We present a high-statistics lattice calculation of the kinetic energy -lambda(1)/2m(b) of the heavy quark inside the B-meson and of the chrome-magnetic term lambda(2), related to the B*-B mass splitting, performed in the HQET. Our results have been obtained from a numerical simulation based on 600 gauge field configurations generated at beta = 6.0, on a lattice volume 24(3) x 40 and using, for the meson correlators, the results obtained with the SW-Clover O(a) improved lattice action for the light quarks. For the kinetic energy we found -lambda(1) = [B(h) over bar(iD)(2)hB]/(2M(B)) = -(0.09 +/- 0.14) GeV2, which is interesting for phenomenological applications. We also found lambda(2) = 0.07 +/- 0.01 GeV2, corresponding to M(B*)(2) - M(B)(2) = 4 lambda(2) = 0.280 +/- 0.060 GeV2, which is about one half of the experimental value. The origin of the discrepancy with the experimental number needs to be clarified.
A high-statistics lattice calculation of lambda(1) and lambda(2) in the B-meson / Gimenez, V.; Martinelli, G.; Sachrajda, C. T.. - In: NUCLEAR PHYSICS. B. - ISSN 0550-3213. - 486:1-2(1997), pp. 227-244. [10.1016/S0550-3213(96)00696-7]
A high-statistics lattice calculation of lambda(1) and lambda(2) in the B-meson
Martinelli, G.;
1997-01-01
Abstract
We present a high-statistics lattice calculation of the kinetic energy -lambda(1)/2m(b) of the heavy quark inside the B-meson and of the chrome-magnetic term lambda(2), related to the B*-B mass splitting, performed in the HQET. Our results have been obtained from a numerical simulation based on 600 gauge field configurations generated at beta = 6.0, on a lattice volume 24(3) x 40 and using, for the meson correlators, the results obtained with the SW-Clover O(a) improved lattice action for the light quarks. For the kinetic energy we found -lambda(1) = [B(h) over bar(iD)(2)hB]/(2M(B)) = -(0.09 +/- 0.14) GeV2, which is interesting for phenomenological applications. We also found lambda(2) = 0.07 +/- 0.01 GeV2, corresponding to M(B*)(2) - M(B)(2) = 4 lambda(2) = 0.280 +/- 0.060 GeV2, which is about one half of the experimental value. The origin of the discrepancy with the experimental number needs to be clarified.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.