B-parameters of the complete set of matrix elements of (ΔB = 2) operators from the lattice
By D. Bečirević, V. Gimenez, G. Martinelli, M. Papinutto, J. Reyes. 2002
141 citations recorded by the source corpus.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/8eaec9a3c27122097084737b4b3dff2c34ba42b6
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In Nuclear and High Energy Physics
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Citations in the corpus
- Model-independent constraints on ΔF = 2 operators and the scale of new physics (2007, background): “8 GeV for charmed mesons, and μK = 2GeV for Kaons, which are the renormalisation scales of the operators used in lattice computations for the matrix elements [46, 47].”
- Anatomy and phenomenology of FCNC and CPV effects in SUSY theories (2009, methodology): “The theoretical prediction in the SM for the semileptonic asymmetry ASL improved thanks to improvements in lattice studies of ∆B = 2 four-fermion operators [105] and to the NLO perturbative calculations of the corresponding Wilson coefficients [106, 107].”
- Charged-Higgs phenomenology in the aligned two-Higgs-doublet model (2010, methodology): “ be taken at the matching scale µtW . the Bi(µ) parametrizing the deviation from the naive factorization limit. These Bi(µ) factors have been evaluated in the quenched approximation on the lattice in [156], using a different operator basis. The connection reads (see again [119], given here with both ”
- ΔF = 2 observables and fine-tuning in a warped extra dimension with custodial protection (2008, methodology): “2 KB LR 1 (µ), (4.28) hQLR 2 (µ)i = 1 2 R(µ)m2 KF 2 KB LR 2 (µ), (4.29) where the B i parameters are known from lattice calculations. They are related to the parameters B 1, B 5 and B 4 calculated in [57,58] as follows BVLL 1 (µ) ≡ B 1 , B LR 1 (µ) ≡ B 5 , B LR 2 (µ) ≡ B 4 , (4.30) and their numeric”
- ΔS=2 and ΔC=2 bag parameters in the standard model and beyond from N$_f$=2+1+1 twisted-mass lattice QCD (2015, unknown): “omputations of the BSM B i see Refs. [42,43]. 5Work in progress of an unquenched N f = 2 + 1 computation for the D-mixing is reported in Ref. [47]. For older works using quenched simulations see Refs [48,49]. 3 (this paper) TM/OS, NP ren. ETMC 15 N f = 2 + 1 + 1 SWME 14 Improved Stagg., PT1 ` ren. D”