Hopping-Randomwalk in Random Fractal Fluctuation and the Application to Photoluminescence Decay in Amorphous Si : H and Nanometer Film

2002 ◽  
Vol 230 (1) ◽  
pp. 15-20 ◽  
Author(s):  
Y. Ando ◽  
A. Sasaki ◽  
M. Shingai ◽  
K. Murayama
Author(s):  
E. I. Alessandrini ◽  
M. O. Aboelfotoh

Considerable interest has been generated in solid state reactions between thin films of near noble metals and silicon. These metals deposited on Si form numerous stable chemical compounds at low temperatures and have found applications as Schottky barrier contacts to silicon in VLSI devices. Since the very first phase that nucleates in contact with Si determines the barrier properties, the purpose of our study was to investigate the silicide formation of the near noble metals, Pd and Pt, at very thin thickness of the metal films on amorphous silicon.Films of Pd and Pt in the thickness range of 0.5nm to 20nm were made by room temperature evaporation on 40nm thick amorphous Si films, which were first deposited on 30nm thick amorphous Si3N4 membranes in a window configuration. The deposition rate was 0.1 to 0.5nm/sec and the pressure during deposition was 3 x 10 -7 Torr. The samples were annealed at temperatures in the range from 200° to 650°C in a furnace with helium purified by hot (950°C) Ti particles. Transmission electron microscopy and diffraction techniques were used to evaluate changes in structure and morphology of the phases formed as a function of metal thickness and annealing temperature.


Author(s):  
M. Libera ◽  
J.A. Ott ◽  
K. Siangchaew ◽  
L. Tsung

Channeling occurs when fast electrons follow atomic strings in a crystal where there is a minimum in the potential energy (1). Channeling has a strong effect on high-angle scattering. Deviations in atomic position along a channel due to structural defects or thermal vibrations increase the probability of scattering (2-5). Since there are no extended channels in an amorphous material the question arises: for a given material with constant thickness, will the high-angle scattering be higher from a crystal or a glass?Figure la shows a HAADF STEM image collected using a Philips CM20 FEG TEM/STEM with inner and outer collection angles of 35mrad and lOOmrad. The specimen (6) was a cross section of singlecrystal Si containing: amorphous Si (region A), defective Si containing many stacking faults (B), two coherent Ge layers (CI; C2), and a contamination layer (D). CBED patterns (fig. lb), PEELS spectra, and HAADF signals (fig. lc) were collected at 106K and 300K along the indicated line.


1991 ◽  
Vol 138 (3) ◽  
pp. 226 ◽  
Author(s):  
C.Y. Chang ◽  
J.W. Hong ◽  
Y.K. Fang

1981 ◽  
Vol 42 (C4) ◽  
pp. C4-463-C4-466
Author(s):  
A. Madan ◽  
W. Czubatyj ◽  
J. Yang ◽  
J. McGill ◽  
S. R. Ovshinsky

2016 ◽  
Vol 213 (9) ◽  
pp. 2446-2451 ◽  
Author(s):  
Klemens Ilse ◽  
Thomas Schneider ◽  
Johannes Ziegler ◽  
Alexander Sprafke ◽  
Ralf B. Wehrspohn

1995 ◽  
Vol 32 (3) ◽  
pp. 295-306 ◽  
Author(s):  
A. Sturm ◽  
A. Wiedenmann ◽  
H. Wollenberger
Keyword(s):  

Nanoscale ◽  
2021 ◽  
Vol 13 (8) ◽  
pp. 4678-4684
Author(s):  
Yan Cheng ◽  
Yonghui Zheng ◽  
Zhitang Song

A 3D nano-bicontinuous structure consisting of a reversible Sb2Te3 phase and amorphous Si phase is visualized. The amorphous Si frame is stable and the Sb2Te3 nano areas switch between the a- and f-structure.


1979 ◽  
Vol 20 (2) ◽  
pp. 716-728 ◽  
Author(s):  
Eva C. Freeman ◽  
William Paul

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