Abstract

We compute the decays $${B\rightarrow D^*_0}$$ and $${B\rightarrow D^*_2}$$ with finite masses for the b and c quarks. We first discuss the spectral properties of both the B meson as a function of its momentum and the $$D^*_0$$ and $$D^*_2$$ at rest. We compute the theoretical formulae leading to the decay amplitudes from the three-point and two-point correlators. We then compute the amplitudes at zero recoil of $${B\rightarrow D^*_0}$$ , which turns out not to be vanishing contrary to what happens in the heavy quark limit. This opens the possibility to get better agreement with experiment. To improve the continuum limit we have added a set of data with smaller lattice spacing. The $${B\rightarrow D^*_2}$$ vanishes at zero recoil and we show a convincing signal but only slightly more than 1 sigma from 0. In order to reach quantitatively significant results we plan to exploit fully smaller lattice spacings as well as another lattice regularisation.

Highlights

  • In this paragraph, all the main formulae up to the differential decay rates will be given for the semileptonic decays of a B heavy meson into the first orbitally excited D∗∗ mesons.We will focus our study on the production of the |3 P0 and the |3 P2 states.1we will give relations in the case where the mass of the lepton cannot be neglected. 376 Page 2 of 25Eur

  • We compute the amplitudes at zero recoil of B → D0∗, which turns out not to be vanishing contrary to what happens in the heavy quark limit

  • All the main formulae up to the differential decay rates will be given for the semileptonic decays of a B heavy meson into the first orbitally excited D∗∗ mesons

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Summary

Theoretical framework

All the main formulae up to the differential decay rates will be given for the semileptonic decays of a B heavy meson into the first orbitally excited D∗∗ mesons. We will focus our study on the production of the |3 P0 (scalar D0∗) and the |3 P2 (tensor D2∗) states.. We will give relations in the case where the mass of the lepton cannot be neglected

P2 state
Differential decay rates
Leptonic tensor μν
Hadronic tensor Wμν
Kinematics and notations
Differential decay widths in the Brest frame
Measure d of the phase space
Extracting the form factors from the transition amplitudes
Kinematics
Summary
Estimation of the contribution of the form factors to the 3 P2 decay width
Infinite mass limit
Quantitative prediction of each contribution to the total width
Simulation set up
Masses and energies
Taking into account the scalar–pseudoscalar mixing
Symmetry properties of the matrix elements
GEVP on the three-point correlators
Subtracting zero momentum three-point correlators
Extracting the matrix element
Conclusions and prospects
P2 states
Findings
P2 form factors
Full Text
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