{"arxiv_id":"1207.1769","incoming":{"papers":24,"sentences":28,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":9,"sentences":9,"quotes":[{"arxiv_id":"1304.4063","title":"Decoherence free Bd and Bs meson systems","url":"/paper/1304.4063","section":"Decoherence parameter $ζ_s$ for $B_s$ system","sentence":"The values of $A^s_sl$ in the first and second row of Table [ref] are obtained by DØ [ref] and LHCb [ref] collaborations, respectively, by measuring the time-integrated charge asymmetry of untagged $B_s →D_s μ X$ decays.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1207.4483","title":"On the origin of the D0 like-sign dimuon charge asymmetry","url":"/paper/1207.4483","section":"Introduction","sentence":"On the other hand, recent measurements of CP violation in wrong sign semileptonic $B_s$ decays from the LHCb and DØ collaborations [ref] a^s_sl=(-1.08±0.72±0.17)% [DØ] , a^s_sl=(-0.24±0.54±0.33)% [LHCb] ,","intent_p":0.82,"contests_p":null},{"arxiv_id":"1210.5076","title":"B decay anomalies in an effective theory","url":"/paper/1210.5076","section":"The like-sign dimuon asymmetry","sentence":"Recently, the DØ Collaboration directly measured $a^s_fs = (-1.08 ±0.72 (stat) ±0.17 (syst))×10^-2$ [ref] which is also consistent with the SM expectation.","intent_p":0.93,"contests_p":null},{"arxiv_id":"2111.04478","title":"Testing the Standard Model with CP-asymmetries in flavour-specific non-leptonic decays","url":"/paper/2111.04478","section":"$A_fs^q$ within the SM","sentence":"The latest world averages [ref] , based mainly on the results of Refs. [ref] , are [equation] The experimental precision for these quantities is expected to increase considerably.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1404.2531","title":"On new physics in $\\Delta \\Gamma_d$","url":"/paper/1404.2531","section":"Mixing formalism","sentence":"We therefore quote in Table [ref] separately the direct measurements in semi-leptonic decays from BaBar [ref] , DØ [ref] and LHCb [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1412.5211","title":"Review of Physics Results from the Tevatron: Heavy Flavor Physics","url":"/paper/1412.5211","section":"CP violation in $B$ mixing","sentence":"The results are consistent with the independent 0̣ measurements [ref] of $a^d_sl$ and $a^s_sl$ described above, and the combination of all 0̣ results are also shown in Fig. [ref](b).","intent_p":0.95,"contests_p":null},{"arxiv_id":"1605.09768","title":"Measurement of the $CP$ asymmetry in $B_s^0-\\overline{B}{}_s^0$ mixing","url":"/paper/1605.09768","section":"Introduction","sentence":"Figure [ref] displays an overview of the most precise measurements of and [ref] .","intent_p":0.84,"contests_p":null}]}],"unlabelled_sentences":17},"outgoing":{"papers":4,"sentences":9,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1208.5813","title":"Measurement of the semileptonic charge asymmetry in B0 meson mixing with the D0 detector","url":"/paper/1208.5813","section":"Introduction","sentence":"These corrections are described in detail in Ref. [ref] .","intent_p":0.94,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":3,"sentences":5,"quotes":[{"arxiv_id":"1202.4717","title":"Determination of the sign of the decay width difference in the B_s system","url":"/paper/1202.4717","section":"Introduction","sentence":"To correct for these differences, a correction is applied to all non-prompt events in simulation, based on the generated lifetime of the $B$ candidate, to give the appropriate world-average $B$ meson lifetimes and measured value of the width difference $ΔΓ_s$ [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1102.4274","title":"Numerical updates of lifetimes and mixing parameters of B mesons","url":"/paper/1102.4274","section":"Introduction","sentence":"The value of the SM prediction for $= (1.9 ±0.3) ×10^-5$ [ref] is negligible compared with current experimental precision.","intent_p":0.92,"contests_p":null},{"arxiv_id":"1010.1589","title":"Averages of b-hadron, c-hadron, and tau-lepton Properties","url":"/paper/1010.1589","section":"Introduction","sentence":"To estimate the effects of trigger selection and track reconstruction, we weight each event as a function of $p_T$ of the reconstructed muon so that it matches the distribution in the data, and as a function of the lifetime to ensure that the $B$-meson lifetimes and $ΔΓ_s$ match the world-average [ref] .","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":3},"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/1207.1769"}}