in the baryon-number violating MSSM","url":"/paper/1611.03846","section":"Introduction","sentence":"Depending on the choice of the LSP and non-zero RPV coupling, there can be a plethora of different kinds of final states [ref] .","intent_p":0.83,"contests_p":null}]}],"unlabelled_sentences":78},"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/2308.02697"}}