Surface morphology and reconstructions of ultra thin Si films grown by solid-phase epitaxy

1997 ◽  
Vol 294 (1-2) ◽  
pp. 88-92 ◽  
Author(s):  
Z Zhang ◽  
M.A Kulakov ◽  
B Bullemer
1992 ◽  
Author(s):  
H. Ishiwara ◽  
H. Wakabayashi ◽  
K. Miyazaki ◽  
K. Fukao ◽  
A. Sawaoka

1997 ◽  
Vol 485 ◽  
Author(s):  
Claudine M. Chen ◽  
Harry A. Atwater

AbstractWith a selective nucleation and solid phase epitaxy (SNSPE) process, grain sizes of 10 μm have been achieved to date at 620°C in 100 nrm thick silicon films on amorphous SiO2, with potential for greater grain sizes. Selective nucleation occurs via a thin film reaction between a patterned array of 20 rnm thick indium islands which act as heterogeneous nucleation sites on the amorphous silicon starting material. Crystal growth proceeds by lateral solid phase epitaxy from the nucleation sites, during the incubation time for random nucleation. The largest achievable grain size by SNSPE is thus approximately the product of the incubation time and the solid phase epitaxy rate. Electronic dopants, such as B, P, and Al, are found to enhance the solid phase epitaxy rate and affect the nucleation rate.


1985 ◽  
Vol 24 (Part 2, No. 7) ◽  
pp. L513-L515 ◽  
Author(s):  
Hiroshi Ishiwara ◽  
Akihiro Tamba ◽  
Hiroshi Yamamoto ◽  
Seijiro Furukawa

1992 ◽  
Vol 280 ◽  
Author(s):  
Katsuhiro Uesugi ◽  
Masamichi Yoshimura ◽  
Takafumi Yao ◽  
Tomoshige Sato ◽  
Takashi Sueyoshi ◽  
...  

ABSTRACTScanning tunneling microscopy (STM) is used to investigate the surface morphology of Ar+-ion bombarded Si(100) surfaces and to elucidate the very beginning stages of solid phase epitaxy (SPE) processes of the Ar+-ion bombarded Si surfaces. The Ar+-ion bombarded Si surface consists of hillocks of 1–2 nm in diameter and 0.35–0.75 nm in height. The onset of SPE initiates at around 590°C, at which temperature a (2×2) structure surrounded by amorphous regions is partially observed on terraces of the surface. During annealing at 590–620°C, the areas of the c(2×2) and c(4×4) reconstruction surrounded by amorphous regions develops. New defect models for the (2×2) and c(4×4) structures are proposed w here alternating arrangements of the buckled dimers together with missing dimer defects are considered. On the other hand, after thermal annealing of the Ar+-ion bombarded Si at 830°C for 10 sec, terraces of (2×1) and (1×2) orientations arc observed on the surface, and pyramidal structures on a nanometer-scale which consists of double-layer step edges (dimer rows perpendicular to terrace edge) arc observed.


1988 ◽  
Vol 63 (4) ◽  
pp. 1065-1069 ◽  
Author(s):  
I. Mizushima ◽  
H. Kuwano ◽  
T. Hamasaki ◽  
T. Yoshii ◽  
M. Kashiwagi

2006 ◽  
Vol 352 (28-29) ◽  
pp. 2986-2992 ◽  
Author(s):  
S. Gąsiorek ◽  
P.K. Sahoo ◽  
K.P. Lieb ◽  
S. Dhar ◽  
T. Sajavaara ◽  
...  

1995 ◽  
Vol 34 (Part 1, No. 1) ◽  
pp. 20-24 ◽  
Author(s):  
Jeong-Hee Oh ◽  
Duck-Young Kim ◽  
Hiroshi Ishiwara

1977 ◽  
Vol 30 (11) ◽  
pp. 598-600 ◽  
Author(s):  
A. Christou ◽  
J. E. Davey ◽  
H. M. Day ◽  
H. B. Dietrich

1985 ◽  
Author(s):  
Hiroshi Ishiwara ◽  
Akihiro Tamba ◽  
Seijiro Furukawa

Sign in / Sign up

Export Citation Format

Share Document