{"arxiv_id":"1001.0293","incoming":{"papers":13,"sentences":22,"groups":[{"kind":"background","label":"Cites it as background","papers":5,"sentences":7,"quotes":[{"arxiv_id":"2110.13238","title":"Two-loop Prediction of the Anomalous Magnetic Moment of the Muon in the Two-Higgs Doublet Model with GM2Calc 2","url":"/paper/2110.13238","section":"The Model","sentence":"* The four well-known types with $Z_2$ symmetry: type I, type II, type X, type Y, * the flavour-aligned () [ref] , which also avoids tree-level Higgs-mediated FCNC and contains the four previous types as special cases, * the with general Yukawa structures.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1104.5123","title":"Interpretation of charged Higgs effects in low energy flavour physics","url":"/paper/1104.5123","section":"Introduction","sentence":"There has been an intense discussion on how the flavour problem can be solved within the class of models with two or more Higgs doublets [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2311.14486","title":"Is there a (Pseudo)Scalar at 95 GeV?","url":"/paper/2311.14486","section":"Minimal Flavour Violation and Natural Flavour Conservation","sentence":"This implementation of NFC is usually called “The Aligned 2HDM\" [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1612.03475","title":"Self-consistent Dark Matter Simplified Models with an s-channel scalar mediator","url":"/paper/1612.03475","section":"Aligned 2HDM+S","sentence":"We can define the linear combinations that couple to up, down quarks and leptons $Φ_u,d,l$ and their orthogonal ones $Φ_u,d,l⊥$ to be [equation] where $i=u,d,l$ and $0≤γ_u,d,l<π$ are arbitrary angles[References (e.g. [ref] ) define the Aligned model in terms of the parameters $ζ_u,d,l$, that can be complex in general.","intent_p":0.84,"contests_p":null},{"arxiv_id":"1106.0034","title":"Theory and phenomenology of two-Higgs-doublet models","url":"/paper/1106.0034","section":"Models with natural flavour conservation","sentence":"In a somewhat related work, Pich and Tuzón [ref] simply assumed that the Yukawa coupling matrices of $Φ_1$ and $Φ_2$ in flavour space are proportional.","intent_p":0.86,"contests_p":null}]}],"unlabelled_sentences":15},"outgoing":{"papers":5,"sentences":5,"groups":[{"kind":"data_used","label":"Uses data or values from","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0907.5386","title":"Flavor Physics in the Quark Sector","url":"/paper/0907.5386","section":"Phenomenology","sentence":"From the present knowledge of $B^+→τ^+ ν_τ$ [ref] , we obtain $|1-Δ_ub|=1.32±0.20$ which implies $M_H^±/√(|Re(ζ_l^+ζ_d)|)>5.7$ GeV ($90%$ CL).","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ex/0107031","title":"Search for Charged Higgs bosons: Preliminary Combined Results Using LEP data Collected at Energies up to 209 GeV","url":"/paper/hep-ex/0107031","section":"Phenomenology","sentence":"Assuming that $Br(H^+→c s̅)+Br(H^+→τ^+ ν_τ)=1$, the combined LEP data on $e^+e^- →H^+ H^-$ constrain $M_H^±>78.6$ GeV (95% CL) [ref] .","intent_p":0.95,"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/1001.0293"}}