{"arxiv_id":"hep-ph/0608139","incoming":{"papers":11,"sentences":30,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0911.1856","title":"Strong decays of newly observed $D_{sJ}$ states in a constituent quark model with effective Lagrangians","url":"/paper/0911.1856","section":"$D_sJ(2|P'_1⟩_H )$, $D_sJ(2^3P_0)$ and $D_sJ(2^3P_2)$","sentence":"Taking the mass of the $D_sJ(2^3P_0)$ as $(2.82∼2.84)$ GeV [ref] , the total width and branching ratio fractions between $D_sη$ and $DK$ are [equation]","intent_p":0.96,"contests_p":null},{"arxiv_id":"0803.2102","title":"Strong decays of heavy-light mesons in a chiral quark model","url":"/paper/0803.2102","section":"Radially excited $D_s$ mesons","sentence":"By fixing the masses of $2^1S_0$ and $2^3S_1$ states as suggested by the quark model [ref] , i.e. $m(D_s(2^1S_0))=2.64$ GeV and $m(D_s(2^3S_1))=2.71$ GeV, we obtain their strong decay widths [equation] which turn out to be narrow.","intent_p":0.93,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":2,"quotes":[{"arxiv_id":"0911.1856","title":"Strong decays of newly observed $D_{sJ}$ states in a constituent quark model with effective Lagrangians","url":"/paper/0911.1856","section":"$D_sJ(2710)$","sentence":"The above mixing scheme is consistent with Ref. [ref] for the low-mass state while the predicted suppression of the $D^*K$ decay mode is different from that of Ref. [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0911.2906","title":"Implication of BaBar's new data on the $D_{s1}(2710)$ and $D_{sJ}(2860)$","url":"/paper/0911.2906","section":"I. Introduction","sentence":"Therefore, the observed $D_s1(2710)$ is most likely a mixture of the $D_s(2 ^3S_1)$ and $D_s(1 ^3D_1)$ [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":7,"sentences":10,"quotes":[{"arxiv_id":"0908.1142","title":"Comment on \"Study of D(sJ) decays to D(*)K in inclusive e(+)e(-) interactions\"","url":"/paper/0908.1142","section":"Introduction","sentence":"When the $D_sJ^∗(2860)^+$ meson was discovered by [ref] , only the $DK$ decay mode was detected, which made an assignment as a radially excited scalar $cs̅$ meson plausible [ref] , though other configurations such as a $3^-$ state [ref] could not be excluded.","intent_p":0.86,"contests_p":null},{"arxiv_id":"0911.2906","title":"Implication of BaBar's new data on the $D_{s1}(2710)$ and $D_{sJ}(2860)$","url":"/paper/0911.2906","section":"I. Introduction","sentence":"In the pure $S$-wave or $D$-wave $cs̅$ picture, the decay properties of the $D_s1(2710)$ and $D_sJ(2860)$ have been studied for several different quantum numbers using various approaches [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"0909.1658","title":"Newly observed D_{sJ}(3040) and the radial excitations of P-wave charmed-strange mesons","url":"/paper/0909.1658","section":"Introduction","sentence":"A series of theoretical work [ref] relevant to $D_s1^*(2710)$ and $D_sJ^*(2860)$ were carried out.","intent_p":0.86,"contests_p":null},{"arxiv_id":"2501.14386","title":"Can one-loop corrections to the one-gluon exchange potential adequately describe the charmed meson spectrum?","url":"/paper/2501.14386","section":"INTRODUCTION","sentence":"In the last years, many studies have been carried out within different theoretical approaches such as lattice-regularized QCD [ref] , unitarized coupled-channels $T$-matrix analyses [ref] , heavy meson effective theory [ref] , Regge-based phenomenology [ref] and phenomenological quark models [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"0911.1856","title":"Strong decays of newly observed $D_{sJ}$ states in a constituent quark model with effective Lagrangians","url":"/paper/0911.1856","section":"$D_sJ(2710)$","sentence":"This state is studied by various models, e.g. as a $2^3S_1$ state [ref] , $1^3D_1$ state [ref] , or admixture of $2^3S_1$-$1^3D_1$ [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":15},"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/0608139"}}