{"arxiv_id":"1206.2970","incoming":{"papers":35,"sentences":46,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1608.07583","title":"Palatable Leptoquark Scenarios for Lepton Flavor Violation in Exclusive $b\\to s\\ell_1\\ell_2$ modes","url":"/paper/1608.07583","section":"$C_i^ℓ_1ℓ_2(μ)$ in Leptoquark Models","sentence":"We adopt the notation of Ref. [ref] and specify the LQ states by their quantum numbers with respect to the SM gauge group, $(SU(3)_c, SU(2)_L)_Y$, where the electric charge, $Q=Y+T_3$, is the sum of hypercharge ($Y$) and the third weak isospin component ($T_3$).","intent_p":0.84,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1603.04993","title":"Physics of leptoquarks in precision experiments and at particle colliders","url":"/paper/1603.04993","section":"$P →P'(V) ℓ^- ℓ^'+$","sentence":"Interplay of leptonic and semileptonic $P →P' ℓ^+ ℓ^-$ decays together constrain the couplings of LQ in the $b s̅$ systems very effectively [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":15,"sentences":15,"quotes":[{"arxiv_id":"1507.02070","title":"Study of the rare semileptonic decays $B_d^0 \\to K^* l^+ l^-$ in scalar leptoquark model","url":"/paper/1507.02070","section":"Introduction","sentence":"The phenomenology of scalar leptoquark and the contribution to new physics has been quite well studied in the literature [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1806.01048","title":"Impact of vector leptoquark on $\\bar B \\to \\bar K^* l^+ l^-$ anomalies","url":"/paper/1806.01048","section":"Introduction","sentence":"In the literature, the observed anomalies at LHCb experiment in various rare decays of $B$ mesons have been studied in the LQ model [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1207.2753","title":"Implications from clean observables for the binned analysis of B -> K*ll at large recoil","url":"/paper/1207.2753","section":"Introduction","sentence":"This has triggered extensive theoretical work studying the constraining power of radiative and semileptonic $B$ decays on New Physics in the framework of the weak effective Hamiltonian [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1310.0713","title":"Effect of scalar leptoquarks on the rare decays of B_s meson","url":"/paper/1310.0713","section":"Introduction","sentence":"The general classification of leptoquark models are discussed in [ref] and the phenomenology of scalar leptoquarks have been studied extensively in the literature [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1501.05193","title":"Scalar leptoquarks and the rare B meson decays","url":"/paper/1501.05193","section":"Introduction","sentence":"The phenomenology of scalar leptoquarks have been studied extensively in the literature [ref] .","intent_p":0.99,"contests_p":null}]}],"unlabelled_sentences":29},"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/1206.2970"}}