{"arxiv_id":"1208.0204","incoming":{"papers":16,"sentences":61,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1405.5861","title":"Phenomenology of charmed mesons in the extended Linear Sigma Model","url":"/paper/1405.5861","section":"The Lagrangian of the eLSM for $N_f=4$","sentence":"In this section we extend the eLSM [ref] to the four-flavor case.","intent_p":1.0,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1608.06569","title":"Dynamical generation of hadronic resonances in effective models with derivative interactions","url":"/paper/1608.06569","section":"Deutsche Zusammenfassung","sentence":"Hierzu wurden durch das sogenannte “erweiterte Lineare Sigma Modell” (eLSM) [ref] inspirierte effektive Theorien mit derivativen Kopplungen eingesetzt, um den eingangs erwähnten Isovektor $a_0(980)$ und das Isodoublet $K_0^∗(800)$ (auch $κ$ genannt) zu beschreiben.","intent_p":0.81,"contests_p":null},{"arxiv_id":"1208.2054","title":"Phenomenology of Axial-Vector Mesons from an Extended Linear Sigma Model","url":"/paper/1208.2054","section":"The Model","sentence":"We then observe that mixing terms containing axial-vectors and pseudoscalars and $K^⋆$ and $K_0^⋆$ arise in the Lagrangian; these are removed as described in Refs. [ref] .","intent_p":0.93,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1501.07906","title":"Glueball Decay Rates in the Witten-Sakai-Sugimoto Model","url":"/paper/1501.07906","section":"Glueball decay to two pions","sentence":"The experimental results for the decay width into two pions are Γ^(ex)(f_0(1500)→ππ)/(1505MeV)=0.025(3), Γ^(ex)(f_0(1710)→ππ)/(1722MeV)= {0.017(4) 0.009(2) . where the first result is taken from Ref. , the second from Ref. [ref] using data from the BES collaboration [ref] (upper entry) and the WA102 collaboration [ref] (lower entry), respectively.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1503.00550","title":"Scalar Glueball in a Top-Down Holographic Approach to QCD","url":"/paper/1503.00550","section":"The Model and Its Implications","sentence":"Experimental data imply $Γ_f_0(1500) →ππ/M_f_0(1500) = 0.025 ±0.003$ [ref] and $Γ_f_0(1710) →ππ/M_f_0(1710) ≃0.009$ – $0.017$ [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1608.06569","title":"Dynamical generation of hadronic resonances in effective models with derivative interactions","url":"/paper/1608.06569","section":"Some words on the scalar isodoublet resonances","sentence":"The final values for the resonance above $1$ GeV have been given as $m_K_0^∗=1.450±0.001$ GeV and $Γ=0.285±0.012$ GeV [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1312.2830","title":"Mesons, PANDA and the scalar glueball","url":"/paper/1312.2830","section":"The scalar glueball","sentence":"* The $f_0(1710)$ resonance decays predominantly into kaons and the pion decay is suppressed; the ratio $Γ_f_0(1710)→ππ / Γ_f_0(1710)→KK ≃(0.2 - 0.4)$, depending on collaboration [ref] .","intent_p":0.93,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1608.06569","title":"Dynamical generation of hadronic resonances in effective models with derivative interactions","url":"/paper/1608.06569","section":"Comparison to the eLSM","sentence":"Furthermore, the branching ratios of the eLSM are [ref] [equation] which differ from ours, see Eq. ([ref]).","intent_p":0.91,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":3,"sentences":5,"quotes":[{"arxiv_id":"1208.0585","title":"Meson vacuum phenomenology in a three-flavor linear sigma model with (axial-)vector mesons","url":"/paper/1208.0585","section":"INTRODUCTION","sentence":"Detailed calculations of all formulas used in this paper as well as further discussion are presented in Ref. [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"1608.06569","title":"Dynamical generation of hadronic resonances in effective models with derivative interactions","url":"/paper/1608.06569","section":"Some words on the scalar–isovector resonances","sentence":"A possible identification of the scalar states in the context of the eLSM was put forward in Refs. [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1508.06928","title":"Functional Renormalization Group Study of the Chiral Phase Transition Including Vector and Axial-vector Mesons","url":"/paper/1508.06928","section":"Extended Linear Sigma Model","sentence":"We work with a mesonic linear sigma model [ref] as an effective implementation of the strong interaction, which, besides scalar and pseudoscalar mesons, also includes vector and axial-vector mesons [ref] : the so-called eLSM [ref] .","intent_p":0.88,"contests_p":null}]}],"unlabelled_sentences":48},"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":null,"_links":{"html":"https://pith.science/paper/1208.0204"}}