We have studied the insulator-superconductor transition (IST) by tuning the
thickness in quench-condensed Bi films. The resistive transitions of the s
uperconducting films are smooth and can be considered to represent "homogen
eous" films. The observation of an IST very close to the quantum resistance
for pairs, R-square(N) similar to h/4e(2) on several substrates supports t
his idea. The relevant length scales here are the localization length, and
the coherence length. However, at the transition, the localization length i
s much higher than the superconducting coherence length, contrary to expect
ation for a "homogeneous" transition. This suggests the invalidity of a pur
ely fermionic model for the transition. Furthermore, the current-voltage ch
aracteristics of the superconducting films are hysteretic, and show the fil
ms to be granular. The relevant energy scales here are the Josephson coupli
ng energy and the charging energy. However, Josephson coupling energies (E-
c) and the charging energies (E-c) at the IST, are found to obey the relati
on E-J < E-c. This is again contrary to expectation, for the IST in a granu
lar or inhomogeneous, system. Hence, a purely bosonic picture of the transi
tion is also inconsistent with our observations. We conclude that the IST o
bserved in our experiments may be either an intermediate case between the f
ermionic and bosonic mechanisms, or in a regime of charge and vortex dynami
cs for which a quantitative analysis has not yet been done. (C) 2001 Elsevi
er Science Ltd. All rights reserved.