We compute nonperturbatively the average up-down and strange quark masses from the large momentum (short-distance) behavior of the quark propagator in the Landau gauge. This method, which has never been applied so far, does not require the explicit calculation of the quark mass renormalization constant. Calculations were performed in the quenched approximation, by using O(a) improved Wilson fermions. The main results of this study are m(l)(RI)(2 GeV) = 5.8(6) MeV and m(s)(RI)(2 GeV) = 136(11) MeV. Using the relations between different schemes, obtained from the available four-loop anomalous dimensions, we also find m(l)(RGI) = 7.6(8) MeV and m(s)(RGI) = 177(14) MeV, and the modified minimal subtraction scheme (<(MS)over bar>) masses m(l)(<(MS)over bar>)(2 GeV) = 4.8(5) MeV and m(s)(<(MS)over bar>)(2 GeV) = 111(9) MeV.
Light quark masses from lattice quark propagators at large momenta / D., Becirevic; V., Gimenez; V., Lubicz; Martinelli, Guido. - In: PHYSICAL REVIEW D. - ISSN 0556-2821. - 61:11(2000), pp. 114507-114525. [10.1103/PhysRevD.61.114507]
Light quark masses from lattice quark propagators at large momenta
Martinelli, Guido
2000-01-01
Abstract
We compute nonperturbatively the average up-down and strange quark masses from the large momentum (short-distance) behavior of the quark propagator in the Landau gauge. This method, which has never been applied so far, does not require the explicit calculation of the quark mass renormalization constant. Calculations were performed in the quenched approximation, by using O(a) improved Wilson fermions. The main results of this study are m(l)(RI)(2 GeV) = 5.8(6) MeV and m(s)(RI)(2 GeV) = 136(11) MeV. Using the relations between different schemes, obtained from the available four-loop anomalous dimensions, we also find m(l)(RGI) = 7.6(8) MeV and m(s)(RGI) = 177(14) MeV, and the modified minimal subtraction scheme (<(MS)over bar>) masses m(l)(<(MS)over bar>)(2 GeV) = 4.8(5) MeV and m(s)(<(MS)over bar>)(2 GeV) = 111(9) MeV.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.