  Polycrystalline samples of A$_x$V$_2$Al$_{20}$ (A = Ce, Th, U, Np, Pu; 0.7 =<
x =< 1.0) actinide intermetallics were synthesized using the arc-melting
method. Crystal structure studies were performed by means of powder x-ray
diffraction and the Rietveld refinement method. All studied compounds
crystallize in the CeCr$_{2}$Al$_{20}$-type structure (space group Fd-3m, no.
227) with the actinide or Ce atom located in the oversized cage formed by Al
atoms. Comparison of the crystallographic results with the reported data for
LnV$_{2}$Al$_{20}$ (Ln = lanthanoids) counterparts reveals distinctly different
behavior of the lanthanide- and actinide-bearing compounds. This difference is
suggested to be caused by fairly localized character of the 4f electrons,
whereas itinerant character of the 5f electrons is likely seen for U- and
Np-containing phases. Magnetic susceptibility and specific heat measurements
did not reveal any magnetic ordering in U$_{0.8}$V$_{2}$Al$_{20}$,
Np$_{0.8}$V$_{2}$Al$_{20}$ and Pu$_{0.8}$V$_{2}$Al$_{20}$ down to 2.5 K. A
small anomaly in low-temperature specific heat of Ce$_{0.8}$V$_{2}$Al$_{20}$,
U$_{0.8}$V$_{2}$Al$_{20}$, and Np$_{0.8}$V$_{2}$Al$_{20}$ is observed, likely
arising from a low-energy Einstein mode.
