% 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{Varykhalov:874717,
author = {Varykhalov, A. and Freyse, F. and Aguilera, Irene and
Battiato, M. and Krivenkov, M. and Marchenko, D. and
Bihlmayer, G. and Blügel, S. and Rader, O. and
Sánchez-Barriga, J.},
title = {{E}ffective mass enhancement and ultrafast electron
dynamics of {A}u(111) surface state coupled to a quantum
well},
journal = {Physical review research},
volume = {2},
number = {1},
issn = {2643-1564},
address = {College Park, MD},
publisher = {APS},
reportid = {FZJ-2020-01629},
pages = {013343},
year = {2020},
abstract = {We show that, although the equilibrium band dispersion of
the Shockley-type surface state of two-dimensional Au(111)
quantum films grown on W(110) does not deviate from the
expected free-electron-like behavior, its nonequilibrium
energy-momentum dispersion probed by time- and
angle-resolved photoemission exhibits a remarkable kink
above the Fermi level due to a significant enhancement of
the effective mass. The kink is pronounced for certain
thicknesses of the Au quantum well and vanishes in the very
thin limit. We identify the kink as induced by the coupling
between the Au(111) surface state and emergent quantum-well
states which probe directly the buried gold-tungsten
interface. The signatures of the coupling are further
revealed by our time-resolved measurements which show that
surface state and quantum-well states thermalize together
behaving as dynamically locked electron populations. In
particular, relaxation of hot carriers following laser
excitation is similar for both surface state and
quantum-well states and much slower than expected for a bulk
metallic system. The influence of quantum confinement on the
interplay between elementary scattering processes of the
electrons at the surface and ultrafast carrier transport in
the direction perpendicular to the surface is shown to be
the reason for the slow electron dynamics.},
cin = {PGI-1 / JARA-FIT / IAS-1 / IEK-5 / JARA-HPC},
ddc = {530},
cid = {I:(DE-Juel1)PGI-1-20110106 / I:(DE-Juel1)VDB881 /
I:(DE-Juel1)IAS-1-20090406 / I:(DE-Juel1)IEK-5-20101013 /
$I:(DE-82)080012_20140620$},
pnm = {522 - Controlling Spin-Based Phenomena (POF3-522) / 142 -
Controlling Spin-Based Phenomena (POF3-142) / 143 -
Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-522 / G:(DE-HGF)POF3-142 /
G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000602699100007},
doi = {10.1103/PhysRevResearch.2.013343},
url = {https://juser.fz-juelich.de/record/874717},
}