{"arxiv_id":"hep-ph/9409309","incoming":{"papers":10,"sentences":17,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2604.01782","title":"Exclusive semileptonic and nonleptonic $J/\\psi$ decays","url":"/paper/2604.01782","section":"INTRODUCTION","sentence":"Therefore, for the description of such processes, we use the approximation of the infinite number of colors ($N_c→∞$) proposed in Ref [ref] .","intent_p":0.87,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":4,"sentences":5,"quotes":[{"arxiv_id":"2302.03312","title":"A combined study of hadronic $D^+\\to K^-\\pi^+\\pi^+$ and $D_s^+\\to K^+K^+\\pi^-$ decays by means of the analysis of semileptonic $D^+\\to K^-\\pi^+ \\ell^+\\nu_\\ell$ decays","url":"/paper/2302.03312","section":"Naïve factorization in decays","sentence":"Theoretically, Ref. [ref] obtained $a_1=1.31(19)$ and $a_2$ ranging between $-0.55(15)$ and $-0.60(22)$, depending on the chosen renormalization scheme.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1003.5232","title":"K pi form factors, final state interactions and D+ -> K- pi+ pi+ decays","url":"/paper/1003.5232","section":"Theoretical framework","sentence":"For the QCD factors $a_1,2$ we use the phenomenological values $a_1=1.2±0.1$ and $a_2=-0.5±0.1$, obtained from different analyses of two-body $D$ meson decays [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"0907.0189","title":"Kpi form factors and final state interactions in D+ --> K- pi+ pi+ decays","url":"/paper/0907.0189","section":"Theoretical framework","sentence":"For these factors we use the phenomenological values [equation] obtained from different analyses of two-body $D$ meson decays [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"2109.04950","title":"Using $B^0_s\\to D_s^\\mp K^\\pm$ Decays as a Portal to New Physics","url":"/paper/2109.04950","section":"Factorisation","sentence":"As a reference point, we shall use the following range: [equation] For the uncertainty, we use the picture arising from the QCD renormalisation group analysis in Ref. [ref] as guidance, where $a_1=1.01±0.02$ is found for the global factorisation parameter $a_1$ for color-allowed decays, varying the QCD dimensional transmutation parameter and renormalisation scale within their allowed ranges.","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1505.01361","title":"Anatomy of $B\\rightarrow D\\bar{D}$ Decays","url":"/paper/1505.01361","section":"Information from Semileptonic Decays","sentence":"In naive factorisation, $a_NF^(q)=a_1$, where $a_1$ represents the appropriate combination of Wilson coefficient functions of the current-current operators[For a detailed discussion, see Ref. [ref] .].","intent_p":0.84,"contests_p":null}]}],"unlabelled_sentences":10},"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/hep-ph/9409309"}}