S. Rosati
University of Pisa
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Featured researches published by S. Rosati.
Physical Review C | 2003
T. S. Park; L. E. Marcucci; R. Schiavilla; Michele Viviani; A. Kievsky; S. Rosati; K. Kubodera; Dong-Pil Min; Mannque Rho
Spurred by the recent complete determination of the weak currents in two-nucleon systems up to
Nuclear Physics | 1996
A. Kievsky; S. Rosati; W. Tornow; M. Viviani
\mathcal{O}{(Q}^{3})
Physical Review C | 2001
A. Kievsky; M. Viviani; S. Rosati
in heavy-baryon chiral perturbation theory, we carry out a parameter-free calculation of the threshold S factors for the solar
Nuclear Physics | 1994
A. Kievsky; M. Viviani; S. Rosati
\mathrm{pp}
Nuclear Physics | 1993
A. Kievsky; M. Viviani; S. Rosati
(proton-fusion) and hep processes in an effective field theory (EFT) that combines the merits of the standard nuclear physics method and systematic chiral expansion. The power of the EFT adopted here is that one can correlate in a unified formalism the weak-current matrix elements of two-, three-, and four-nucleon systems. Using the tritium
Physical Review C | 2003
A. Nogga; A. Kievsky; H. Kamada; W. Glöckle; L. E. Marcucci; S. Rosati; Michele Viviani
\ensuremath{\beta}
Physical Review C | 2000
L. E. Marcucci; R. Schiavilla; M. Viviani; A. Kievsky; S. Rosati; John F. Beacom
-decay rate as an input to fix the only unknown parameter in the theory, we can evaluate the threshold S factors with drastically improved precision; the results are
Physical Review C | 2005
M. Viviani; A. Kievsky; S. Rosati
{S}_{\mathrm{pp}}(0)=3.94\ifmmode\times\else\texttimes\fi{}(1\ifmmode\pm\else\textpm\fi{}0.004)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}25}\mathrm{MeV}\mathrm{}\mathrm{b}
Physical Review C | 2005
A. Deltuva; A. C. Fonseca; A. Kievsky; S. Rosati; P. U. Sauer; Michele Viviani
and
Physical Review C | 2005
R. Lazauskas; J. Carbonell; A. C. Fonseca; Michele Viviani; A. Kievsky; S. Rosati
{S}_{\mathrm{hep}}(0)=(8.6\ifmmode\pm\else\textpm\fi{}1.3)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}20}\mathrm{keV}\mathrm{}\mathrm{b}.