The f and d electron density of states of the one-dimensional
Falicov-Kimball model are studied in the weak-coupling limit by exact
diagonalization calculations. The resultant behaviors are used to examine the
d-electron gap (Δd), the f-electron gap (Δf), and the
fd-electron gap (Δfd) as functions of the f-level energy Ef
and hybridization V. It is shown that the spinless Falicov-Kimball model
behaves fully differently for zero and finite hybridization between f and d
states. At zero hybridization the energy gaps do not coincide (Δd=Δf=Δfd), and the activation gap Δfd vanishes
discontinuously at some critical value of the f-level energy Efc. On the
other hand, at finite hybridization all energy gaps coincide and vanish
continuously at the insulator-metal transition point Ef=Efc. The
importance of these results for a description of real materials is discussed.Comment: 10 pages, 7 figures, LaTe