{"arxiv_id":"2501.16406","incoming":{"papers":1,"sentences":1,"groups":[],"unlabelled_sentences":1},"outgoing":{"papers":51,"sentences":151,"groups":[{"kind":"contests","label":"Contests","papers":4,"sentences":5,"quotes":[{"arxiv_id":"1903.00860","title":"Semileptonic $D_{(s)} \\to A \\ell^+ \\nu$ and nonleptonic $D\\to K_1(1270,1400) \\pi$ decays in LCSR","url":"/paper/1903.00860","section":"RESULTS AND DISCUSSION","sentence":"Again for the $D_s^+→K_1(1270)^0e^+ν_e$ decay Ref. [ref] predicts the value which is about a factor of 4 higher than experimental limit, while our result and other theoretical predictions [ref] are well consistent with this upper bound.","intent_p":0.78,"contests_p":0.82},{"arxiv_id":"2404.03857","title":"Study of the axial-vector and tensor resonant contributions to the $D \\to VP\\ell^+\\nu_\\ell$ decays based on SU(3) flavor analysis","url":"/paper/2404.03857","section":"RESULTS AND DISCUSSION","sentence":"Again for the $D_s^+→K_1(1270)^0e^+ν_e$ decay Ref. [ref] predicts the value which is about a factor of 4 higher than experimental limit, while our result and other theoretical predictions [ref] are well consistent with this upper bound.","intent_p":0.78,"contests_p":0.82},{"arxiv_id":"1707.02851","title":"Branching fractions of semileptonic $D$ and $D_s$ decays from the covariant light-front quark model","url":"/paper/1707.02851","section":"RESULTS AND DISCUSSION","sentence":"Again for the $D_s^+→K_1(1270)^0e^+ν_e$ decay Ref. [ref] predicts the value which is about a factor of 4 higher than experimental limit, while our result and other theoretical predictions [ref] are well consistent with this upper bound.","intent_p":0.78,"contests_p":0.82},{"arxiv_id":"0812.1352","title":"Semileptonic $D_{q}\\to K_{1}\\ell \\nu$ and nonleptonic $D\\to K_1 \\pi$ decays in three--point QCD sum rules and factorization approach","url":"/paper/0812.1352","section":"RESULTS AND DISCUSSION","sentence":"Again for the $D_s^+→K_1(1270)^0e^+ν_e$ decay Ref. 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[ref] and very recently semimuonic ones were reported in Ref. [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"1907.11370","title":null,"url":"/paper/1907.11370","section":"INTRODUCTION","sentence":"The branching fractions of the semielectronic $D$ decays into the axial-vector $K_1(1270)$ meson were measured in Refs. [ref] and very recently semimuonic ones were reported in Ref. [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2502.03828","title":null,"url":"/paper/2502.03828","section":"INTRODUCTION","sentence":"The branching fractions of the semielectronic $D$ decays into the axial-vector $K_1(1270)$ meson were measured in Refs. [ref] and very recently semimuonic ones were reported in Ref. [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"0910.5612","title":"Heavy-light meson spectroscopy and Regge trajectories in the relativistic quark model","url":"/paper/0910.5612","section":"Conclusion","sentence":"These wave functions are known from the previous calculations of the meson mass spectra [ref] .","intent_p":0.84,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":18,"sentences":48,"quotes":[{"arxiv_id":"hep-ph/0509103","title":"Semileptonic Decay of $B$ and $D\\to K^*_0(1430) \\bar{\\ell}\\nu$ From QCD Sum Rule","url":"/paper/hep-ph/0509103","section":"INTRODUCTION","sentence":"We compare our results with available experimental data [ref] and previous predictions [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"0705.4276","title":"Evidence for the Decay D^0 --> K^_pi^+pi^-e^+nu_e","url":"/paper/0705.4276","section":"INTRODUCTION","sentence":"We compare our results with available experimental data [ref] and previous predictions [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"0812.1352","title":"Semileptonic $D_{q}\\to K_{1}\\ell \\nu$ and nonleptonic $D\\to K_1 \\pi$ decays in three--point QCD sum rules and factorization approach","url":"/paper/0812.1352","section":"INTRODUCTION","sentence":"We compare our results with available experimental data [ref] and previous predictions [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1608.03651","title":"$D \\rightarrow a_1, f_1$ transition form factors and semileptonic decays via 3-point QCD sum rules","url":"/paper/1608.03651","section":"INTRODUCTION","sentence":"We compare our results with available experimental data [ref] and previous predictions [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1707.02851","title":"Branching fractions of semileptonic $D$ and $D_s$ decays from the covariant light-front quark model","url":"/paper/1707.02851","section":"INTRODUCTION","sentence":"We compare our results with available experimental data [ref] and previous predictions [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":15,"sentences":16,"quotes":[{"arxiv_id":"0910.5612","title":"Heavy-light meson spectroscopy and Regge trajectories in the relativistic quark model","url":"/paper/0910.5612","section":"Masses and wave functions of excited light and strange mesons","sentence":"The spectroscopy of heavy-light and light mesons was discussed in detail in Refs. [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"0903.5183","title":"Mass spectra and Regge trajectories of light mesons in the relativistic quark model","url":"/paper/0903.5183","section":"Masses and wave functions of excited light and strange mesons","sentence":"The spectroscopy of heavy-light and light mesons was discussed in detail in Refs. 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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/2501.16406"}}