We investigate the quantum phase transition in a one-dimensional chain
of ultrasmall superconducting grains, considering both the self-and j
unction capacitances. At zero temperature, the system is transformed i
nto a two-dimensional system of classical vortices, where the junction
capacitance introduces anisotropy in the interaction between vortices
. This leads to the superconductor-insulator transition of the Berezin
skii-Kosterlitz-Thouless type, as the ratios of the Josephson coupling
energy to the charging energies are varied. It is found that the junc
tion capacitance plays a role similar to that of dissipation and tends
to suppress quantum fluctuations; nevertheless the insulator region s
urvives even for arbitrarily large values of the junction capacitance.