{"arxiv_id":"hep-ph/0401041","incoming":{"papers":33,"sentences":39,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":6,"sentences":6,"quotes":[{"arxiv_id":"1305.4797","title":"Isospin asymmetries in $B\\to (K^*,\\rho) \\gamma/ l^+ l^-$ and $B \\to K l^+ l^-$ in and beyond the Standard Model","url":"/paper/1305.4797","section":"Wilson coefficients","sentence":"The calculation is carried out as described in the appendix of [ref] using the full anomalous dimension matrix computed in [ref] , at fixed $N_f=5$, and initial conditions are computed at $μ=M_W$ as described therein using the NNLO expressions in [ref] for $C_1-6$ and $C_9,10$ and those in [ref] for $C_7,8^eff$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"2108.07026","title":"Dark matter in three-Higgs-doublet models with $S_3$ symmetry","url":"/paper/2108.07026","section":"$B$ physics constraints","sentence":"The rate is determined from an expansion of the relevant Wilson coefficients in powers of $α_s/(4π)$, starting with (1) the matching of these coefficients to the full theory at some high scale ($μ_0∼m_W$ or $m_t$), then (2) evolving them down to the low scale $μ_b∼m_b$ (in this process the operators mix), and (3) determine the matrix elements at the low scale [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1704.05447","title":"On Flavourful Easter eggs for New Physics hunger and Lepton Flavour Universality violation","url":"/paper/1704.05447","section":"New Physics Benchmarks for $ΔB = 1$","sentence":"All the SM WCs in this work are evolved from the mass scale of the W boson down to $μ_b=4.8$ GeV, using state-of-the-art perturbative QCD and QED calculations for the matching conditions [ref] and the anomalous dimension matrices [ref] relevant for the processes considered in this analysis.","intent_p":0.97,"contests_p":null},{"arxiv_id":"0706.2997","title":"Constraining the Two-Higgs-Doublet-Model parameter space","url":"/paper/0706.2997","section":"$B̅→X_sγ$","sentence":"In the NNLO, the perturbative contribution $P$ is obtained via the following three steps [ref] : * Evaluation of the Wilson coefficients at the “high” (electroweak) scale, $μ_0$ [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"0805.3911","title":"Fermionic corrections to the interference of the electro- and chromomagnetic dipole operators in anti-B --> X(s) gamma at O(alpha(s)**2)","url":"/paper/0805.3911","section":"Numerical impact","sentence":"Determining the effect of the new fermionic corrections on $Br(B̅→X_sγ)$ in this case would require to repeat the interpolation procedure performed in [ref] .","intent_p":0.88,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1701.04029","title":"The $\\Lambda_b\\to \\Lambda(\\to p\\pi^-)\\mu^+\\mu^-$ decay in the aligned two-Higgs-doublet model","url":"/paper/1701.04029","section":"Results within the SM","sentence":"For the short-distance Wilson coefficients at the low scale $μ_b=4.2 GeV$, we use the numerical values collected in Table [ref], which are obtained at the next-to-next-to-leading logarithmic (NNLL) accuracy within the SM [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1205.6569","title":"Probing the charged Higgs boson at the LHC in the CP-violating type-II 2HDM","url":"/paper/1205.6569","section":"Experimental constraints","sentence":"The most up-to-date SM prediction for this decay, at the Next-to-Next-to-Leading Order (NNLO), gives [ref] : [equation] while the combined experimental value from HFAG points to a larger value [ref] : [equation] For type-II Yukawa interactions, which we consider here, light charged Higgs bosons are excluded by this observable.","intent_p":0.93,"contests_p":null},{"arxiv_id":"2409.00181","title":"On the smallness of charm loop effects in $B\\to K^{(*)} \\ell\\ell$ at low $q^2$: light meson Distribution Amplitude analysis","url":"/paper/2409.00181","section":"Introduction","sentence":"In the SM, $C_1 = -0.2507$, $C_2 = 1.0136$, $C_7γ = -0.3143$, $C_9 = 4.0459$ and $C_10 = -4.2939$ [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0805.3911","title":"Fermionic corrections to the interference of the electro- and chromomagnetic dipole operators in anti-B --> X(s) gamma at O(alpha(s)**2)","url":"/paper/0805.3911","section":"Fermionic corrections","sentence":"In this limit our result for the complete expression with $i=$ reduces to [equation] which is in agreement with the asymptotic form found in [ref] (see equation (5.10) of that reference).","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"0709.4422","title":"Towards $B \\to V \\gamma$ Decays at NNLO in SCET","url":"/paper/0709.4422","section":"Introduction","sentence":"The Wilson coefficients $C_i$ have been known within the next-to-leading logarithmic approximation (NLL) for over a decade (for a review, see [ref] ), and have been recently calculated at next-to-next-to-leading logarithmic order (NNLL) in a series of papers [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"2310.13051","title":"Low-energy effective field theory below the electroweak scale: one-loop renormalization in the 't Hooft-Veltman scheme","url":"/paper/2310.13051","section":"Introduction","sentence":"Partial results for the RGEs were known previously and have been studied to higher loop orders [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1607.01320","title":"Prospects for charged Higgs searches at the LHC","url":"/paper/1607.01320","section":"Constraints from $H^+$ loop-level exchange","sentence":"A huge effort has been devoted to the calculation of these corrections, the bulk of which are the same as in the SM [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"2101.01344","title":"Study on pure annihilation type B to V gamma decays","url":"/paper/2101.01344","section":"Introduction","sentence":"Most $B →Vγ$ decays occur via the flavour-changing neutral-current transitions $b→sγ$ or $b→dγ$, and the quark level transition amplitudes are now approaching next-to-next-to-leading order accuracy [ref] .","intent_p":0.95,"contests_p":null}]}],"unlabelled_sentences":25},"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/hep-ph/0401041"}}