scholarly journals Hydrogen intercalation of epitaxial graphene and buffer layer probed by mid-infrared absorption and Raman spectroscopy

AIP Advances ◽  
2018 ◽  
Vol 8 (4) ◽  
pp. 045015 ◽  
Author(s):  
J. Kunc ◽  
M. Rejhon ◽  
P. Hlídek
2010 ◽  
Vol 645-648 ◽  
pp. 623-628 ◽  
Author(s):  
Christian Riedl ◽  
Camilla Coletti ◽  
Takayuki Iwasaki ◽  
Ulrich Starke

In this report we review how intrinsic drawbacks of epitaxial graphene on SiC(0001) such as n-doping and strong electronic influence of the substrate can be overcome. Besides surface transfer doping from a strong electron acceptor and transfer of epitaxial graphene from SiC(0001) to SiO2 the most promising route is to generate quasi-free standing epitaxial graphene by means of hydrogen intercalation. The hydrogen moves between the (6p3×6p3)R30◦ reconstructed initial carbon (so-called buffer) layer and the SiC substrate. The topmost Si atoms which for epitaxial graphene are covalently bound to this buffer layer, are now saturated by hydrogen bonds. The buffer layer is turned into a quasi-free standing graphene monolayer, epitaxial monolayer graphene turns into a decoupled bilayer. The intercalation is stable in air and can be reversed by annealing to around 900 °C. This technique offers significant advances in epitaxial graphene based nanoelectronics.


2012 ◽  
Vol 717-720 ◽  
pp. 649-652 ◽  
Author(s):  
Markus Ostler ◽  
Roland J. Koch ◽  
Florian Speck ◽  
Felix Fromm ◽  
Hendrik Vita ◽  
...  

Epitaxial graphene (EG) grown on SiC(0001) resides on the so-called buffer layer. This carbon rich (6√3×6√3)R30° reconstruction is covalently bound to the topmost silicon atoms of the SiC. Decoupling the graphene buffer layer from the SiC interface is a well studied topic since successful intercalation has been shown for hydrogen [1-3]. Recently, intercalation was also shown for oxygen [4, 5]. We present ARPES, XPS and Raman spectroscopy studies to determine the quality of oxygen intercalated buffer layer samples in terms of decoupling and integrity of the transformed graphene layer. The decoupling effect is demonstrated by ARPES measurements showing a graphene-like π band. XPS shows whether the oxidation takes place in the buffer layer or at the interface. Raman spectroscopy is well suited to investigate oxygen induced defects in graphene-like material.


2012 ◽  
Vol 111 (11) ◽  
pp. 114307 ◽  
Author(s):  
K. Grodecki ◽  
J. A. Blaszczyk ◽  
W. Strupinski ◽  
A. Wysmolek ◽  
R. Stępniewski ◽  
...  

2016 ◽  
Vol 108 (5) ◽  
pp. 051605 ◽  
Author(s):  
P. Dharmaraj ◽  
P. Justin Jesuraj ◽  
K. Jeganathan

2006 ◽  
Vol 75 (2) ◽  
pp. 023703 ◽  
Author(s):  
Hidekazu Okamura ◽  
Masato Matsubara ◽  
Koichiro Tanaka ◽  
Kazutoshi Fukui ◽  
Mitsushi Terakami ◽  
...  

The Analyst ◽  
2018 ◽  
Vol 143 (8) ◽  
pp. 1735-1757 ◽  
Author(s):  
Matthew J. Baker ◽  
Hugh J. Byrne ◽  
John Chalmers ◽  
Peter Gardner ◽  
Royston Goodacre ◽  
...  

This review examines the state-of-the-art of clinical applications of infrared absorption and Raman spectroscopy, outstanding challenges, and progress towards translation.


1998 ◽  
Vol 533 ◽  
Author(s):  
Ran Liu ◽  
Stefan Zollner ◽  
Ming Liaw ◽  
David O'meara ◽  
Nigel Cave

AbstractRaman scattering studies were carried out on epi Si/Si1-xGex (x = 0.1 to 0.3) heterostructures consisting of a thin Si cap layer (100 - 400 A˚), a grade-down Si1-xGex layer, a constant Si1-xGex, buffer layer and a grade-up graded Si1-xGex layer on (100) oriented Si substrates. Different Ge composition, Si1-xGex layer thicknesses and thermal treatment were used to achieve different relaxation in the Si1-xGex layers. It has been revealed that, to a very good approximation, the absolute strains in the cap Si and constant Si1-xGex layers follow a simple sum-rule that is imposed by the lattice mismatch between unstrained Si and completely relaxed Si1-x Gex. This sum rule can be used to determine the Ge composition and stresses in both cap Si and constant Si1-xGex layers. Excellent agreement was found between the theoretical curve obtained with LO phonon strain coefficient b=−930cm−1 and the experimental total strain for all samples, regardless of the degree of the relaxation of the grade-up Si1-xGex layer.


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