{"arxiv_id":"1606.04833","incoming":{"papers":57,"sentences":82,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2208.13705","title":"Light dark matter around 100 GeV from the inert doublet model","url":"/paper/2208.13705","section":"Limits from collider searches","sentence":"HiggsBounds [ref] incorporates results from LEP [ref] , the Tevatron [ref] , the ATLAS [ref] , and the CMS [ref] experiments.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1607.03706","title":"Classification of simple heavy vector triplet models","url":"/paper/1607.03706","section":"Introduction","sentence":"For example, the effective Lagrangian given in Refs. [ref] provides a simple framework for $V'$ phenomenology at the LHC, and the framework is used in the analysis of ATLAS and CMS [ref] .","intent_p":0.87,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":9,"sentences":10,"quotes":[{"arxiv_id":"1705.09171","title":"Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton-proton collisions at sqrt(s) = 8 and 13 TeV","url":"/paper/1705.09171","section":"Spin-2 resonances","sentence":"For $k̃=1$, where the bulk graviton has comparable or larger width than the detector resolution, the most stringent lower limit of 1.1on its mass is set by a combination of searches in the diboson final state [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1607.01464","title":"Phenomenology of Bulk Scalar Singlets in the Randall Sundrum Model","url":"/paper/1607.01464","section":"SM Decays","sentence":"So we scale them using the parton luminosity ratios] run for a $600$ $(1000)$ GeV scalar are given by [ref] :","intent_p":0.99,"contests_p":null},{"arxiv_id":"1809.08933","title":"Improved constraints on the mixing and mass of $Z'$ bosons from resonant diboson searches at the LHC at $\\sqrt{s}=13$ TeV and predictions for Run II","url":"/paper/1809.08933","section":"Introduction","sentence":"By combining the results of searches in the $ννjj$, $ℓνjj$, $ℓℓjj$ and $jjjj$ channels, the ATLAS Collaboration [ref] set a lower bound of 2.60 on the mass of a spin-1 resonance at the 95% confidence level, in the context of the heavy vector triplet model.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1608.00463","title":"The limits on the strong Higgs sector parameters in the presence of new vector resonances","url":"/paper/1608.00463","section":"The vector resonance mass limits and the upper bounds on $σ(pp→ρ+X)×$","sentence":"For the sake of completeness, we should mention that the combined $WW+WZ$ analysis of $3.2fb^-1$ of $13TeV$ data [ref] implies stronger limits $g”>13.6$ and $g”>10.6$ for $M_ρ=1.5$ and $2TeV$, respectively.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1802.00354","title":"Hadron Collider Searches for Diboson Resonances","url":"/paper/1802.00354","section":"Searches for $ZZ$ Resonances","sentence":"Finally, the already reported combination of multiple searches in 8-TeV data [ref] resulted in a lower limit at 810 GeV; a combination of results of searches in the 2015 dataset of 13-TeV collisions [ref] produced a 95% CL exclusion of masses below 1.1 TeV, as already reported supra (Sec. [ref]).","intent_p":0.91,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":3,"quotes":[{"arxiv_id":"1607.08911","title":"Traces of a triboson resonance","url":"/paper/1607.08911","section":"ATLAS $ννJ$ diboson channel","sentence":"This value is slightly larger than the efficiency of 0.05 found by the ATLAS Collaboration for this type of signal [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":15,"sentences":16,"quotes":[{"arxiv_id":"1809.08933","title":"Improved constraints on the mixing and mass of $Z'$ bosons from resonant diboson searches at the LHC at $\\sqrt{s}=13$ TeV and predictions for Run II","url":"/paper/1809.08933","section":"Introduction","sentence":"These include fully leptonic ($ℓνℓν$, $ℓνℓℓ$) [ref] , semileptonic ($ννjj$, $ℓνjj$, $ℓℓjj$) [ref] and fully hadronic ($jjjj$) $VV$ [ref] final states.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1705.09171","title":"Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton-proton collisions at sqrt(s) = 8 and 13 TeV","url":"/paper/1705.09171","section":"Introduction","sentence":"Searches for such VV and VH resonances in different final states have previously been performed by the ATLAS [ref] and CMS [ref] experiments at the CERN LHC.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1706.09425","title":"CP violation effects in the diphoton spectrum of heavy scalars","url":"/paper/1706.09425","section":"Direct heavy neutral scalar searches","sentence":"The direct searches of heavy neutral scalars have been performed at the LHC, in the decay modes of heavy scalars into the SM particles of $VV = WW$, $ZZ$ [ref] , $hh$ [ref] and $hZ$ [ref] , with the $h$, $W$ and $Z$ bosons decaying further into lighter SM particles.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1808.01257","title":"Search for narrow H$\\gamma$ resonances in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","url":"/paper/1808.01257","section":"Introduction","sentence":"A number of searches for resonances decaying into the $$, $$, $$, $$, or $$ channels have been carried out at 7, 8, and 13center-of-mass energies [ref] by the ATLAS and CMS Collaborations, and stringent limits on their production have been set.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1612.09159","title":"Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at sqrt(s) = 13 TeV","url":"/paper/1612.09159","section":"Introduction","sentence":"Searches for diboson resonances have been previously performed in many different final states, placing lower limits on the masses of these resonances above the TeV scale [ref] .","intent_p":0.88,"contests_p":null}]}],"unlabelled_sentences":51},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"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":{"arxiv_id":"1606.04833","kind":"model","paper_version":2,"prompt_version":"held-up-v3.5","generated_at":"2026-10-27T21:52:03+00:00","loaded_at":"2026-10-28T01:04:19.274911+00:00","evidence":"substantial","account":[],"groups":[{"kind":"comparison","label":"Compares with it","papers":1,"entries":[{"p":1.0,"quote":null,"citing":[{"self":false,"year":2016,"title":"Traces of a triboson resonance","arxiv_id":"1607.08911"}],"verified":true,"paraphrase":"Reported its own efficiency of 0.053 for a W' to WZ diboson signal with M_W' = 2 TeV as close to this paper's reported efficiency of around 0.06 for a W' boson signal of this mass."}],"papers_all":1,"self_papers":0,"self_entries":[]}],"counts":{"by_kind":{"data_used":9,"comparison":1,"method_or_tool":2},"dropped":{"relied_on":0,"unknown_ids":0,"account_lines":0,"contest_vetoed":0,"below_threshold":0,"contest_drawback":0,"contest_without_basis":0,"contest_not_one_sentence":0,"contest_on_group_citation":0},"papers_read":11,"self_papers":2,"citing_papers":57,"sentences_read":15,"citing_sentences":82,"unambiguous_read":15,"typed_independent":12,"independent_papers":55,"by_kind_independent":{"data_used":9,"comparison":1,"method_or_tool":2}},"input_sha256":"22e81b6140a4c8322075c0f515202a3456719cb77d077ba512268036cf8f5e75","method":"For a paper with five or more citing arXiv papers, Pith selected up to 40 citing sentences its citation classifier typed, read those whose citation markers point at this paper alone, and wrote one paraphrase for each later paper in each group, each resting on one sentence. A later paper is listed under a label only when the classifier gives one of its sentences that label at intent probability 0.8 or more (0.95 for support), Pith's reading of the sentence finds that the citing paper itself did it, and a second check of the paraphrase against the sentence passes. The section lists uses only: building on the paper, using its method, tool, data or values, comparing with it and citing it as support. It does not list criticism or disagreement, so their absence says nothing about how the paper has been received. Code counted the papers, wrote the summary from the listed entries, set the evidence level and linked each entry to its citing paper. Quotes are copied from the citing sentence and shown only when the citing paper's licence is CC BY, CC BY-SA or CC0; otherwise the paraphrase is shown. Papers that share an author with this one are listed apart. A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"1 later paper by other authors is listed below: 1 compared its own results with it."},"_links":{"html":"https://pith.science/paper/1606.04833"}}