https://doi.org/10.1007/s100510170299
High frequency sound and the boson peak in amorphous silica
Institut für Physik, Johannes Gutenberg-Universität,
Staudinger Weg 7, 55099 Mainz, Germany
Corresponding author: a kob@ldv.univ-montp2.fr
Received:
27
June
2000
Revised:
9
January
2001
Published online: 15 February 2001
We present the results of extensive molecular dynamics computer
simulations in which the high frequency dynamics of silica, i.e. for
frequencies THz, is investigated in the viscous liquid state
as well as in the glass state. We characterize the properties of high
frequency sound modes by analyzing
and
, the
longitudinal and transverse current correlation function, respectively.
For wave-vectors q> 0.4 Å-1 the spectra are sitting on top of a
flat background.
The dynamic structure factor
exhibits for q> 0.23 Å-1
a boson peak which is located nearly independent of q
around 1.7 THz and for which the intensity scales approximately
linearly with temperature. We show that the low frequency part of the boson
peak is mainly due to the elastic scattering of transverse acoustic modes
with frequencies around 1 THz. The strength of this scattering depends on
q and is largest around q=1.7 Å-1, the location of the first sharp
diffraction peak in the static structure factor. By studying
for different system sizes we show that strong finite size effects are
present in the low frequency part of the boson peak in that for small
systems part of its intensity is missing. We discuss the consequences
of these finite size effects for the structural relaxation.
PACS: 61.20.Lc – Time-dependent properties; relaxation / 61.20.Ja – Computer simulation of liquid structure / 02.70.Ns – Molecular dynamics and particle methods / 64.70.Pf – Glass transitions
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag, 2001