{"arxiv_id":"1003.0705","incoming":{"papers":44,"sentences":61,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1101.4758","title":"W mass and Leptonic Z-decays in the NMSSM","url":"/paper/1101.4758","section":"Numerical results","sentence":"This program is then coupled to the NMSSMTools 2.3.2 package [ref] , computing the NMSSM spectrum and checking already several phenomenological constraints: stability of the electroweak vacuum, bounds from LEP [ref] , and in particular the new Aleph limits [ref] [A bug in the corresponding version of the code for the computation of Aleph constraints was replaced by a self-made program.","intent_p":0.94,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":7,"sentences":8,"quotes":[{"arxiv_id":"1002.2952","title":"Hidden Higgs Decaying to Lepton Jets","url":"/paper/1002.2952","section":"Efficiencies of the Searches","sentence":"The numbers of observed events and the background estimates given in Table [ref] refer to the following: * $H →4 τ$ search: invisible Z channel, $n_1,2^track =$2 or 4, see Table 3 of [ref] , * Invisible Higgs search in OPAL: more-than-2-jet events with $M_miss$ in the 100-104 GeV bin, see Fig.4 in [ref] , * $H →WW^*$ search in ALEPH: the class 2c and 2t defined in Table 3 of [ref] , * Six-lepton search in ALEPH: small $Δm$ selection defined in Table 3.4 of [ref] , * $2j+ E/$ search in OPAL and ALEPH: selection A, see Table 2 of [ref] , and large $Δm$ AJ selection (years 1999-2000), see Table 5 of [ref] , * $2j+2l+ E/$ in ALEPH: to the large $Δm$ selection (years 1999-2000), see Table 5 of [ref] * Dark photon search in D0: electron pairs with 0.2-0.4 GeV invariant mass, see Fig. 2 of [ref] , * Unified trilepton search in CDF: trileptons defined by the (least tight) ttt cut, see Table 1 of","intent_p":0.99,"contests_p":null},{"arxiv_id":"1002.1971","title":"New constraints on a light CP-odd Higgs boson and related NMSSM Ideal Higgs Scenarios","url":"/paper/1002.1971","section":"Introduction","sentence":"We also quantify the impact of these constraints, as well as the impact of the new ALEPH LEP results in the $→Z+4τ$ final state [ref] , on the Next-to-Minimal Supersymmetric Model (NMSSM) ideal Higgs scenarios.","intent_p":0.87,"contests_p":null},{"arxiv_id":"1007.1918","title":"Rare Z-decay into light CP-odd Higgs bosons: a comparative study in different new physics models","url":"/paper/1007.1918","section":"Constraints on the new physics models","sentence":"We compute the signals from the Higgs-strahlung production $e^+ e^- →Z h_i$ ($i= 1, 2$) with $h_i →2 b, 2 τ, 4 b, 4 τ, 2 b 2 τ$ [ref] and from the associated production $e^+ e^- →h_i a$ with $h_i a →4 b, 4 τ, 2 b 2 τ, 6 b, 6 τ$ [ref] , and compare them with the corresponding LEP data which have been inputted into our code.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1009.2555","title":"CoGeNT, DAMA, and Neutralino Dark Matter in the Next-To-Minimal Supersymmetric Standard Model","url":"/paper/1009.2555","section":"Constraints and Scanning in the NMSSM","sentence":"However, we have updated the limit on $Γ_Z→$ to $1.9$ as in [ref] .] We have augmented to include the recent ALEPH constraints [ref] on $→Z +Higgs$ with $Higgs→aa$ (in our case $a=$, the lightest CP-odd Higgs boson of the NMSSM) with $a→$.","intent_p":0.85,"contests_p":null},{"arxiv_id":"1012.1316","title":"SUSY Digs up a Buried Higgs","url":"/paper/1012.1316","section":"Introduction","sentence":"If $m_η<12$ GeV, the lower bound is slightly stronger [ref] , $m_h>86$ GeV, while recently recasted [ref] ALEPH data [ref] set $m_η≳4$ GeV for $m_h=100$ GeV.","intent_p":0.89,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1002.1971","title":"New constraints on a light CP-odd Higgs boson and related NMSSM Ideal Higgs Scenarios","url":"/paper/1002.1971","section":"Effective $ξ^2$ in the $h→4τ$ channel for vector-boson fusion at the LHC and LEP $Zh$ channel constraints","sentence":"Of course, the knowledgeable reader will recognize that all the $ξ^2$ plots presented are aimed at comparing these NMSSM models to the new ALEPH analysis of the $4τ$ final state [ref] .","intent_p":0.81,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1812.00380","title":"A search for pair production of new light bosons decaying into muons in proton-proton collisions at 13 TeV","url":"/paper/1812.00380","section":"Signal modeling","sentence":"This range is motivated by constraints set by the relic density measurements from WMAP [ref] and Planck [ref] , as well as searches at LEP [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":3,"sentences":3,"quotes":[{"arxiv_id":"2110.13225","title":"Exotic Higgs Decays to Four Taus at Future Electron-Positron Colliders","url":"/paper/2110.13225","section":"Introduction","sentence":"Previous studies of $h→4τ$ at lepton colliders include the searches carried out at LEP [ref] , and an ILC study performed in the context of the NMSSM [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1510.06534","title":"Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into tau leptons in pp collisions at sqrt(s) = 8 TeV","url":"/paper/1510.06534","section":"Introduction","sentence":"The analyses carried out by the OPAL and ALEPH Collaborations at LEP [ref] searched for the decay of the CP-even Higgs boson into a pair of light CP-odd Higgs bosons, exploiting the Higgs-strahlung process, where the CP-even state is produced in association with a boson.","intent_p":0.87,"contests_p":null},{"arxiv_id":"1808.01890","title":"Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at $\\sqrt{s} =$ 8 and 13 TeV","url":"/paper/1808.01890","section":"Introduction","sentence":"Despite an extensive program of searches for such resonances by the CERN LEP experiments [ref] , and by the ATLAS [ref] , CMS [ref] , and LHCb [ref] Collaborations, the present experimental limits on the product of production cross sections and branching fractions do not yet exclude the existence of such particles [ref] .","intent_p":0.87,"contests_p":null}]}],"unlabelled_sentences":47},"outgoing":{"papers":4,"sentences":4,"groups":[],"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":{"arxiv_id":"1003.0705","kind":"model","paper_version":2,"prompt_version":"held-up-v3.5","generated_at":"2026-10-28T00:25:08+00:00","loaded_at":"2026-10-28T01:04:53.546715+00:00","evidence":"substantial","account":[],"groups":[{"kind":"data_used","label":"Uses its data or values","papers":2,"entries":[{"p":0.87,"quote":null,"citing":[{"self":false,"year":2010,"title":"New constraints on a light CP-odd Higgs boson and related NMSSM Ideal Higgs Scenarios","arxiv_id":"1002.1971"}],"verified":true,"paraphrase":"Quantified the impact of this paper's new ALEPH LEP results in the Z+4tau final state on the NMSSM ideal Higgs scenarios."},{"p":0.85,"quote":null,"citing":[{"self":false,"year":2010,"title":"CoGeNT, DAMA, and Neutralino Dark Matter in the Next-To-Minimal Supersymmetric Standard Model","arxiv_id":"1009.2555"}],"verified":true,"paraphrase":"Augmented its limits to include this paper's recent ALEPH constraints on Z+Higgs with Higgs to aa and a to taus."}],"papers_all":7,"self_papers":0,"self_entries":[]}],"counts":{"by_kind":{"data_used":7,"comparison":1,"method_or_tool":1,"supports_this_paper":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":20,"self_papers":2,"citing_papers":45,"sentences_read":28,"citing_sentences":62,"unambiguous_read":28,"typed_independent":10,"independent_papers":43,"by_kind_independent":{"data_used":7,"comparison":1,"method_or_tool":1,"supports_this_paper":2}},"input_sha256":"922d23e3c52d4f452e781806ec89b29fab986cb18c8bffc4caf1417647be52d5","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":"2 later papers by other authors are listed below: 2 used its data or values."},"_links":{"html":"https://pith.science/paper/1003.0705"}}