% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Sforzini:188581,
author = {Sforzini, J. and Nemec, L. and Denig, T. and Stadtmüller,
B. and Lee, T.-L. and Kumpf, C. and Subach, Sergey and
Starke, U. and Rinke, P. and Blum, V. and Posseik, Francois
and Tautz, Frank Stefan},
title = {{A}pproaching {T}ruly {F}reestanding {G}raphene: {T}he
{S}tructure of {H}ydrogen-{I}ntercalated {G}raphene on
6{H}−{S}i{C}(0001)},
journal = {Physical review letters},
volume = {114},
number = {10},
issn = {1079-7114},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2015-01932},
pages = {106804},
year = {2015},
abstract = {We measure the adsorption height of hydrogen-intercalated
quasifreestanding monolayer graphene on the (0001) face of
6H silicon carbide by the normal incidence x-ray standing
wave technique. A density functional calculation for the
full (63√×63√)−R30° unit cell, based on a van der
Waals corrected exchange correlation functional, finds a
purely physisorptive adsorption height in excellent
agreement with experiments, a very low buckling of the
graphene layer, a very homogeneous electron density at the
interface, and the lowest known adsorption energy per atom
for graphene on any substrate. A structural comparison to
other graphenes suggests that hydrogen-intercalated graphene
on 6H−SiC(0001) approaches ideal graphene.},
cin = {PGI-3},
ddc = {550},
cid = {I:(DE-Juel1)PGI-3-20110106},
pnm = {142 - Controlling Spin-Based Phenomena (POF3-142)},
pid = {G:(DE-HGF)POF3-142},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000352073400018},
pubmed = {pmid:25815955},
doi = {10.1103/PhysRevLett.114.106804},
url = {https://juser.fz-juelich.de/record/188581},
}