{"arxiv_id":"hep-ph/0406080","incoming":{"papers":34,"sentences":52,"groups":[{"kind":"contests","label":"Contests it","papers":4,"sentences":4,"quotes":[{"arxiv_id":"2504.06043","title":"Hadronic molecules and multiquark states","url":"/paper/2504.06043","section":"Hadronic Molecules","sentence":"Thus, the total rate of this transition cannot be sensitive to the molecular component of the $X(3872)$ [ref] in a model independent way, contrary to what is claimed, e.g., in Refs. [ref] .","intent_p":0.98,"contests_p":0.83},{"arxiv_id":"2603.09315","title":"Exotic hadrons associated with $b$-quark","url":"/paper/2603.09315","section":"Radiative decays of $$","sentence":"Thus, the estimates of the ratio $R_X^mol≪1$ in Refs. [ref] , based on the overlap of the molecular $$ wave function, do not apply to the studied case and as such can not be regarded as decisive (see also a detailed discussion in Ref. [ref] ).","intent_p":0.59,"contests_p":0.83},{"arxiv_id":"2212.12893","title":"The $X(3872)\\rightarrow J/\\psi \\pi \\gamma$ and $X(3872)\\rightarrow J/\\psi \\pi\\pi \\gamma$ decays","url":"/paper/2212.12893","section":"Introduction","sentence":"* The ratio $Γ(B^0→K^0 X)/Γ(B^+→K^+ X)$ is about unity according to an estimation based on the molecule picture [ref] , which is about two times larger than measurements by the BaBar [ref] and Belle [ref] Collaborations. * The predicted branching ratios of $X(3872)→D^0 D̅^0 γ$ and $X(3872)→J/ψγ$ [ref] largely deviated from the experimental data. * As a loosely bound hadronic molecule with a small binding energy, $X(3872)$ was expected to be so fragile that it would be hard to explain the observed production rate in the high energy $pp̅$ collisions at the Tevatron [ref] .","intent_p":0.32,"contests_p":0.82},{"arxiv_id":"1106.2968","title":"$Z_b(10610)^\\pm$ and $Z_b(10650)^\\pm$ as the $B^*\\bar{B}$ and $B^*\\bar{B}^{*}$ molecular states","url":"/paper/1106.2968","section":"The $BB̅^*$ and $DD̅^*$ systems","sentence":"The BaBar Collaboration measured the radiative decay of $X(3872)$ and found a ratio of $B(X(3872)→ψ(2S)γ)/B(X(3872)→J/ψγ)=3.4±1.4$ [ref] , which contradicts the prediction with a purely $DD̅^*$ molecular assignment to $X(3872)$ [ref] .","intent_p":0.52,"contests_p":0.77}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1812.08207","title":"QCD Sum Rules Approach to the $X,~Y$ and $Z$ States","url":"/paper/1812.08207","section":"The X(3872) state","sentence":"For example, in Ref. [ref] , the molecular model gives rise to a suppression of the $γ ψ(2S)$ channel, providing: $Γ(X →ψ(2S) γ)Γ(X→ψγ)∼4×10^-3$.","intent_p":0.83,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":2,"quotes":[{"arxiv_id":"2207.01101","title":"Diabatic Representation of Exotic Hadrons in the Dynamical Diquark Model","url":"/paper/2207.01101","section":"$$ Sector","sentence":"We note that the results of Eqs. ([ref]) are comparable to the predictions of 71 keV and 95 keV, respectively, from Ref. [ref] [which also uses Eq. ([ref]), but with somewhat different numerical values for the matrix elements].","intent_p":1.0,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2212.12893","title":"The $X(3872)\\rightarrow J/\\psi \\pi \\gamma$ and $X(3872)\\rightarrow J/\\psi \\pi\\pi \\gamma$ decays","url":"/paper/2212.12893","section":"Introduction","sentence":"The molecule picture not only explains the coincidence of the mass of the $X(3872)$ with the $D^0 D̅^*0$ threshold naturally, but also explains its isospin violation in the $J/ψρ$ decay mode [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":6,"sentences":6,"quotes":[{"arxiv_id":"2207.08563","title":"Establishing the heavy quark spin and light flavor molecular multiplets of the $X(3872)$, $Z_c(3900)$ and $X(3960)$","url":"/paper/2207.08563","section":"Introduction","sentence":"The $X(3872)$ [ref] , also known as $χ_c1(3872)$, and the $Z_c(3900)$ [ref] have been proposed as candidates of isoscalar and isovector $DD̅^*$ hadronic molecules, respectively, since long [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1010.3607","title":"Strong and radiative decays of X(3872) as a hadronic molecule with a negative parity","url":"/paper/1010.3607","section":"Introduction","sentence":"In the literature, $X(3872)$ has been interpreted as a $cc̅g$ hybrid state [ref] , a diquark-antidiquark state [ref] , a $cc̅$ and meson cloudy mixing state [ref] or a deuteron-like molecular state concerning its mass is approximate to the threshold of $D^0D^∗ 0$ [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1005.2167","title":"Using Line Shapes to Discriminate between Binding Mechanisms for the X(3872)","url":"/paper/1005.2167","section":"Charm meson scattering parameters","sentence":"More elaborate meson potential models include the effects of the exchange of other mesons [ref] or the exchange of quarks [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1104.3974","title":"One-photon decay of the tetraquark state $X(3872) \\to \\gamma + J/\\psi$ in a relativistic constituent quark model with infrared confinement","url":"/paper/1104.3974","section":"Introduction","sentence":"Some tests of the hypothesis that the $X(3872)$ is a weakly bound $D^0D̅^0*$ molecule state were suggested in [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1404.0275","title":"Evidence for the decay $X(3872)\\rightarrow\\psi(2S)\\gamma$","url":"/paper/1404.0275","section":"Introduction","sentence":"In particular for the state, interpretation as a $$ molecule [ref] , tetraquark [ref] , $$ hybrid meson [ref] , vector glueball [ref] or mixed are proposed.","intent_p":0.96,"contests_p":null}]}],"unlabelled_sentences":38},"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/0406080"}}