Brand, Christian; Tinnemann, Verena; Hanisch-Blicharski, Anja; Tajik, Mohammad; Fortmann, Jonas Darius; Kaßen, Alexander; Thiemann, Fabian; Horn-von Hoegen, Michael:
Non-Equilibrium Pathways for Excitation of Bulk and Surface Phonons through Anharmonic Coupling
2023
2023article/chapterOA Green
Physics (incl. Astronomy)Scientific institutes » Center for Nanointegration Duisburg-Essen (CENIDE)
Title in English:
Non-Equilibrium Pathways for Excitation of Bulk and Surface Phonons through Anharmonic Coupling
Author:
Brand, ChristianUDE
LSF ID
59817
ORCID
0000-0002-2984-4456ORCID iD
Other
connected with university
;
Tinnemann, VerenaUDE
LSF ID
55029
Other
connected with university
;
Hanisch-Blicharski, Anja;Tajik, Mohammad;Fortmann, Jonas DariusUDE
LSF ID
61635
ORCID
0000-0001-9887-5638ORCID iD
Other
connected with university
;
Kaßen, Alexander;Thiemann, FabianUDE
LSF ID
62299
ORCID
0000-0002-2903-2933ORCID iD
Other
connected with university
;
Horn-von Hoegen, MichaelUDE
GND
1201039908
LSF ID
10366
ORCID
0000-0003-0324-3457ORCID iD
Other
connected with university
corresponding author
Year of publication:
2023
Open Access?:
OA Green
arXiv.org ID
Language of text:
English

Abstract:

Upon impulsive optical excitation of solid-state materials, the non-equilibrium flow of energy from the excited electronic system to the lattice degrees of freedom typically happens in a few picoseconds. Here we identified the surface of thin Bi films grown on Si(001) as an additional subsystem which is excited much slower on a 100 ps timescale that is caused by decoupling due to mismatched phonon dispersions relations of bulk and surface. Anharmonic coupling among the phonon systems provides pathways for excitations which exhibits a 1/T-dependence causing a speed-up of surface excitation at higher temperatures. A quantitative justification is provided by phonon Umklapp processes from lattice thermal conductivity of the Bi bulk. Three-temperature model simulations reveal a pronounced non-equilibrium situation up to nanoseconds: initially, the surface is colder than the bulk, that situation is then inverted during cooling and the surface feeds energy back into the bulk phonon system.