Matches in SemOpenAlex for { <https://semopenalex.org/work/W3041103539> ?p ?o ?g. }
- W3041103539 abstract "In this paper, we studied systematically the semileptonic decays ${overline{B}}_{s}ensuremath{rightarrow}{K}^{(*)}{ensuremath{ell}}^{+}{ensuremath{ell}}^{ensuremath{-}}$ with ${l}^{ensuremath{-}}=({e}^{ensuremath{-}},{ensuremath{mu}}^{ensuremath{-}},{ensuremath{tau}}^{ensuremath{-}})$ by using the perturbative QCD (PQCD) and the ``$mathrm{PQCD}+mathrm{Lattice}$'' factorization approach, respectively. We first evaluated all relevant form factors ${F}_{i}({q}^{2})$ in the low-${q}^{2}$ region using the PQCD approach, and we also took the available lattice QCD results at the end point ${q}_{mathrm{max}}^{2}$ as additional inputs to improve the extrapolation of the form factors to the high-${q}^{2}$ region. We calculated the branching ratios and twelve other kinds of physical observables. From our studies, we find the following points: (a) for ${overline{B}}_{s}ensuremath{rightarrow}K{l}^{+}{l}^{ensuremath{-}}$ decays, the PQCD and $mathrm{PQCD}+mathrm{Lattice}$ predictions for branching ratios $mathcal{B}({overline{B}}_{s}ensuremath{rightarrow}K{l}^{+}{l}^{ensuremath{-}})$, the ratios of the branching ratios ${R}_{K}^{eensuremath{mu}}$ and ${R}_{K}^{ensuremath{mu}ensuremath{tau}}$, and the longitudinal polarization asymmetry of the leptons ${P}_{L}$ agree well within errors; (b) the PQCD and $mathrm{PQCD}+mathrm{Lattice}$ predictions for the $CP$-averaged branching ratio $mathcal{B}({overline{B}}_{s}ensuremath{rightarrow}{K}^{*}{ensuremath{mu}}^{+}{ensuremath{mu}}^{ensuremath{-}})$ are $(3.1{7}_{ensuremath{-}0.78}^{+0.95})ifmmodetimeselsetexttimesfi{}{10}^{ensuremath{-}8}$ and $(2.4{8}_{ensuremath{-}0.50}^{+0.56})ifmmodetimeselsetexttimesfi{}{10}^{ensuremath{-}8}$ respectively, which agree well with the LHCb measured value $(2.9ifmmodepmelsetextpmfi{}1.1)ifmmodetimeselsetexttimesfi{}{10}^{ensuremath{-}8}$ and the light-cone sum rule prediction; (c) for the ratios ${R}_{{K}^{*}}^{eensuremath{mu}}$ and ${R}_{{K}^{*}}^{ensuremath{mu}ensuremath{tau}}$, the PQCD and $mathrm{PQCD}+mathrm{Lattice}$ predictions agree well with each other and have a small error less than 10%; (d) for the direct $CP$ asymmetries ${mathcal{A}}_{CP}$ of all considered decay modes, they are always very small as expected: less than 5% in magnitude; (e) for the angular observables ${P}_{1,2,3}$ and ${P}_{4,5,6,8}^{ensuremath{'}}$, our theoretical predictions for each kind of lepton are consistent within errors; (f) the theoretical predictions of the angular observables ${P}_{3}$ and ${P}_{6}^{ensuremath{'}}$ are less than ${10}^{ensuremath{-}2}$ in size, but the magnitude of ${P}_{1,2}$ and ${P}_{4,5}^{ensuremath{'}}$ are larger than 0.2; and (g) the PQCD and $mathrm{PQCD}+mathrm{Lattice}$ predictions of the binned values of all considered observables in the two ${q}^{2}$ bins $[0.1--0.98]text{ }text{ }{mathrm{GeV}}^{2}$ and $[1.1--6]text{ }text{ }{mathrm{GeV}}^{2}$ generally agree with each other and are also consistent with the light-cone sum rule results within errors. We believe that above predictions could be tested by future LHCb and Belle-II experiments." @default.
- W3041103539 created "2020-07-16" @default.
- W3041103539 creator A5033898863 @default.
- W3041103539 creator A5077004706 @default.
- W3041103539 creator A5091196440 @default.
- W3041103539 date "2020-07-07" @default.
- W3041103539 modified "2023-10-12" @default.
- W3041103539 title "Study of <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:msub><mml:mi>B</mml:mi><mml:mi>s</mml:mi></mml:msub><mml:mo stretchy=false>→</mml:mo><mml:msup><mml:mi>K</mml:mi><mml:mrow><mml:mo stretchy=false>(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=false>)</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mo>ℓ</mml:mo><mml:mo>−</mml:mo></mml:msup></mml:math> decays in the PQCD factorization approach with …" @default.
- W3041103539 cites W1010974669 @default.
- W3041103539 cites W1485951081 @default.
- W3041103539 cites W1515652023 @default.
- W3041103539 cites W1561863491 @default.
- W3041103539 cites W1563131206 @default.
- W3041103539 cites W1572009945 @default.
- W3041103539 cites W1573726524 @default.
- W3041103539 cites W1589815764 @default.
- W3041103539 cites W1592535523 @default.
- W3041103539 cites W1671677220 @default.
- W3041103539 cites W1798970806 @default.
- W3041103539 cites W1814236352 @default.
- W3041103539 cites W1965997378 @default.
- W3041103539 cites W1966050800 @default.
- W3041103539 cites W1969551354 @default.
- W3041103539 cites W1971504869 @default.
- W3041103539 cites W1973032229 @default.
- W3041103539 cites W1974615017 @default.
- W3041103539 cites W1979646867 @default.
- W3041103539 cites W1987201696 @default.
- W3041103539 cites W1987758977 @default.
- W3041103539 cites W1989709563 @default.
- W3041103539 cites W2000497329 @default.
- W3041103539 cites W2002660159 @default.
- W3041103539 cites W2007088632 @default.
- W3041103539 cites W2008720733 @default.
- W3041103539 cites W2011734771 @default.
- W3041103539 cites W2025074645 @default.
- W3041103539 cites W2033305982 @default.
- W3041103539 cites W2033643447 @default.
- W3041103539 cites W2042852519 @default.
- W3041103539 cites W2053449237 @default.
- W3041103539 cites W2058321324 @default.
- W3041103539 cites W2078270404 @default.
- W3041103539 cites W2081315250 @default.
- W3041103539 cites W2081413191 @default.
- W3041103539 cites W2083703917 @default.
- W3041103539 cites W2084724589 @default.
- W3041103539 cites W2085314172 @default.
- W3041103539 cites W2096578925 @default.
- W3041103539 cites W2098161722 @default.
- W3041103539 cites W2099019126 @default.
- W3041103539 cites W2100661111 @default.
- W3041103539 cites W2101354462 @default.
- W3041103539 cites W2117836026 @default.
- W3041103539 cites W2122880996 @default.
- W3041103539 cites W2169681162 @default.
- W3041103539 cites W2180664799 @default.
- W3041103539 cites W2207853794 @default.
- W3041103539 cites W2209755258 @default.
- W3041103539 cites W2222592244 @default.
- W3041103539 cites W2263776277 @default.
- W3041103539 cites W2279275894 @default.
- W3041103539 cites W2285146553 @default.
- W3041103539 cites W2319907582 @default.
- W3041103539 cites W2574359264 @default.
- W3041103539 cites W2589693489 @default.
- W3041103539 cites W2593580726 @default.
- W3041103539 cites W2595675837 @default.
- W3041103539 cites W2598542921 @default.
- W3041103539 cites W2602585683 @default.
- W3041103539 cites W2609225800 @default.
- W3041103539 cites W2738825493 @default.
- W3041103539 cites W2749699019 @default.
- W3041103539 cites W2804422045 @default.
- W3041103539 cites W2899140785 @default.
- W3041103539 cites W2909209084 @default.
- W3041103539 cites W2938994039 @default.
- W3041103539 cites W2941678098 @default.
- W3041103539 cites W2949273330 @default.
- W3041103539 cites W2963814033 @default.
- W3041103539 cites W2987209375 @default.
- W3041103539 cites W2988748154 @default.
- W3041103539 cites W3101192299 @default.
- W3041103539 cites W3102388234 @default.
- W3041103539 cites W3102980454 @default.
- W3041103539 cites W3104658238 @default.
- W3041103539 cites W3105997193 @default.
- W3041103539 cites W3106427498 @default.
- W3041103539 cites W3119995751 @default.
- W3041103539 cites W3123207238 @default.
- W3041103539 cites W3123612560 @default.
- W3041103539 cites W3125738030 @default.
- W3041103539 cites W3125912098 @default.
- W3041103539 cites W372381130 @default.
- W3041103539 cites W4232077750 @default.
- W3041103539 cites W61684932 @default.
- W3041103539 cites W62223043 @default.
- W3041103539 cites W68975410 @default.
- W3041103539 cites W2901398526 @default.
- W3041103539 doi "https://doi.org/10.1103/physrevd.102.013001" @default.
- W3041103539 hasPublicationYear "2020" @default.