{"arxiv_id":"1604.07598","incoming":{"papers":8,"sentences":10,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1602.04020","title":"Universal Unitarity Triangle 2016 and the Tension Between $\\Delta M_{s,d}$ and $\\varepsilon_K$ in CMFV Models","url":"/paper/1602.04020","section":"Determination of the UUT","sentence":"The inclusive ones are summarized well in [ref] . _incl=(42.21±0.78)·10^-3, _incl=(4.40±0.25)·10^-3.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1604.02344","title":"331 Models Facing the Tensions in $\\Delta F=2$ Processes with the Impact on $\\varepsilon^\\prime/\\varepsilon$, $B_s\\to\\mu^+\\mu^-$ and $B\\to K^*\\mu^+\\mu^-$","url":"/paper/1604.02344","section":"Numerical Analysis","sentence":"The inclusive ones are summarized well in [ref] _incl=(42.21±0.78)·10^-3, _incl=(4.40±0.25)·10^-3.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1812.00065","title":"Selected updates on semileptonic $B$ decays and $|V_{xb}|$ determination","url":"/paper/1812.00065","section":"Inclusive $|V_ub|$ determination","sentence":"The latest analyses and theoretical progresses in semi-leptonic heavy to light decays involve power corrections [ref] , global fits to inclusive rare and semileptonic data [ref] and, most recently, exploratory lattice calculations of inclusive B meson semileptonic decay [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"2102.00020","title":"Measurements of Partial Branching Fractions of Inclusive $B \\to X_u \\, \\ell^+\\, \\nu_{\\ell}$ Decays with Hadronic Tagging","url":"/paper/2102.00020","section":"introduction","sentence":"In the future, more model-independent approaches aim to directly measure the leading-order shape function [ref] .","intent_p":0.82,"contests_p":null}]}],"unlabelled_sentences":6},"outgoing":{"papers":28,"sentences":53,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":3,"sentences":7,"quotes":[{"arxiv_id":"0707.2493","title":"Inclusive semileptonic B decays and the determination of |V_ub|","url":"/paper/0707.2493","section":"Distribution Functions in $B →X_u ℓν̅_ℓ$","sentence":"At higher $q^2$ the rate must be modelled and we employ the second method described in Sec. 5 of Ref. [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1307.4551","title":"Inclusive semileptonic fits, heavy quark masses, and V_cb","url":"/paper/1307.4551","section":"Results and discussion","sentence":"The theoretical correlation between different $q^2$ bins is estimated with method C in Sec. 3 of [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1012.0836","title":"Reweighting NNPDFs: the W lepton asymmetry","url":"/paper/1012.0836","section":"Results and discussion","sentence":"Indeed, one can reweight the NN replicas using their $χ^2_X$, giving more importance to the replicas whose $M_X$ spectrum is closer to the experimental one and therefore have lower $χ^2_X$, see [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":2,"sentences":4,"quotes":[{"arxiv_id":"0707.2493","title":"Inclusive semileptonic B decays and the determination of |V_ub|","url":"/paper/0707.2493","section":"Introduction","sentence":"In the GGOU approach [ref] it reads |V_ub|_incl=(4.51±0.16^+0.12_-0.15)×10^-4 and very close values are found with the other methods.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1411.6560","title":"Precision determination of the CKM element Vcb","url":"/paper/1411.6560","section":"Results and discussion","sentence":"The OPE parameters are taken from [ref] and the theoretical uncertainties of the $F_i$ moments are estimated as in that paper.","intent_p":0.85,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":4,"sentences":6,"quotes":[{"arxiv_id":"0707.2493","title":"Inclusive semileptonic B decays and the determination of |V_ub|","url":"/paper/0707.2493","section":"Results and discussion","sentence":"As a first step, we train the NN on the moments only and compare with the functional form error found in [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1412.7515","title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of summer 2014","url":"/paper/1412.7515","section":"Results and discussion","sentence":"As we adopt up-to-date inputs, we can extract $|V_ub|$ from the latest experimental results and compare the results with the most recent HFAG compilation [ref] ; this is done in Table 1 for the most representative cases, using the isospin average $τ_B=1.582(5)$ps, employed in the derivation of the HFAG values.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1501.05373","title":"$B \\to \\pi \\ell \\nu$ and $B_s \\to K \\ell \\nu$ form factors and $|V_{ub}|$ from 2+1-flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks","url":"/paper/1501.05373","section":"Results and discussion","sentence":"On the other hand, the values reported in the first three rows of Table 1 are consistent with the recent exclusive $|V_ub|$ results given in [ref] and [ref] within 1.5$σ$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1503.07839","title":"$|V_{ub}|$ from $B\\to\\pi\\ell\\nu$ decays and (2+1)-flavor lattice QCD","url":"/paper/1503.07839","section":"Results and discussion","sentence":"On the other hand, the values reported in the first three rows of Table 1 are consistent with the recent exclusive $|V_ub|$ results given in [ref] and [ref] within 1.5$σ$.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":14,"sentences":14,"quotes":[{"arxiv_id":"1409.7816","title":"Extrapolation and unitarity bounds for the $B \\to \\pi$ form factor","url":"/paper/1409.7816","section":"Introduction","sentence":"The precise determination of the CKM matrix element $V_ub$ remains an important goal in flavour physics, instrumental in performing stringent tests of the CKM matrix unitarity, see [ref] for a review. $|V_ub|$ can be extracted from $b→u ℓν$ decays, and in in particular from $B→πℓν$, using lattice QCD [ref] or light-cone sum rules [ref] calculations of the relevant form factors.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1203.1359","title":"Two-loop Corrections to the B to pi Form Factor from QCD Sum Rules on the Light-Cone and |V(ub)|","url":"/paper/1203.1359","section":"Introduction","sentence":"The precise determination of the CKM matrix element $V_ub$ remains an important goal in flavour physics, instrumental in performing stringent tests of the CKM matrix unitarity, see [ref] for a review. $|V_ub|$ can be extracted from $b→u ℓν$ decays, and in in particular from $B→πℓν$, using lattice QCD [ref] or light-cone sum rules [ref] calculations of the relevant form factors.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1503.07839","title":"$|V_{ub}|$ from $B\\to\\pi\\ell\\nu$ decays and (2+1)-flavor lattice QCD","url":"/paper/1503.07839","section":"Introduction","sentence":"The precise determination of the CKM matrix element $V_ub$ remains an important goal in flavour physics, instrumental in performing stringent tests of the CKM matrix unitarity, see [ref] for a review. $|V_ub|$ can be extracted from $b→u ℓν$ decays, and in in particular from $B→πℓν$, using lattice QCD [ref] or light-cone sum rules [ref] calculations of the relevant form factors.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1501.05373","title":"$B \\to \\pi \\ell \\nu$ and $B_s \\to K \\ell \\nu$ form factors and $|V_{ub}|$ from 2+1-flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks","url":"/paper/1501.05373","section":"Introduction","sentence":"The precise determination of the CKM matrix element $V_ub$ remains an important goal in flavour physics, instrumental in performing stringent tests of the CKM matrix unitarity, see [ref] for a review. $|V_ub|$ can be extracted from $b→u ℓν$ decays, and in in particular from $B→πℓν$, using lattice QCD [ref] or light-cone sum rules [ref] calculations of the relevant form factors.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1406.6311","title":"The Physics of the B Factories","url":"/paper/1406.6311","section":"Introduction","sentence":"The precise determination of the CKM matrix element $V_ub$ remains an important goal in flavour physics, instrumental in performing stringent tests of the CKM matrix unitarity, see [ref] for a review. $|V_ub|$ can be extracted from $b→u ℓν$ decays, and in in particular from $B→πℓν$, using lattice QCD [ref] or light-cone sum rules [ref] calculations of the relevant form factors.","intent_p":0.9,"contests_p":null}]}],"unlabelled_sentences":22},"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/1604.07598"}}