We studied the defect physics in CuInSe2, a prototype chalcopyrite sem
iconductor. We showed that (i) it takes much less energy to form a Cu
vacancy in CuInSe2 than to form cation vacancies in II-VI: compounds (
ii) defect formation energies vary considerably both with the Fermi en
ergy and with the chemical potential of the atomic species, and (iii)
the defect pairs such as (2V(Cu)(-)+In-Cu(2+)) and (2Cu(In)(2-)+In-Cu(
2+)) have particularly low formation energies (under certain condition
s, even exothermic). Using (i)-(iii), we (a) explain the existence of
unusual ordered compounds CuIn5Se8, CuIn3Se5, Cu2In4Se7, and Cu3In5Se9
as a repeat of a single unit of (2V(Cu)(-)+In-Cu(2+)) pairs for each
n=4, 5, 7, and 9 units, respectively, of CuInSe2; (b) attribute the ve
ry efficient p-type self-doping ability of CuInSe2 to the exceptionall
y low formation energy of the shallow defect Cu vacancies; (c) explain
ed in terms of an electronic passivation of the In-Cu(2+) by 2V(Cu)(-)
the electrically benign character of the large defect population in C
uInSe2. Our calculation leads to a set of new assignment of the observ
ed defect transition energy levels in the band gap. The calculated lev
el positions agree rather well with available experimental data. [S016
3-1829(98)01516-1].