Stress control in polycrystalline thin films—reduction in adatoms diffusion into grain boundaries via surfactants

2010 ◽  
Vol 96 (21) ◽  
pp. 211903 ◽  
Author(s):  
Yi Yang ◽  
Hanchen Huang ◽  
S. K. Xiang ◽  
Eric Chason
1994 ◽  
Vol 343 ◽  
Author(s):  
C. S. Nichols

ABSTRACTMany materials for engineering applications are used in polycrystalline form and contain grain boundaries with a range of structures and properties. However, most research on grain boundaries to date has focussed exclusively on symmetric coincidence site lattice interfaces. To go beyond descriptions for these simple interfaces and thence to an aggregate of grains and grain boundaries in a polycrystal will require a new approach. Here we discuss two models for properties of polycrystalline materials, including their advantages and drawbacks, and indicate the microstructural variables available to optimize properties.


2016 ◽  
Vol 119 (5) ◽  
pp. 055305 ◽  
Author(s):  
D. Magnfält ◽  
A. Fillon ◽  
R. D. Boyd ◽  
U. Helmersson ◽  
K. Sarakinos ◽  
...  

2008 ◽  
Vol 95 (1) ◽  
pp. 225-232 ◽  
Author(s):  
Tomoaki Sawabe ◽  
Koshi Okamura ◽  
Tomoki Sueyoshi ◽  
Takashi Miyamoto ◽  
Kazuhiro Kudo ◽  
...  

Author(s):  
D J H Cockayne ◽  
D R McKenzie

The study of amorphous and polycrystalline materials by obtaining radial density functions G(r) from X-ray or neutron diffraction patterns is a well-developed technique. We have developed a method for carrying out the same technique using electron diffraction in a standard TEM. It has the advantage that studies can be made of thin films, and on regions of specimen too small for X-ray and neutron studies. As well, it can be used to obtain nearest neighbour distances and coordination numbers from the same region of specimen from which HREM, EDS and EELS data is obtained.The reduction of the scattered intensity I(s) (s = 2sinθ/λ ) to the radial density function, G(r), assumes single and elastic scattering. For good resolution in r, data must be collected to high s. Previous work in this field includes pioneering experiments by Grigson and by Graczyk and Moss. In our work, the electron diffraction pattern from an amorphous or polycrystalline thin film is scanned across the entrance aperture to a PEELS fitted to a conventional TEM, using a ramp applied to the post specimen scan coils. The elastically scattered intensity I(s) is obtained by selecting the elastically scattered electrons with the PEELS, and collecting directly into the MCA. Figure 1 shows examples of I(s) collected from two thin ZrN films, one polycrystalline and one amorphous, prepared by evaporation while under nitrogen ion bombardment.


2019 ◽  
Author(s):  
D.O. Alikin ◽  
Y. Fomichov ◽  
S.P. Reis ◽  
A.S. Abramov ◽  
D.S. Chezganov ◽  
...  

1997 ◽  
Vol 296 (1-2) ◽  
pp. 114-117 ◽  
Author(s):  
O. Pesty ◽  
P. Canet ◽  
F. Lalande ◽  
H. Carchano ◽  
D. Lollman

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