We have investigated the electrical and optical properties of the deep levels responsible for the 1.4-1.5 eV luminescence band usually observed in II-VI compounds. We compared the energy levels found by cathodoluminescence and junction spectroscopy methods for semi-insulating ͑CdTe:Cl and Cd 0.8 Zn 0.2 Te͒ and semiconducting samples ͑undoped CdTe͒. The techniques utilized were deep level transient spectroscopy ͑DLTS͒ on semiconducting samples and photoinduced current transient spectroscopy and photo-DLTS on high resistivity materials. These last two techniques are complementary and allow the determination of the trap character ͑donor/acceptor͒. Three acceptor levels are seen in the electrical transient data at E v ϩ0.12, 0.14, and 0.16 eV with hole capture cross sections of 2ϫ10
Ϫ16, 1ϫ10
Ϫ16, and 4ϫ10 Ϫ17 cm 2 , respectively. The lowest level is seen only in Cl doped material corroborating the literature optical and electron spin resonance identification of a level at E v ϩ0.12 eV as being a V Cd ϩCl Te donor-acceptor pair center. All three levels may be present in the 1.4 eV luminescence band. © 1996 American Institute of Physics. ͓S0003-6951͑96͒04949-2͔Cadmium-telluride is a wide band gap II-VI compound that has promising applications as an x-and ␥-ray detector, thanks to its high average atomic number and to its good mobility-lifetime product, for both electrons and holes. In order to obtain the high resistivity (Ͼ10 8 ⍀cm͒ required for such applications, CdTe crystals are usually grown in Te-rich conditions and doped during growth with group III ͑Ga,In͒ or group VII ͑Cl,Br͒ donors. Due to the Te-rich growth conditions, the dominant intrinsic defect are Cd vacancies (V Cd ) and related complexes.1,2 One of the most interesting complexes is the so called A center, a single acceptor formed by a cadmium vacancy and a donor.3 It has been proposed that it plays a major role in the compensation process, namely in the neutralization of the native acceptor defects (V Cd ) which provide most of the free carriers.1,4,5 Some doubts have been recently cast on models that describe A center as the sole center responsible for the high resistivity of compensated materials: as its energy level in the band gap is located at approximately E v ϩ0.15 eV, it is too shallow to account for the pinning of the Fermi level near midgap, which is observed in semi-insulating ͑SI͒ materials. 6 In order to understand its actual role in the determination of the electrical and optical properties of the material, we have studied the carrier capture and emission processes of the deep levels located at approximately E v ϩ0.15 eV, obtaining information on the origin of the detected traps.Luminescence investigations recently carried out on CdTe;Cl provided evidence, for the existence of A center in CdTe:Cl and suggested its relation to the band located at ϳ1.4 eV.7 Junction spectroscopy methods, such as thermally stimulated current ͑TSC͒ and photoinduced current transient spectroscopy ͑PICTS͒, have also revealed single deep energy levels scattere...