We investigate the order-disorder transition line from a Bragg glass to an
amorphous vortex glass in the H-T phase diagram of three-dimensional type-I
I superconductors taking into account both pinning-caused and thermal fluct
uations of the vortex lattice. Our approach is based on the Lindemann crite
rion and on results of the collective pinning theory and generalizes previo
us work of other authors. It is shown that the shapes of the order-disorder
transition line and the vortex-lattice melting curve are determined only b
y the Ginzburg number. which characterizes thermal fluctuations, and by a p
arameter which describes the strength of the quenched disorder in the flux-
fine lattice. In the framework of this unified approach we obtain the H-T p
hase diagrams for both conventional and high-T-c superconductors. Several w
ell-known experimental results concerning the fishtail effect and the phase
diagram of high-T-c superconductors are naturally explained by assuming th
at a peak effect in the critical current density versus H signalizes the or
der-disorder transition line in superconductors with point defects.