LATTICE STUDY OF THE GLUON PROPAGATOR IN MOMENTUM-SPACE

We consider pure glue QCD at beta=5.7, beta=6.0, and beta=6.3. We eval uate the gluon propagator both in time at zero three-momentum and in m omentum space. From the former quantity we obtain evidence for a dynam ically generated effective mass, which at beta=6.0 and beta=6.3 increa ses with the time separation of the sources, in agreement with earlier results. The momentum space propagator G(k) provides further evidence for mass generation. In particular, at beta=6.0, for 300 MeV less tha n or similar to k less than or similar to 1 GeV, the propagator G(k) c an be fit to a continuum formula proposed by Gribov and others, which contains a mass scale b, presumably related to the hadronization mass scale. For higher momenta Gribov's model no longer provides a good fit , as G(k) tends rather to follow an inverse power law approximate to 1 /k(2+gamma). The results at beta=6.3 are consistent with those at beta =6.0, but only the high momentum region is accessible on this lattice. We find b in the range of 300 to 400 MeV and gamma about 0.7. Fits to particle + ghost expressions are also possible, often resulting in lo w values for chi(DF)(2), but the parameters are very poorly determined . On the other hand, at beta=5.7 (where we can only study momenta up t o 1 GeV) G(k) is best fit to a simple massive boson propagator with ma ss m. We argue that such a discrepancy may be related to a lack of sca ling for low momenta at beta=5.7. From our results, the study of corre lation functions in momentum space looks promising, especially because the data points in Fourier space turn out to be much less correlated than in real space.