Abstract
We examine the density-functional theory of macroscopic insulators, obtained in the large-cluster limit or under periodic boundary conditions. For polar crystals, we find that the two procedures are not equivalent. In a large-cluster case, the exact exchange-correlation potential acquires a homogeneous ``electric field'' which is absent from the usual local approximations, and the Kohn-Sham electronic system becomes metallic. With periodic boundary conditions, such a field is forbidden, and the polarization deduced from Kohn-Sham wavefunctions is incorrect even if the exact functional is used.
Original language | English |
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Pages (from-to) | 294-297 |
Number of pages | 3 |
Journal | Physical Review Letters |
Volume | 78 |
Issue number | 2 |
DOIs | |
Publication status | Published - 13 Jan 1997 |