Understand
We report on a calculation of the $B^*B\pi$ coupling in lattice QCD.
- The strong matrix element $\langle B \pi | B^*\rangle$ is directly related to the leading order low-energy constant in heavy meson chiral perturbation theory (HM$\chi$PT) for $B$-mesons.
- We carry out our calculation directly at the $b$-quark mass using a non-perturbatively tuned clover action that controls discretisation effects of order $|\vec{p}a|$ and $(ma)^n$ for all $n$.
- Our analysis is performed on RBC/UKQCD gauge configurations using domain wall fermions and the Iwasaki gauge action at two lattice spacings of $a^{-1}=1.73(3)$ GeV, $a^{-1}=2.28(3)$ GeV, and unitary pion masses down to 290 MeV.
Built on
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N. Christ, M. Li, and H.-W. Lin, Relativistic heavy quark effective action
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H. Ohki, H. Matsufuru, and T. Onogi, Determination of B*B π \pi coupling in unquenched lattice QCD
2008
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2011
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Then
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D. Bečirević and F. Sanfilippo, Theoretical estimate of the decay rate
2013
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