  The angular dependence of the first-order phase transition (FOT) in the
vortex lattice in Bi$_{2}$Sr$_{2}$CaCu$_{2}$O$_{8}$ crystals was investigated
by a low frequency AC shielding technique (with the AC field $\parallel c$), in
which the static-field component parallel to $c$- ($H_{\perp}$) was varied with
the in-plane field $H_{\parallel}$ held constant. The linear decrease of the
FOT field $H_{\perp}^{FOT}$ with increasing $H_{\parallel}$ ends at a
temperature--dependent critical value of $H_{\parallel}$. A new transition,
marked by the abrupt drop of the $ab$-plane shielding current, appears at this
point. We draw a new phase diagram with $H_{\parallel}$ and $H_{\perp}$ field
components as coordinates; this features at least two distinct regions in the
vortex solid phase, that are determined by the different interplay between the
pancake vortex-- and Josephson vortex lattice.
