In this paper, we introduce a Ginzburg-Landau (GL) theory for the
extended-s and d-wave superconductors (SC) in granular systems that is
defined on a lattice. In contrast to the ordinary Abelian Higgs model (AHM)
that is a GL theory for the s-wave SC, Cooper-pair field (Higgs field) is put
on links of the lattice in the present model. By means of Monte-Carlo (MC)
simulations, we study phase structure, gauge-boson mass (the inverse magnetic
penetration depth) and density of instantons. In the ordinary {\em noncomapct}
U(1) AHM, there exists a second-order phase transition from the normal to SC
states and the gauge-boson mass develops continuously from the phase transition
point. In the present gauge system with link Higgs field, on the other hand,
phase transition to the SC state is of first order at moderate coupling
constants. The gauge-boson mass changes from vanishing to finite values
discontinuously at the phase transition points.Comment: 4 papges, 14 figure