We present a high-statistics lattice calculation of the kinetic energy of the heavy quark inside the -meson and of the chromo-magnetic term , related to the – mass splitting, performed in the HQET. Our results have been obtained from a numerical simulation based on 600 gauge field configurations generated at , on a lattice volume and using, for the meson correlators, the results obtained with the SW-Clover improved lattice action for the light quarks. For the kinetic energy we found $-\lambda_1=\langle B \vert \bar h (i\vec{D})^{2} h \vert B \rangle /(2 M_B )=-(0.09 \pm 0.14)^2$, which is interesting for phenomenological applications. We also find $\lambda_2= 0.07 \pm 0.01^2M^2_{B^*}-M^2_B= 4 \lambda_2= 0.280 \pm 0.060 ^2$, which is about one half of the experimental value. The origin of the discrepancy with the experimental number needs to be clarified.

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