A high-pressure Cs IV phase of alkali metals is equivalent to the beta -Sn(II) structure predicted previously. At higher pressures, the beta -Sn(II) phase tends to become more stable than beta -Sn(i), which corresponds to the well known beta -Sn-type structure as a high-pressure phase of diamond-type structure. Numerical calculations of the relative stability of diamond or zinc-blende, beta -Sn(I) and beta -Sn(II) structures are performed for Si and GaSb, and of BCC, FCC, beta -Sn(I) and beta -Sn(II) structures for Rb and Cs using a perturbational treatment based on the pseudopotential formalism. Numerical results for the transition pressure, relative volume, volume discontinuity and transition heat are then discussed together with the observed data.
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