Texture analysis of CoGe2 alloy films grown heteroepitaxially on GaAs(100) using partially ionized beam deposition

1997 ◽  
Vol 81 (11) ◽  
pp. 7261-7267 ◽  
Author(s):  
K. E. Mello ◽  
S. P. Murarka ◽  
T.-M. Lu ◽  
S. L. Lee
1996 ◽  
Vol 427 ◽  
Author(s):  
K. E. Mello ◽  
S. P. Murarkak ◽  
S. L. Lee ◽  
T.-M. Lu

AbstractThe Partially ionized beam (PIB) deposition technique was used to deposit CoGe2 thin films heteroepitaxially on GaAs(100) substrates in a conventional vacuum. For the CoGe2(001)/GaAs(100) system, which leads to an Ohmic contact, a substrate temperature of 280°C and ∼1200 eV Ge+ ions are required. Reducing the ion energy or lowering the substrate temperature both produce a different orientation in the films. Films deposited at 280°C with a zero accelerating potential for the ions, and those deposited at 200°C with -1200 eV Ge+ ions result in a CoGe2(100)//GaAs(100) type orientation domination, leading to rectifying behavior.


1990 ◽  
Vol 68 (7) ◽  
pp. 3619-3624 ◽  
Author(s):  
P. Bai ◽  
G.‐R. Yang ◽  
T.‐M. Lu

1991 ◽  
Vol 70 (11) ◽  
pp. 6766-6773 ◽  
Author(s):  
T. C. Nason ◽  
J. F. McDonald ◽  
T.‐M. Lu

1987 ◽  
Vol 51 (24) ◽  
pp. 1992-1994 ◽  
Author(s):  
C.‐H. Choi ◽  
R. A. Harper ◽  
A. S. Yapsir ◽  
T.‐M. Lu

1996 ◽  
Vol 80 (10) ◽  
pp. 5759-5764 ◽  
Author(s):  
P. K. Wu ◽  
S. Dabral ◽  
G.‐R. Yang ◽  
B. Gittleman ◽  
C. Li ◽  
...  

1989 ◽  
Vol 54 (24) ◽  
pp. 2443-2445 ◽  
Author(s):  
P. Li ◽  
A. S. Yapsir ◽  
K. Rajan ◽  
T.‐M. Lu

1988 ◽  
Vol 64 (4) ◽  
pp. 2206-2208 ◽  
Author(s):  
W. I. Lee ◽  
J. Wong ◽  
J. M. Borrego ◽  
T.‐M. Lu

1989 ◽  
Vol 66 (9) ◽  
pp. 4519-4521 ◽  
Author(s):  
G.‐R. Yang ◽  
P. Bai ◽  
T.‐M. Lu ◽  
W. M. Lau

1989 ◽  
Vol 157 ◽  
Author(s):  
P. Bai ◽  
CH. SteinbrÜChel ◽  
T.-M. Lu

ABSTRACTIn ion-assisted deposition techniques such as partially ionized beam deposition, ions derived from the depositing material itself concurrently bombard the surface during thin film growth. The ion percentage in the deposition beam ranges from less than 0.1% to 100% (Ion Beam Deposition) with the ion energy varying between a few eV and several keV. When the sputtering yield of the self-sputtering is greater than one, there is a critical ion percentage, for a given ion energy, above which no net deposition can be obtained. The self-sputtering yield is shown to have a square root dependence on the ion energy above the threshold energy by fitting the experimental data obtained from the literature. The critical ion percentage for Al, Cu, Au, Ag, and C is then calculated and plotted as a function of the ion energy so that deposition and no-deposition regions are illustrated in terms of the ion energy and ion percentage.


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