{"arxiv_id":"1006.1682","incoming":{"papers":21,"sentences":26,"groups":[{"kind":"contests","label":"Contests it","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1008.4445","title":"TeV scale horizontal gauge symmetry and its implications in B-physics","url":"/paper/1008.4445","section":"Meson Mixing","sentence":"In contrast to the paper [ref] , it is clearly that from the upper right plot in FIG [ref], there is no region allowed by all experimental constraints within the 1 $σ$ [We notice that in [ref] , they use SM prediction directly from [ref] which use the old decay constants and bag parameters.","intent_p":0.76,"contests_p":0.83}]},{"kind":"background","label":"Cites it as background","papers":7,"sentences":7,"quotes":[{"arxiv_id":"1105.0970","title":"Reconciling anomalous measurements in $B_s-\\bar{B}_s$ mixing: the role of CPT-conserving and CPT-violating new physics","url":"/paper/1105.0970","section":"Introduction","sentence":"The resolutions of the above anomalies, separately or simultaneously, have been discussed in the context of specific NP models: a scalar leptoquark model [ref] , models with an extra flavor-changing neutral gauge boson $Z'$ or R-parity violating supersymmetry [ref] , two-Higgs doublet model [ref] , models with a fourth generation of fermions [ref] , supersymmetric grand unified models [ref] , supersymmetric models with split sfermion generations [ref] or models with a very light spin-1 particle [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1010.5123","title":"The D0 same-charge dimuon asymmetry and possibile new CP violation sources in the $B_s-\\bar{B}_s$ system","url":"/paper/1010.5123","section":"Introduction","sentence":"The D0 result has attracted a great deal of attention by introducing new TeV scale particles, such as the leptoquark models [ref] , the MSSM with non-minimal flavor violation [ref] , an $R$-parity violating supersymmetric model [ref] , a split SUSY model [ref] , $Z'$ models [ref] , a fourth generation model [ref] , additional right-handed currents [ref] , an additional SM SU(2)$_L$ doublet scalar not developing a vacuum expectation value (VEV) [ref] , and an extra SUSY Higgs doublet [ref] , etc [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"1104.4127","title":"An Effective Z'","url":"/paper/1104.4127","section":"Like-sign dimuon asymmetry","sentence":"The possibility of using flavor-violating $Z'$s to address $B$-physics anomalies been considered in [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1103.5705","title":"Like-sign dimuon asymmetry of B0 meson and LFV in SU(5) SUSY GUT with S4 flavor symmetry","url":"/paper/1103.5705","section":"Introduction","sentence":"As a possibility, new physics contribute to decay width of the $B_s$ meson [ref] - [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"1006.5331","title":"The like-sign dimuon charge asymmetry in SUSY models","url":"/paper/1006.5331","section":"Introduction","sentence":"The dimuon asymmetry has already been investigated in the context of generic new physics [ref] and specific new physics models, for example models with flavour changing neutral Higgs [ref] , flavour changing $Z'$ [ref] , or Axigluons [ref] (see also [ref] ).","intent_p":0.99,"contests_p":null}]}],"unlabelled_sentences":17},"outgoing":{"papers":19,"sentences":48,"groups":[{"kind":"data_used","label":"Uses data or values from","papers":5,"sentences":6,"quotes":[{"arxiv_id":"0808.1297","title":"Averages of b-hadron and c-hadron Properties at the End of 2007","url":"/paper/0808.1297","section":"Introduction","sentence":"Using the current experimental value [ref] $a_sl^d = -0.0047±0.0046$ which is consistent with zero and also with the SM prediction [ref] $a^d_sl = (-4.8^+1.0_-1.2)×10^-4$ within errors, one requires [ref] [equation] to obtain the D0 value of $A^b_sl$.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1005.2757","title":"Evidence for an anomalous like-sign dimuon charge asymmetry","url":"/paper/1005.2757","section":"Introduction","sentence":"Using the current experimental value [ref] $a_sl^d = -0.0047±0.0046$ which is consistent with zero and also with the SM prediction [ref] $a^d_sl = (-4.8^+1.0_-1.2)×10^-4$ within errors, one requires [ref] [equation] to obtain the D0 value of $A^b_sl$.","intent_p":0.98,"contests_p":null},{"arxiv_id":"0904.3907","title":"Search for CP violation in semileptonic Bs decays","url":"/paper/0904.3907","section":"Introduction","sentence":"D0 [ref] also performed a direct measurement of $a^s_sl$, but the result does not show any deviation from the SM, although the error bars are quite large: $a_sl^s = - 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[ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"1005.5310","title":"Higgs-mediated FCNCs: Natural Flavour Conservation vs. Minimal Flavour Violation","url":"/paper/1005.5310","section":"Introduction","sentence":"Several theoretical attempts to explain the data have been made [ref] .","intent_p":0.82,"contests_p":null}]}],"unlabelled_sentences":29},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"1008.5277","url":"/paper/1008.5277","title":"The D0 Dimuon Charge Asymmetry and Baryon Asymmetry of the Universe","main_claim":"New physics beyond the SM in B_s - \\bar B_s mixing is needed to explain the data.","p":0.95}]}],"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/1006.1682"}}