The dielectric function data for CuGaSe2 and CuInSe2 have been modeled for
both perpendicular (E perpendicular to c) and parallel (E \ \ c) polarizati
ons. We employ the modified Adachi's model dielectric function model with v
ariable broadening. Variable broadening is accomplished by replacing the da
mping constant Gamma with the energy-dependent expression Gamma (E), where
the shape of the broadening function is determined by two adjustable model
parameters. In spite of one additional parameter per transition, this model
requires fewer parameters than the conventional Adachi's model to achieve
equal or better agreement with the experimental data. Our calculations give
the relative rms errors for the real and imaginary parts of the index of r
efraction, delta (n) and delta (k), equal to 0.9% and 9.5% for CuGaSe2 (E p
erpendicular to c), 0.8% and 7.3% for CuGaSe2 (E \ \ c), 1.1% and 3.0% for
CuInSe2 (E perpendicular to c), and 2.5% and 3.7% for CuInSe2 (E \ \ c), re
spectively.