Dopant redistribution and crystalline damage removal during rapid thermal annealing of Be and Mg implants in Ga0.47In0.53As

1987 ◽  
Vol 85 (3) ◽  
pp. 433-439 ◽  
Author(s):  
J.H. Wilkie ◽  
G.D.T. Spiller ◽  
I.D. Henning ◽  
B.J. Sealy
1985 ◽  
Vol 52 ◽  
Author(s):  
M. Tabasky ◽  
E. S. Bulat ◽  
B. M. Ditchek ◽  
M. A. Sullivan ◽  
S. Shatas

ABSTRACTRapid thermal annealing is used to form cobalt silicide directly on unimplanted as well as B, As, and P implanted wafers. The films are characterized by sheet resistance, X-ray diffraction, SEM, SIMS, and contact resistance measurements. The direct silicidation of cobalt on Si by rapid thermal annealing yields smooth, low resistivity films with minimal dopant redistribution.


1986 ◽  
Vol 48 (21) ◽  
pp. 1433-1435 ◽  
Author(s):  
N. S. Alvi ◽  
D. L. Kwong ◽  
C. G. Hopkins ◽  
S. G. Bauman

1987 ◽  
Vol 92 ◽  
Author(s):  
Tan-Hua Yu ◽  
Sujane Wang

ABSTRACTA buried p-layer in GaAs MESFET channel is successfully formed by (Si,Be) co-implantation and rapid thermal annealing process. The annealing cycle is optimized to activate Si and Be simultaneously and to minimize the dopant redistribution for precise dopant control. As a result, more than 80% activation efficiency for both Si and Be, as well as the greatly improved doping abruptness from 85 nm/decade to 65 nm/decade are achieved. Devices are fabricated and superior performance including sharper pinchoff, an increase of RF gain by 2–3dB and a 40% decrease in backgating effect is observed.


1986 ◽  
Vol 71 ◽  
Author(s):  
Archie Y.C. Chan

AbstractThe diffusion of ion-implanted dopants in silicon during rapid thermal annealing is modeled using the finite difference method.The change in impurity profile for an initial Pearson IV boron implant is negligible(less than 1 % change in junction depth) when the peak annealing temperature(TP ) is less than 1050 °C and its duration is shorter than 20 seconds. The dopant redistribution becomes significant(greater than 25 % change in junction depth) when Tp is greater than 1200 °C and its duration is longer than 40 seconds.The heatup and cooldown portions of the transient annealing cycle are found to have little effect on dopant redistribution provided that their rates are higher than 120 °C per second.


1988 ◽  
Vol 126 ◽  
Author(s):  
B. G. Streetman ◽  
A. Dodabalapur

ABSTRACTWe review the applications of ion implantation in several III-V materials, and rapid thermal annealing techniques to activate the implant and remove the crystalline damage. Ion implantation has become the preferred technique when selective area doping is necessary. It has been used successfully to fabricate n, n+, p, p+, and semi-insulating regions in III-V binary, ternary, and quaternary compounds, and multilayer structures. Ion implantation has also been used to produce layer mixing in multilayer structures, and superlattice disordering. The annealing step necessary to activate the implant and remove the crystalline damage is complicated by several factors such as incongruent evaporation of the group V element, layer mixing, and dopant redistribution. Rapid thermal annealing techniques, which typically employ anneal times between 1 second and 100 seconds, are generally more suitable than conventional furnace annealing. The short annealing times result in much less dopant redistribution, and reduced layer mixing in multilayer structures. Even for short annealing times, it is necessary to employ a protection scheme to suppress the loss of the group V element. Several such methods are discussed, including dielectric encapsulation, proximity techniques, and controlled ambient techniques.


2003 ◽  
Vol 27 (11) ◽  
pp. 1083-1086 ◽  
Author(s):  
H. Ito ◽  
T. Kusunoki ◽  
H. Saito ◽  
S. Ishio

2002 ◽  
Vol 716 ◽  
Author(s):  
G.Z. Pan ◽  
E.W. Chang ◽  
Y. Rahmat-Samii

AbstractWe comparatively studied the formation of ultra thin Co silicides, Co2Si, CoSi and CoSi2, with/without a Ti-capped and Ti-mediated layer by using rapid thermal annealing in a N2 ambient. Four-point-probe sheet resistance measurements and plan-view electron diffraction were used to characterize the silicides as well as the epitaxial characteristics of CoSi2 with Si. We found that the formation of the Co silicides and their existing duration are strongly influenced by the presence of a Ti-capped and Ti-mediated layer. A Ti-capped layer promotes significantly CoSi formation but suppresses Co2Si, and delays CoSi2, which advantageously increases the silicidation-processing window. A Ti-mediated layer acting as a diffusion barrier to the supply of Co suppresses the formation of both Co2Si and CoSi but energetically favors directly forming CoSi2. Plan-view electron diffraction studies indicated that both a Ti-capped and Ti-mediated layer could be used to form ultra thin epitaxial CoSi2 silicide.


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