{"arxiv_id":"1105.2566","incoming":{"papers":60,"sentences":84,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1505.03517","title":"Photon-tagged and B-meson-tagged b-jet production at the LHC","url":"/paper/1505.03517","section":"Modification of tagged b-jet production in dense QCD matter","sentence":"To generate the medium-modified B-meson+b-jet cross section per binary collision, we first calculate the medium-modified b-quark+b-jet cross section as follows [ref] 1/⟨N_bin⟩ dσ^AA/dp_T^b dp_T^j = ∑_(s,s') ∫_0^1 dϵP_(s)(ϵ) 1/1-ϵ ∫_0^1 dϵ' P_(s')(ϵ') J_(s')(ϵ') dσ_(s,s')^LO+PS(p_T^b/(1-ϵ), J_(s')(ϵ') p_T^j)/dp_T^b dp_T^j,","intent_p":0.84,"contests_p":null},{"arxiv_id":"1210.4782","title":"Jet probes of QCD matter: single jets and dijets in heavy-ion collisions","url":"/paper/1210.4782","section":"Dijet productions in HIC","sentence":"Dijet spectrum in heavy ion collisions is ready to be given similarly as the inclusive jet [ref] , [equation] The two jets have symmetric final transverse momentum at leading-order.","intent_p":0.8,"contests_p":null},{"arxiv_id":"1110.6601","title":"Cold Nuclear Matter Effects on Dijet Productions in Relativistic Heavy-ion Reactions at LHC","url":"/paper/1110.6601","section":"Dijet Production in nucleon-nucleon Collisions","sentence":"To quantify the transverse momentum imbalance between the leading jet and the subleading jet one defines the dijet transverse momentum asymmetry $A_J$ as, [equation] The $A_J$ distribution can be expressed from the dijet transverse energy spectrum as follows [ref] : [equation] where $E_T 1 = E_T 2(1+A_J)/(1-A_J)$ is the transverse energy for leading jet.","intent_p":0.91,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":2,"sentences":3,"quotes":[{"arxiv_id":"1207.6558","title":"Probing nuclear matter with jets","url":"/paper/1207.6558","section":"Inclusive jet production in HIC","sentence":"Fig. [ref] illustrates the dependence of the nuclear modification factor for single jet production $R_AA^1-jet$ in central Pb+Pb collisions on the jet size $R$ with an acceptance cut without ($p_T^min=0$ GeV) and with ($p_T^min>0$ GeV) collisional energy loss [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1108.6297","title":"Jet momentum balance independent of shear viscosity","url":"/paper/1108.6297","section":"Calculating the Parton Shower Energy Deposition Rate","sentence":"Using results based on the analysis of [ref] one finds for these parameters that the probability that the primary partons initiating the dijets are two gluons is about 37$%$, the probability for two quarks is about 21$%$, and the probability for a quark and a gluon is about 42$%$.","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1210.7332","title":"D meson nuclear modification factors in Pb-Pb collisions at sqrt(s_NN) = 2.76 TeV with the ALICE detector","url":"/paper/1210.7332","section":"D meson nuclear modification factors","sentence":"We found that radiative energy loss supplemented with in-medium D meson dissociation [ref] and radiative plus collisional energy loss in the WHDG [ref] implementations, together with BDMPS-ASW [ref] and POWLANG [ref] describe the data reasonably well.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":19,"sentences":19,"quotes":[{"arxiv_id":"2304.04649","title":"Multijet topology in high-energy nuclear collisions: jet broadening","url":"/paper/2304.04649","section":"Introduction","sentence":"As the running of heavy-ion programs at the LHC with its unprecedented colliding energies, the study of parton energy loss has been extended to medium modifications of many jet observables [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1810.10007","title":"Light and heavy flavor dijet production and dijet mass modification in heavy ion collisions","url":"/paper/1810.10007","section":"Modification of dijet production","sentence":"The implementation of energy loss effects in heavy ion collisions is explained in detail in, e.g., Refs. [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"1901.04155","title":"Extracting jet transport coefficient via single hadron and dihadron productions in high-energy heavy-ion collisions","url":"/paper/1901.04155","section":"Introduction","sentence":"Phenomenological studies have been performed on various jet quenching observables, such as the nuclear modifications of single hadron productions [ref] , dihadron and photon-hadron correlations [ref] , as well as the observables related to fully reconstructed jets in relativistic nuclear collisions [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"2301.02485","title":"Hard jet substructure in a multistage approach","url":"/paper/2301.02485","section":"Introduction","sentence":"On the theory side, many studies have attempted to describe and understand the jet-medium interaction by constructing models that reproduce these various observables or propose predictions and new observables [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1603.01920","title":"Full jet evolution in quark-gluon plasma and nuclear modification of jet production and jet shape in Pb+Pb collisions at 2.76 ATeV at the LHC","url":"/paper/1603.01920","section":"Introduction","sentence":"In recent years, the experimental reconstruction of full jets with a given cone size defined as $R=√((Δϕ)^2 + (Δη)^2)$ from large fluctuating background became available in relativistic heavy-ion experiments [ref] , which has stimulated intensive theoretical interest in the study of full jets and their nuclear modification in high-energy nuclear collisions [ref] .","intent_p":0.8,"contests_p":null}]}],"unlabelled_sentences":58},"outgoing":{"papers":14,"sentences":45,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":2,"sentences":3,"quotes":[{"arxiv_id":"0910.1090","title":"Jet tomography of high-energy nucleus-nucleus collisions at next-to-leading order","url":"/paper/0910.1090","section":"Inclusive jet and di-jet production in heavy ion collisions","sentence":"We take into account the longitudinal Bjorken expansion of the medium and, by assuming local thermal equilibrium, we can evaluate the physical quantities, such as the Debye screening scale, the in-medium jet scattering cross sections, and the mean free paths [ref] , that are employed in the calculation of the radiative energy loss [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"hep-ph/0201195","title":"New Generation of Parton Distributions with Uncertainties from Global QCD Analysis","url":"/paper/hep-ph/0201195","section":"Inclusive jet and di-jet production in p+p collisions","sentence":"In the calculations that follow we will take advantage of the Ellis, Kunszt and Soper (EKS) numerical implementation of $O( α_s^3 )$ jets production in hadron-hadron collisions [ref] and the CTEQ6.1M parametrization set of parton distribution functions [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1105.2067","title":"Parton showers as sources of energy-momentum deposition in the QGP and their implication for shockwave formation at RHIC and at the LHC","url":"/paper/1105.2067","section":"Inclusive jet and di-jet production in heavy ion collisions","sentence":"Specifically, one can adjust the value of $p_T i^min$ to reflect the collisional energy loss of the parton shower $⟨δE_T ⟩$ evaluated in Ref. [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1102.1957","title":"Observation and studies of jet quenching in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV","url":"/paper/1102.1957","section":"Quenching of inclusive jets","sentence":"In central Pb+Pb collisions at the LHC, for a typical jet size $R=0.5$, on the order of 100 GeV of the jet energy is interpreted as QGP background and subtracted from the total reconstructed energy [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1101.2878","title":"Fluctuations and asymmetric jet events in PbPb collisions at the LHC","url":"/paper/1101.2878","section":"Quenching of di-jets and their $E_T$ asymmetry","sentence":"In this sense, our result is similar to the argument presented in [ref] that background fluctuations can generate much of the asymmetry observed by ATLAS and CMS.","intent_p":0.87,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":2,"sentences":4,"quotes":[{"arxiv_id":"1105.2067","title":"Parton showers as sources of energy-momentum deposition in the QGP and their implication for shockwave formation at RHIC and at the LHC","url":"/paper/1105.2067","section":"Introduction","sentence":"We find that a part of this enhancement may arise from the uncertainty in the jet/background separation and/or the dissipation of the energy from the shower into the QGP due to collisional processes [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1006.2389","title":"The physics of $Z^0/\\gamma^*$-tagged jets at the LHC","url":"/paper/1006.2389","section":"Summary and Conclusions","sentence":"The importance of reliable $O( α_s^3 )$ calculation cannot be under emphasized, since for tagged jets and di-jets an inaccurate description of the p+p baseline at LO can produce even qualitatively incorrect jet quenching predictions [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0910.1090","title":"Jet tomography of high-energy nucleus-nucleus collisions at next-to-leading order","url":"/paper/0910.1090","section":"Summary and Conclusions","sentence":"Jet production and modification in high-energy nucleus-nucleus collisions have been proposed as new ways to unravel the properties of the hot and dense QCD medium and to elucidate the mechanisms of in-medium parton shower formation [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"1006.2389","title":"The physics of $Z^0/\\gamma^*$-tagged jets at the LHC","url":"/paper/1006.2389","section":"Summary and Conclusions","sentence":"Jet production and modification in high-energy nucleus-nucleus collisions have been proposed as new ways to unravel the properties of the hot and dense QCD medium and to elucidate the mechanisms of in-medium parton shower formation [ref] .","intent_p":0.95,"contests_p":null}]}],"unlabelled_sentences":33},"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":"1105.2566","kind":"model","paper_version":2,"prompt_version":"held-up-v3.5","generated_at":"2026-10-27T20:53:22+00:00","loaded_at":"2026-10-28T01:03:58.285042+00:00","evidence":"some","account":[],"groups":[{"kind":"data_used","label":"Uses its data or values","papers":1,"entries":[{"p":0.99,"quote":null,"citing":[{"self":false,"year":2011,"title":"Jet momentum balance independent of shear viscosity","arxiv_id":"1108.6297"}],"verified":true,"paraphrase":"Used results based on this paper's analysis to find parton-initiated dijet probabilities for 120 GeV dijets in 2.76 TeV heavy-ion collisions."}],"papers_all":2,"self_papers":0,"self_entries":[]}],"counts":{"by_kind":{"data_used":2,"comparison":1,"method_or_tool":3,"supports_this_paper":1},"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":10,"self_papers":22,"citing_papers":63,"sentences_read":16,"citing_sentences":87,"unambiguous_read":16,"typed_independent":2,"independent_papers":41,"by_kind_independent":{"data_used":1,"comparison":1}},"input_sha256":"d0c7e00a68e5921b14c0c2848ab13a0a4dec5fd4e251c2a376145009cb3b3eef","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 used its data or values."},"_links":{"html":"https://pith.science/paper/1105.2566"}}