Combined influence of chemostimulator oxides V2O5 and MnO2 introduced via the gas phase on InP thermal oxidation

2015 ◽  
Vol 85 (4) ◽  
pp. 796-801
Author(s):  
I. Ya. Mittova ◽  
N. N. Tretyakov ◽  
V. F. Kostryukov ◽  
B. V. Sladkopevtsev
Keyword(s):  
2007 ◽  
Vol 52 (10) ◽  
pp. 1498-1502 ◽  
Author(s):  
V. F. Kostryukov ◽  
V. R. Pshestanchik ◽  
I. A. Donkareva ◽  
B. L. Agapov ◽  
S. I. Lopatin ◽  
...  
Keyword(s):  

2011 ◽  
Vol 51 (6) ◽  
pp. 448-453 ◽  
Author(s):  
R. R. Grigoryan ◽  
S. D. Arsentev ◽  
A. A. Mantashyan

2016 ◽  
Vol 50 (18) ◽  
pp. 10106-10113 ◽  
Author(s):  
Nirmala K. Dharmarathne ◽  
John C. Mackie ◽  
Eric M. Kennedy ◽  
Michael Stockenhuber
Keyword(s):  

1994 ◽  
Vol 342 ◽  
Author(s):  
John M. Grant

ABSTRACTA comparison study of the effectiveness of in-situ vapor/gas phase cleaning versus conventional wet RCA based cleaning has been performed. The effectiveness of the cleans were compared using Surface Photo-Voltage (SPV) measurements of the quality of a 70Å gate dielectric. Dielectrics grown in oxygen by Rapid Thermal Oxidation (RTO) were measured using SPV. The vapor/gas phase cleaning processes studied have three steps corresponding to the baths in a conventional RCA-based clean. A clean using O2 was used to clean the organic contaminants normally cleaned in the SC-1 bath, a C12 based step corresponded to the SC-2 solution, and an HF/alcohol etch was used to remove the oxide normally etched using buffered HF. It was seen that temperature control of the cleaning chamber walls is necessary to insure reproducible processes and reasonable pump down times. Measurements by SPV indicate that dielectrics grown after vapor-gas phase cleaning have lower interface trap densities than oxides grown after an RCA-based clean.


2001 ◽  
Vol 697 ◽  
Author(s):  
Takashi Kawamoto ◽  
Yukihiro Shimogaki

AbstractZrO2 films were investigated as high-k gate insulators for possible gate dielectric applications. These thin films were deposited by chemical vapor deposition (CVD). We had investigated kinetics of ZrO2-CVD reaction system and thermal stability of ZrO2 film deposited from zirconium-tetra-tertiary-butoxide (ZTB) and tetrakis-diethylamio-zirconium (TDEAZ) as Zr source. In the case of ZTB, ZTB decomposed into two active intermediate precursors by gas phase reaction. These intermediate precursors also contributed to the film growth. The step coverage, the contents of carbon and oxygen, and film structures depended on the growth precursor contributed to the film growth. Film structures also depended on the deposition temperature. As the films subjected to the rapid thermal oxidation annealing, the film structure changed amorphous into cubic and then into monoclinic. However, in the case of the films deposited at 300°C, the film structure kept amorphous state after 900°C annealing. On the other hand, in the case of TDEAZ, TDEAZ directly deposited on the growing surface and the decomposition of TDEAZ by gas phase reaction did not exist. The films deposited by TDEAZ contained more carbon than by ZTB. The film structure kept amorphous state independent of the deposition temperature. As the films subjected to the rapid thermal oxidation annealing, the film structure changed amorphous into monoclinic and then into amorphous again. This structural change resulted from the decrease of the impurity contents of the residual nitrogen and the residual carbon and the increase of the content of silicon diffused from the substrate in the ZrO2 films.


Author(s):  
Richard E. Hartman ◽  
Roberta S. Hartman ◽  
Peter L. Ramos

The action of water and the electron beam on organic specimens in the electron microscope results in the removal of oxidizable material (primarily hydrogen and carbon) by reactions similar to the water gas reaction .which has the form:The energy required to force the reaction to the right is supplied by the interaction of the electron beam with the specimen.The mass of water striking the specimen is given by:where u = gH2O/cm2 sec, PH2O = partial pressure of water in Torr, & T = absolute temperature of the gas phase. If it is assumed that mass is removed from the specimen by a reaction approximated by (1) and that the specimen is uniformly thinned by the reaction, then the thinning rate in A/ min iswhere x = thickness of the specimen in A, t = time in minutes, & E = efficiency (the fraction of the water striking the specimen which reacts with it).


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