CM Seminar @ICTP Stasi Seminar Room Friday 9 September at 11.30 a.m. - Roman MARTONAK
Condensed Matter Section
cm at ictp.it
Tue Sep 6 09:07:02 CEST 2016
Condensed Matter and Statistical Physics Seminar
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Friday, 9 September at 11.30 a.m.
Luigi Stasi Seminar Room, first floor, Leonardo building
Roman MARTONAK
Comenius University, Dept. of Experimental Physics
Bratislava, Slovak Republic
Title: New High Pressure Layered Phases of CS2 and SiS2
Abstract:
CS2 and SiS2 belong to the important family of IVâVI AB2 compounds
made of light elements which includes archetypal systems such as CO2 and
SiO2. In solid CS2 a series of structural transitions was observed at
high pressure upon compression of the Cmca molecular crystal, eventually
resulting in a disordered tetrahedral structure [1] which did not allow
an accurate structural determination. We applied an ab initio
evolutionary search [2] and found a new layered tetrahedral P21/c
structure, of especially high stability, and characterized by pairs of
edge-sharing tetrahedra [3]. Unlike tetrahedrally coordinated CO2
phases, this structure undergoes a semiconductor-metal transition at the
relatively low pressure of 30-50 GPa [3], a transition which is in
agreement with experiment [1]. This layered structure appears to be a
likely candidate for the phase found experimentally above 30 GPa in
Ref.[1]. With that in mind we suggest that by applying high pressure at
low temperature one could perhaps prepare this phase with higher
crystallinity thus allowing for better structural comparisons with our
prediction, and to this end we calculated the Raman and IR spectra of
the new phase. Wondering moreover whether similar phases could appear in
different compounds of the same family, we extended our interest to
SiS2. Strikingly, the very same P21/c layered structure which we
predicted for CS2 turned out to be recently observed (and named HP1) in
SiS2 [4], a finding which points to a new link in the high-pressure
crystal chemistry of this family of compounds. Actually, the
high-pressure phase diagram of SiS2 is currently known only up to cca 6
GPa, featuring several tetrahedrally coordinated phases (NP, HP1, HP2,
HP3), but nothing seems to be known about the structural and electronic
evolution of SiS2 at higher pressures. By means of ab initio
calculations combined with evolutionary structure searching [5] we now
predict three new low-enthalpy phases of SiS2 with space groups P-3m1,
P63mc and R-3m [6]. In all three phases, the Si coordination has
switched from 4 to 6 and, interestingly, all these new structures are
layered, consisting of sheets formed by edge-sharing octahedra (SiS6
units). The most stable P-3m1 phase (with a single SiS2 layer per unit
cell) is isostructural to CdI2, where all sheets are directly above each
other. It becomes stable above 6 GPa and at low pressures is
semiconducting with an indirect band gap. The gap closes with increasing
pressure leading to metallization around 30 GPa. New high pressure
measurements will be called for to address these predictions. Facile
sliding of these high pressure layered structures should also be of
interest.
[1] R. P. Dias, C.-S. Yoo, M. Kim, J. S. Tse, Phys. Rev. B 84, 144104
(2011).
[2] A. Oganov , C. Glass, J. Chem. Phys. 124, 244704 (2006).
[3] S. S. Naghavi, Y. Crespo, R. MartoÅák, E. Tosatti, Phys. Rev. B
91, 224108 (2015).
[4] J. Evers, P. Mayer, et al., Inorg. Chem. 54, 1240 (2015).
[5] D. Lonie, E. Zurek, Comput. Phys. Commun. 182, 372 (2011) [6] D.
PlaÅ¡ienka, R. MartoÅák, E. Tosatti, in preparation.
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