Abstract

We present a high-statistics lattice calculation of the kinetic energy λ1/2mb-\lambda_1/2 m_b of the heavy quark inside the BB-meson and of the chromo-magnetic term λ2\lambda_2, related to the BB^*--BB mass splitting, performed in the HQET. Our results have been obtained from a numerical simulation based on 600 gauge field configurations generated at β=6.0\beta=6.0, on a lattice volume 243×4024^3 \times 40 and using, for the meson correlators, the results obtained with the SW-Clover O(a)O(a) improved lattice action for the light quarks. For the kinetic energy we found λ1=Bhˉ(iD)2hB/(2MB)=(0.09±0.14)-\lambda_1=\langle B \vert \bar h (i\vec{D})^{2} h \vert B \rangle /(2 M_B )=-(0.09 \pm 0.14)~GeV2^2, which is interesting for phenomenological applications. We also find λ2=0.07±0.01\lambda_2= 0.07 \pm 0.01 GeV2^2, corresponding to MB2MB2=4λ2=0.280±0.060M^2_{B^*}-M^2_B= 4 \lambda_2= 0.280 \pm 0.060 GeV2^2, which is about one half of the experimental value. The origin of the discrepancy with the experimental number needs to be clarified.Comment: 26 pages, latex, 5 figure

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