G.M. Todesco
Sapienza University of Rome
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Physics Letters B | 1995
Chris Allton; M. Crisafulli; Vittorio Lubicz; G. Martinelli; F. Rapuano; N. Stella; A. Vladikas; A. Bartoloni; C. Battista; S. Bacasino; N. Cabibbo; Emanuele Panizzi; P.S. Paolucci; R. Sarno; G.M. Todesco; M. Torelli; P. Vicini
Abstract We present the results of a high statistics lattice calculation of hadronic form factors relevant for D - and B -meson semi-leptonic decays into light pseudoscalar and vector mesons. The results have been obtained by averaging over 170 gauge field configurations, generated in the quenched approximation, at β = 6.0, on a 18 3 × 64 lattice, using the O ( α )-improved SW-Clover action. From the study of the matrix element 〈 K − |J μ |D 0 〉, we obtain f + (0) = 0.78 ± 0.08 and from the matrix element 〈 K ∗0 |J μ |D + 〉 we obtain V (0) = 1.08 ± 0.22, A i (0) = 0.67 ± 0.11 and A 2 (0) = 0.49 ± 0.34. We also obtain the ratios V(0) A 1 (0) = 1.6 ± 0.3 and A 2 (0) A 1 (0) = 0.7 ± 0.4 . Our predictions for the different form factors are in good agreement with the experimental data, although, in the case of A 2 (0), the errors are still too large to draw any firm conclusion. With the help of the Heavy Quark Effective Theory (HQET) we have also extrapolated the lattice results to B -meson decays. The form factors follow a behaviour compatible with the HQET predictions. Our results are in agreement with a previous lattice calculation, performed at β = 6.4, using the standard Wilson action.
International Journal of Modern Physics C | 1993
A. Bartoloni; C. Battista; S. Cabasino; P.S. Paolucci; J. Pech; R. Sarno; G.M. Todesco; M. Torelli; W. Tross; P. Vicini; R. Benzi; N. Cabibbo; F. Massaioli; R. Tripiccione
In this paper we describe an implementation of the Lattice Boltzmann Equation method for fluid-dynamics simulations on the APE100 parallel computer. We have performed a simulation of a two-dimensional Rayleigh-Benard convection cell. We have tested the theory proposed by Shraiman and Siggia for the scaling of the Nusselt number vs. Rayleigh number.
International Journal of Modern Physics C | 1993
A. Bartoloni; G. Bastianello; C. Battista; S. Cabasino; F. Marzano; P.S. Paolucci; J. Pech; F. Rapuano; Emanuele Panizzi; R. Sarno; G.M. Todesco; M. Torelli; W. Tross; P. Vicini; N. Cabibbo; A. Fucci; R. Tripiccione
APE100 processors are based on a simple Single Instruction Multiple Data architecture optimized for the simulation of Lattice Field Theories or other complex physical systems. This paper describes the hardware implementation of the first APE100 machine.
International Journal of Modern Physics C | 1993
A. Bartoloni; G. Bastianello; C. Battista; S. Cabasino; F. Marzano; P.S. Paolucci; J. Pech; F. Rapuano; Emanuele Panizzi; R. Sarno; G.M. Todesco; M. Torelli; W. Tross; P. Vicini; N. Cabibbo; R. Tripiccione
We describe the software environment available for the APE100 parallel processor. We discuss the parallel programming language that we have defined for APE100 and its optimizing compiler. We then describe the operating system that allows to control APE100 from a host computer.
Nuclear Physics | 1994
Chris Allton; Vittorio Lubicz; G. Martinelli; G Salina; A. Vladikas; A. Bartoloni; C. Battista; S. Cabasino; N. Cabibbo; F. Marzano; P.S. Paolucci; J. Pech; F. Rapuano; R. Sarno; G.M. Todesco; M. Torelli; W. Tross; R Tripiccione; P. Vicini
We present a high statistics calculation of ƒB in the static limit. The results have been obtained by numerical simulation of quenched QCD, at β = 6.0 on a 183 × 32 lattice. We compare ƒB calculated by using the Wilson and the Clover quark actions. The decay constant is obtained by studying heavy-light correlation functions of different smeared operators, on a sample of 210 gauge field configurations. We find that cubic smearings of size Ls ⩽ 3 or Ls ⩾ 9 are bad projectors on the lightest pseudoscalar state. Combining the information coming from smearing Ls = 5 and Ls = 7, we have obtained ƒB = 370±40 MeV in the clover case and ƒB = 350±40±30 MeV in the Wilson case. Our results support a large value of the pseudoscalar decay constant in the static approximation.
Physics Letters B | 1996
As. Abada; Ph. Boucaud; N. Cabibbo; M. Crisafulli; Jp Leroy; Lubicz; G. Martinelli; F. Rapuano; Marco Serone; N. Stella; A. Bartoloni; C. Battista; S. Cabasino; Emanuele Panizzi; P.S. Paolucci; R. Sarno; G.M. Todesco; M. Torelli; P. Vicini
Abstract We present the results of a numerical calculation of the B → K ∗ γ form factors. The results have been obtained by studying the relevant correlation functions at β = 6.0, on an 18 3 × 64 lattice, using the O ( a )-improved fermion action, in the quenched approximation. From the study of the matrix element 〈K ∗ | s σ μν b|B〉 we have obtained the form factor T 1 (0) which controls the exclusive decay rate. The results are compared with the recent results from CLEO. We also discuss the compatibility between the scaling laws predicted by the Heavy Quark Effective Theory (HQET) and pole dominance, by studying the mass- and q 2 -dependence of the form factors. From our analysis, it appears that the form factors follow a mass behaviour compatible with the predictions of the HQET and that the q 2 -dependence of T 2 is weaker than would be predicted by pole dominance.
Nuclear Physics B - Proceedings Supplements | 1995
A. Bartoloni; C. Battista; M. Bellacci; S. Cabasino; N. Cabibbo; M. Cosimi; U. Dagostino; F. Marzano; Emanuele Panizzi; P.S. Paolucci; F. Rapuano; W. Rinaldi; R. Sarno; G.M. Todesco; M. Torelli; P. Vicini; F. Laico; R. Tripiccione
We describe APEmille, the latest generation of the APE parallel processors. This machine, an evolution of the APE100 concept, is very efficient for LGT simulations as well as for a broader class of applications requiring massive floating point computations. Several new features characterise this evolution. In particular local addressing capabilities are added to all computing nodes. APEmille also exhibits a higher degree of integration with a network of workstations acting as a global host system. An APEmille system in the Teraflops range will be completed in three-four years. The architecture proposed in this paper is being currently simulated and evaluated.
Nuclear Physics B - Proceedings Supplements | 1994
Chris Allton; M. Crisafulli; Vittorio Lubicz; G. Martinelli; G Salina; A. Bartoloni; C. Battista; S. Cabasino; N. Cabibbo; F. Marzano; P.S. Paolucci; J. Pech; F. Rapuano; R. Sarno; G.M. Todesco; M. Torelli; W. Tross; P. Vicini
The decay constants of the heavy-light pseudoscalar mesons are studied in a high statistics run using the Wilson action at β = 6.0 and β = 6.2, and the clover action at β = 6.0. The systematics of O(a) discretisation errors are discussed.. Our best estimates of the decay constant are: fD = 218(9) MeV, fD/fDs = 1.11(1) and we obtain preliminary values for fB.The decay constants of the heavy-light pseudoscalar mesons are studied in a high statistics run using the Wilson action at
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
G. Bastianello; R. Borgognoni; C. Battista; S. Cabasino; N. Cabibbo; A. Fucci; A. Lai; F. Marzano; P.S. Paolucci; J. Pech; R. Sarno; G.M. Todesco; M. Torelli; R. Tripiccione; W. Tross; P. Vicini
\beta=6.0
arXiv: High Energy Physics - Lattice | 1995
M. Crisafulli; A. Donini; Lubicz; G. Martinelli; F. Rapuano; C Ungarelli; A. Vladikas; A. Bartoloni; C. Battista; S. Cabasino; N. Cabibbo; F. Marzano; Emanuele Panizzi; P.S. Paolucci; R. Sarno; G.M. Todesco; M. Torelli; P. Vicini
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