Nucleation and Initial-Growth Behavior of Thin-Film Deposits

1967 ◽  
Vol 4 (5) ◽  
pp. 209-218 ◽  
Author(s):  
B. Lewis ◽  
D. S. Campbell
2012 ◽  
Vol 22 (30) ◽  
pp. 15037 ◽  
Author(s):  
Woongkyu Lee ◽  
Jeong Hwan Han ◽  
Sang Woon Lee ◽  
Sora Han ◽  
Woo Jin Jeon ◽  
...  

Crystals ◽  
2019 ◽  
Vol 9 (7) ◽  
pp. 373 ◽  
Author(s):  
Roland Resel ◽  
Markus Koini ◽  
Jiri Novak ◽  
Steven Berkebile ◽  
Georg Koller ◽  
...  

A 30 nm thick quinquephenyl (5P) film was grown by molecular beam deposition on a Cu(110)(2×1)O single crystal surface. The thin film morphology was studied by light microscopy and atomic force microscopy and the crystallographic structure of the thin film was investigated by X-ray diffraction methods. The 5P molecules crystallise epitaxially with (201)5P parallel to the substrate surface (110)Cu and with their long molecular axes parallel to [001]Cu. The observed epitaxial alignment cannot be explained by lattice matching calculations. Although a clear minimum in the lattice misfit exists, it is not adapted by the epitaxial growth of 5P crystals. Instead the formation of epitaxially oriented crystallites is determined by atomic corrugations of the substrate surface, such that the initially adsorbed 5P molecules fill with its rod-like shape the periodic grooves of the substrate. Subsequent crystal growth follows the orientation and alignment of the molecules taken within the initial growth stage.


CrystEngComm ◽  
2019 ◽  
Vol 21 (38) ◽  
pp. 5779-5788 ◽  
Author(s):  
Yuan-Chang Liang ◽  
Chen-Shiang Hung

The crystal growth properties of hydrothermally derived WO3 nanorods were investigated using various WO3 thin-film seed layers.


2008 ◽  
Vol 354 (45-46) ◽  
pp. 5014-5017
Author(s):  
W.L. Li ◽  
Q.G. Chi ◽  
J.M. Wang ◽  
W.D. Fei

2001 ◽  
Vol 226-230 ◽  
pp. 1610-1612 ◽  
Author(s):  
M Futamoto ◽  
Y Hirayama ◽  
Y Honda ◽  
N Inaba

2005 ◽  
Vol 871 ◽  
Author(s):  
Th. B. Singh ◽  
N. Marjanovic ◽  
G. J. Matt ◽  
S. Günes ◽  
N. S. Sariciftci ◽  
...  

AbstractElectron mobilities were studied as a function of thin-film growth conditions in hot wall epitaxially grown C60 based field-effect transistors. Mobilities in the range of ∼ 0.5 to 6 cm2/Vs are obtained depending on the thin-film morphology arising from the initial growth conditions. Moreover, the field-effect transistor current is determined by the morphology of the film at the interface with the dielectric, while the upper layers are less relevant to the transport. At high electric fields, a non-linear transport has been observed. This effect is assigned to be either because of the dominance of the contact resistance over the channel resistance or because of the gradual move of the Fermi level towards the band edge as more and more empty traps are filled due to charge injection.


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