The effects of water on oxide and interface trapped charge generation in thermal SiO2 films

Water was diffused into very dry thermal SiO2 films under conditions such that the penetration of water related electron trapping centers was of the order of the oxide thickness. In both dry oxides and water diffused oxides, production of negative bulk oxide charge Qot and positive interface charge Qit by an avalanche‐injected electron flux was observed. The efficiencies of both processes were enhanced by water indiffusion. Analysis of the kinetics of charge generation indicated that production of trapped electron centers (Qot ) was required for subsequent production of interface states and charge (Qit ). Models for both processes are discussed. We suggest that inelastic collisions of conduction electrons with the trapped electron centers releases mobile hydrogen atoms or excitons. The mobile species migrate to the Si–SiO2 interface and form states and fixed charge.

[1]  S. Lai,et al.  Two‐carrier nature of interface‐state generation in hole trapping and radiation damage , 1981 .

[2]  D. Young Characterization of electron traps in SiO2 as influenced by processing parameters , 1981 .

[3]  Max J. Schulz,et al.  Insulating Films on Semiconductors , 1981 .

[4]  F. B. McLean A Framework for Understanding Radiation-Induced Interface States in SiO2 MOS Structures , 1980, IEEE Transactions on Nuclear Science.

[5]  P. S. Winokur,et al.  Interface-State Generation in Radiation-Hard Oxides , 1980, IEEE Transactions on Nuclear Science.

[6]  Radiation-induced trapping centers in thin silicon dioxide films , 1980 .

[7]  Walter C. Johnson,et al.  Relationship between trapped holes and interface states in MOS capacitors , 1980 .

[8]  B. E. Deal Standardized terminology for oxide charges associated with thermally oxidized silicon , 1980, IEEE Transactions on Electron Devices.

[9]  K. Yamabe,et al.  The Effect of Hot Electron Injection on Interface Charge Density at the Silicon to Silicon Dioxide Interface , 1980 .

[10]  Hisham Z. Massoud,et al.  Electron trapping in SiO2 at 295 and 77 °K , 1979 .

[11]  Donald R. Young,et al.  Exciton or hydrogen diffusion in SiO2 , 1979 .

[12]  P. S. Winokur,et al.  Two‐stage process for buildup of radiation‐induced interface states , 1979 .

[13]  D. Dimaria,et al.  THE PROPERTIES OF ELECTRON AND HOLE TRAPS IN THERMAL SILICON DIOXIDE LAYERS GROWN ON SILICON , 1978 .

[14]  D. Dimaria,et al.  Determination of insulator bulk trapped charge densities and centroids from photocurrent‐voltage charactersitcs of MOS structures , 1976 .

[15]  A. Goetzberger,et al.  Interface states on semiconductor/insulator surfaces , 1976 .

[16]  R. A. Gdula,et al.  The Effects of Processing on Hot Electron Trapping in SiO2 , 1976 .

[17]  W. C. Johnson Study of Electronic Transport and Breakdown in Thin Insulating Films , 1976 .

[18]  D. Dimaria,et al.  Capture and emission of electrons at 2.4-eV-deep trap level in SiO2films , 1975 .

[19]  E. Irene The Effects of Trace Amounts of Water on the Thermal Oxidation of Silicon in Oxygen , 1974 .

[20]  J. M. Andrews,et al.  Electrochemical Charging of Thermal SiO2 Films by Injected Electron Currents , 1971 .

[21]  C. N. Berglund,et al.  Photoinjection Studies of Charge Distributions in Oxides of MOS Structures , 1971 .

[22]  C. N. Berglund,et al.  Avalanche Injection of Electrons into Insulating SiO2 Using MOS Structures , 1970 .

[23]  C. N. Berglund,et al.  AVALANCHE INJECTION CURRENTS AND CHARGING PHENOMENA IN THERMAL SiO2 , 1969 .

[24]  Richard Williams,et al.  Photoemission of Electrons from Silicon into Silicon Dioxide , 1965 .