Modified compensation model of CdTe

The traditional compensation model to explain the high resistivity properties of CdTe is based on the presence of a deep acceptor level of the cadmium vacancy in the middle of the band gap. A new compensation model based on a deep intrinsic donor level is presented. The compensation model is used together with an appropriate segregation model to calculate axial distributions of resistivity which are compared with spatially resolved resistivity measurements. The Te-antisite defect is discussed as a possible origin cause of this intrinsic defect, which is also supported by theoretical calculations.

[1]  K. Benz,et al.  Characterization of Ti and V doped CdTe by time dependent charge measurement (TDCM) and photoinduced current transient spectroscopy (PICTS) , 1995 .

[2]  K. Benz,et al.  Optically detected magnetic resonance investigations on titanium and vanadium ions in CdTe , 1995 .

[3]  J. Tregilgas,et al.  The kinetics of tellurium precipitation in Hg0.8Cd0.2Te , 1986 .

[4]  K. Benz,et al.  Studies of the compensation mechanism in CdTe grown from the vapour phase , 1995 .

[5]  K. Benz,et al.  Investigation of CdTe:Cl grown from the vapour phase under microgravity conditions with time dependent charge measurements and photoinduced current transient spectroscopy , 1995 .

[6]  G M Khattak,et al.  Characteristics of deep levels in n-type CdTe , 1991 .

[7]  W. Jantz,et al.  Contactless evaluation of semi-insulating GaAs wafer resistivity using the time-dependent charge measurement , 1991 .

[8]  Y. Marfaing Models of donor impurity compensation in cadmium telluride , 1977 .

[9]  P. Rudolph,et al.  New method for the determination of VCd concentrations in p-CdTe , 1993 .

[10]  P. Siffert,et al.  Status of semi-insulating cadmium telluride for nuclear radiation detectors , 1992 .

[11]  T. Schlesinger,et al.  Semiconductors for room temperature nuclear detector applications , 1995 .

[12]  Wang,et al.  Monte Carlo study of the liquid CdTe surface. , 1989, Physical review. B, Condensed matter.

[13]  Beatrice Fraboni,et al.  Deep energy levels in CdTe and CdZnTe , 1998 .

[14]  Jean Lajzerowicz,et al.  Gamma- and X-ray detectors manufactured from Cd1−xZnx Te grown by a high pressure bridgman method , 1993 .

[15]  R. Triboulet CdTe And CdTe : Hg alloys crystal growth using stoichiometric and off-stoichiometric zone passing techniques , 1977 .

[16]  M. Avrami Kinetics of Phase Change. I General Theory , 1939 .

[17]  R. Nitsche,et al.  Seeded vapour growth of cadmium telluride using focused radiation heating , 1985 .

[18]  W. Tiller,et al.  The redistribution of solute atoms during the solidification of metals , 1953 .

[19]  R. Davies,et al.  The role of deep‐level centers and compensation in producing semi‐insulating GaAs , 1983 .

[20]  N. Nachtrieb,et al.  The chemistry of imperfect crystals , 1973 .

[21]  G. Martin,et al.  Compensation mechanisms in GaAs , 1980 .

[22]  J. S. Blakemore,et al.  Transient photoconductivity measurements in semi‐insulating GaAs. I. An analog approach , 1987 .

[23]  Meyer,et al.  Identification of the chlorine A center in CdTe. , 1992, Physical review. B, Condensed matter.

[24]  Meyer,et al.  Identification of the cadmium vacancy in CdTe by electron paramagnetic resonance. , 1993, Physical review. B, Condensed matter.

[25]  N. V. Agrinskaya,et al.  Fermi level pinning in the middle of the band gap in CdTe: Cl crystals: Role of deep localized states , 1989 .

[26]  M. Schilfgaarde,et al.  Defects in ZnTe, CdTe, and HgTe: Total energy calculations , 1990 .