It is shown that the universal behavior of the spacing distribution of
nearest energy levels at the metal-insulator Anderson transition is i
ndeed dependent on the boundary conditions. The spectral rigidity Sigm
a(2)(E) also depends on the boundary conditions, but this dependence v
anishes at high energy E. This implies that the multifractal exponent
D-2 of the participation ratio of wave functions in the bulk is not af
fected by the boundary conditions.