TY - JOUR
T1 - Orbital and lattice dynamics in pyroxenes
AU - Popovic, Z.V.
AU - Konstantinovic, Milan
AU - Dohcevic-Mitrovic, Z
AU - Isobe, M.
AU - Ueda, Y.
A2 - Van den Berghe, Sven
N1 - Score = 10
PY - 2006/5/1
Y1 - 2006/5/1
N2 - We have studied with infrared reflectivity and Raman scattering techniques the orbital and lattice dynamics, and the origin of the
phase transitions in the pyroxene compounds NaMSi2O6 (with M ¼ Ti, V, and Cr). In the quasi one-dimensional S ¼ 1/2 system
NaTiSi2O6 we observe the anomalous high-temperature phonon broadenings and large changes of the phonon energies and line-widths
across the phase transition at 210 K. The phonon anomalies originate from an orbital order–disorder type of the phase transition, which
we describe as an orbital analogue of the spin-Peierls phase transition. In the S ¼ 1 NaVSi2O6 system orbital degrees of freedom are
strongly suppressed since both of the active t2g orbitals are occupied and the magnetic excitations are well described within the
Heisenberg model, indicating that at TN ¼ 19K this system orders antiferromagnetically. The NaCrSi2O6 has a fully polarized t2g core,
no orbital degrees of freedom, and no anomalous phonon broadening in the Raman spectra.
AB - We have studied with infrared reflectivity and Raman scattering techniques the orbital and lattice dynamics, and the origin of the
phase transitions in the pyroxene compounds NaMSi2O6 (with M ¼ Ti, V, and Cr). In the quasi one-dimensional S ¼ 1/2 system
NaTiSi2O6 we observe the anomalous high-temperature phonon broadenings and large changes of the phonon energies and line-widths
across the phase transition at 210 K. The phonon anomalies originate from an orbital order–disorder type of the phase transition, which
we describe as an orbital analogue of the spin-Peierls phase transition. In the S ¼ 1 NaVSi2O6 system orbital degrees of freedom are
strongly suppressed since both of the active t2g orbitals are occupied and the magnetic excitations are well described within the
Heisenberg model, indicating that at TN ¼ 19K this system orders antiferromagnetically. The NaCrSi2O6 has a fully polarized t2g core,
no orbital degrees of freedom, and no anomalous phonon broadening in the Raman spectra.
KW - Orbital ordering
KW - Pyroxenes
KW - Infrared and Raman spectra
UR - http://ecm.sckcen.be/OTCS/llisapi.dll/open/ezp_76420
UR - http://knowledgecentre.sckcen.be/so2/bibref/3979
U2 - 10.1016/j.physb.2006.01.469
DO - 10.1016/j.physb.2006.01.469
M3 - Article
SN - 0921-4526
VL - 378-380
SP - 1072
EP - 1074
JO - Physica B: Condensed Matter
JF - Physica B: Condensed Matter
T2 - Proceedings of the International Conference on Strongly Correlated Electron Systems - SCES 2005
Y2 - 1 August 2005 through 1 August 2005
ER -