scholarly journals Circular test structure for the determination of piezoelectric constants of Sc x Al 1−x N thin films applying Laser Doppler Vibrometry and FEM simulations

2015 ◽  
Vol 222 ◽  
pp. 301-308 ◽  
Author(s):  
P.M. Mayrhofer ◽  
H. Euchner ◽  
A. Bittner ◽  
U. Schmid
Author(s):  
Jamie Chilles ◽  
William Frier ◽  
Abdenaceur Abdouni ◽  
Marcello Giordano ◽  
Orestis Georgiou

2014 ◽  
Vol 363 ◽  
pp. 179-187 ◽  
Author(s):  
Ronnie Varghese ◽  
Ravindranath Viswan ◽  
Keyur Joshi ◽  
Safoura Seifikar ◽  
Yuan Zhou ◽  
...  

2007 ◽  
Vol 16 (3) ◽  
pp. 675-683 ◽  
Author(s):  
Luigi La Spina ◽  
Alexander W. van Herwaarden ◽  
Hugo Schellevis ◽  
Wim H. A. Wien ◽  
Neboja Nenadovic ◽  
...  

2002 ◽  
Author(s):  
Enrico Esposito ◽  
M Navarri ◽  
S. Papalini ◽  
M Pontillo ◽  
Enrico P. Tomasini ◽  
...  

Author(s):  
R. M. Anderson ◽  
T. M. Reith ◽  
M. J. Sullivan ◽  
E. K. Brandis

Thin films of aluminum or aluminum-silicon can be used in conjunction with thin films of chromium in integrated electronic circuits. For some applications, these films exhibit undesirable reactions; in particular, intermetallic formation below 500 C must be inhibited or prevented. The Al films, being the principal current carriers in interconnective metal applications, are usually much thicker than the Cr; so one might expect Al-rich intermetallics to form when the processing temperature goes out of control. Unfortunately, the JCPDS and the literature do not contain enough data on the Al-rich phases CrAl7 and Cr2Al11, and the determination of these data was a secondary aim of this work.To define a matrix of Cr-Al diffusion couples, Cr-Al films were deposited with two sets of variables: Al or Al-Si, and broken vacuum or single pumpdown. All films were deposited on 2-1/4-inch thermally oxidized Si substrates. A 500-Å layer of Cr was deposited at 120 Å/min on substrates at room temperature, in a vacuum system that had been pumped to 2 x 10-6 Torr. Then, with or without vacuum break, a 1000-Å layer of Al or Al-Si was deposited at 35 Å/s, with the substrates still at room temperature.


Author(s):  
D. R. Liu ◽  
S. S. Shinozaki ◽  
R. J. Baird

The epitaxially grown (GaAs)Ge thin film has been arousing much interest because it is one of metastable alloys of III-V compound semiconductors with germanium and a possible candidate in optoelectronic applications. It is important to be able to accurately determine the composition of the film, particularly whether or not the GaAs component is in stoichiometry, but x-ray energy dispersive analysis (EDS) cannot meet this need. The thickness of the film is usually about 0.5-1.5 μm. If Kα peaks are used for quantification, the accelerating voltage must be more than 10 kV in order for these peaks to be excited. Under this voltage, the generation depth of x-ray photons approaches 1 μm, as evidenced by a Monte Carlo simulation and actual x-ray intensity measurement as discussed below. If a lower voltage is used to reduce the generation depth, their L peaks have to be used. But these L peaks actually are merged as one big hump simply because the atomic numbers of these three elements are relatively small and close together, and the EDS energy resolution is limited.


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