Electronic properties of (Co, Ag) self-organized nano dots on Au(1 1 1) vicinal surfaces

2007 ◽  
Vol 254 (1) ◽  
pp. 45-49 ◽  
Author(s):  
C. Didiot ◽  
Y. Fagot-Revurat ◽  
S. Pons ◽  
B. Kierren ◽  
D. Malterre ◽  
...  
2000 ◽  
Vol 447 (1-3) ◽  
pp. L152-L156 ◽  
Author(s):  
V. Repain ◽  
J.M. Berroir ◽  
S. Rousset ◽  
J. Lecoeur

2015 ◽  
Vol 44 (2) ◽  
pp. 126-128 ◽  
Author(s):  
Kyosuke Isoda ◽  
Tomonori Abe ◽  
Ippei Kawamoto ◽  
Makoto Tadokoro

2002 ◽  
Vol 88 (20) ◽  
Author(s):  
A. Pimpinelli ◽  
V. Tonchev ◽  
A. Videcoq ◽  
M. Vladimirova

1999 ◽  
Vol 201-202 ◽  
pp. 101-105 ◽  
Author(s):  
D. Martrou ◽  
P. Gentile ◽  
N. Magnea

2014 ◽  
Vol 16 (26) ◽  
pp. 13329-13339 ◽  
Author(s):  
Mauricio J. Prieto ◽  
Emilia A. Carbonio ◽  
Shadi Fatayer ◽  
Richard Landers ◽  
Abner de Siervo

Morphology and electronic properties of Pt nanostructures are influenced by the underlying Au surface orientation and surface alloy formation, respectively.


2007 ◽  
Vol 40 (5) ◽  
pp. 874-882 ◽  
Author(s):  
Geoffroy Prévot ◽  
Alessandro Coati ◽  
Bernard Croset ◽  
Yves Garreau

It is demonstrated that grazing-incidence X-ray diffraction is a direct tool for measuring the elastic displacement modes near the surface of a crystal. Due to the fact that X-ray diffraction is a Fourier transform of the electronic density, and thus, of the atomic positions, elastic displacement modes appear as additional spots in the reciprocal space. Their characteristics can be directly derived from the elastic constants of the material. Measuring the amplitude of the diffracted wave for these peaks allows direct determination of the force distribution at the surface, which is at the origin of the elastic displacements. Various examples of such determinations are given for self-organized surfaces and for vicinal surfaces.


2009 ◽  
Vol 256 (3) ◽  
pp. 924-928 ◽  
Author(s):  
E. Thune ◽  
A. Boulle ◽  
D. Babonneau ◽  
F. Pailloux ◽  
W. Hamd ◽  
...  

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