• Chinese Physics C
  • Vol. 44, Issue 1, (2020)
Rui-Yu Zhou1、*, Lei Guo1、*, Hai-Bing Fu1、*, Wei Cheng1、*, and Xing-Gang Wu1、*
Author Affiliations
  • 1Department of Physics, Chongqing University1Department of Physics, Chongqing University, Chongqing 401331, China
  • 1Department of Physics, Guizhou Minzu University2Department of Physics, Guizhou Minzu University, Guiyang 550025, China
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    DOI: 10.1088/1674-1137/44/1/013101 Cite this Article
    Rui-Yu Zhou, Lei Guo, Hai-Bing Fu, Wei Cheng, Xing-Gang Wu. The semileptonic decay within the LCSR approach under heavy quark effective field theory *[J]. Chinese Physics C, 2020, 44(1): Copy Citation Text show less
    (color online) The behavior of LCDA predicted by the BHL model, including the uncertainties of the input parameters. For comparison, we present the JLab fit [13], QCD SR [18], CZ form [46] and the asymptotic form [47].
    Fig. 1. (color online) The behavior of LCDA predicted by the BHL model, including the uncertainties of the input parameters. For comparison, we present the JLab fit [13], QCD SR [18], CZ form [46] and the asymptotic form [47].
    (color online) The extrapolated TFFs calculated using the two correlators LCSR-/(left/right plots). The shaded bands are the uncertainties from the error sources. As a comparison, the predictions of lattice QCD [7], LCSR [14, 15], pQCD [49] and HPQCD [50] are also shown.
    Fig. 2. (color online) The extrapolated TFFs calculated using the two correlators LCSR- / (left/right plots). The shaded bands are the uncertainties from the error sources. As a comparison, the predictions of lattice QCD [7], LCSR [14, 15], pQCD [49] and HPQCD [50] are also shown.
    (color online) The differential branching fractions for the two correlators LCSR-/(left/right plots). As a comparison, the BABAR data [53, 55] and the Belle data [54, 56] are also shown.
    Fig. 3. (color online) The differential branching fractions for the two correlators LCSR- / (left/right plots). As a comparison, the BABAR data [53, 55] and the Belle data [54, 56] are also shown.
    AβB
    0.03923.500.610.075
    0.11224.630.590.010
    0.18523.500.630.141
    Table 1. Parameters of twist-2 LCDA determined from [45].
    Total
    Table 2. Uncertainties of TFFs at . The uncertainties of the total TFFs are summed up in quadrature.
    Twist-2Twist-3Twist-4Central
    0.284−0.0090.276
    0.1530.134−0.0040.282
    Table 3. Different twist terms in TFFs for large recoils
    −1.600−1.4530.03%
    −1.1552.075−3.3770.01%
    −1.309−1.7570.50%
    −1.1970.656−0.6110.06%
    Table 4. The fit parameters and quality of fit of LCSR- and LCSR- TFFs
    Exclusive decays
    LCSR- (This work)
    LCSR- (This work)
    RBC/UKQCD [7]
    Fermilab/MILC [8]
    pQCD [9]
    -meson LCSR [13]
    Imsong 2014 (LCSR) [15]
    BABAR 2012 [53]
    Belle 2013 [54]
    CKM fitter [57]
    UT fitter [58]
    FLAG 2016 [59]
    HFAG 2016 [60]
    Table 5. A comparison of derived using various approaches.
    Exclusive decays
    LCSR- (This work)
    LCSR- (This work)
    PDG [40]
    BABAR 2012 [53]
    Belle 2013 [54]
    BABAR 2010 [55]
    Belle 2010 [56]
    CLEO [61]
    HFAG 2016 [60]
    Table 6. A comparison of the branching fraction of with the experimental measurements. Both LCSR- and LCSR- predictions are consistent with the data.
    Rui-Yu Zhou, Lei Guo, Hai-Bing Fu, Wei Cheng, Xing-Gang Wu. The semileptonic decay within the LCSR approach under heavy quark effective field theory *[J]. Chinese Physics C, 2020, 44(1):
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