TY - JOUR
T1 - Structural phase transition in deuterated benzil C14 D10 O2
T2 - Neutron inelastic scattering
AU - Goossens, D. J.
AU - Welberry, T. R.
AU - Hagen, M. E.
AU - Fernandez-Baca, J. A.
PY - 2006
Y1 - 2006
N2 - Neutron inelastic scattering has been used to examine the structural phase transition in deuterated benzil C14 D10 O2. The transition in benzil, in which the unit cell goes from a trigonal P 31 21 unit cell above TC to a cell doubled P 21 unit cell below TC, leads to the emergence of a Bragg peak at the M -point of the high temperature Brillouin zone. It has previously been suggested that the softening of a transverse optic phonon at the Γ -point leads to the triggering of an instability at the M -point causing the transition to occur. This suggestion has been investigated by measuring the phonon spectrum at the M -point for a range of temperatures above TC and the phonon dispersion relation along the Γ-M direction just above TC. It is found that the transverse acoustic phonon at the M -point is of lower energy than the Γ -point optic mode and has a softening with temperature as T approaches TC from above that is much faster than that of the Γ -point optic mode. This behavior is inconsistent with the view that the Γ -point mode is responsible for triggering the phase transition. Rather the structural phase transition in benzil appears to be driven by a conventional soft TA mode at the M -point.
AB - Neutron inelastic scattering has been used to examine the structural phase transition in deuterated benzil C14 D10 O2. The transition in benzil, in which the unit cell goes from a trigonal P 31 21 unit cell above TC to a cell doubled P 21 unit cell below TC, leads to the emergence of a Bragg peak at the M -point of the high temperature Brillouin zone. It has previously been suggested that the softening of a transverse optic phonon at the Γ -point leads to the triggering of an instability at the M -point causing the transition to occur. This suggestion has been investigated by measuring the phonon spectrum at the M -point for a range of temperatures above TC and the phonon dispersion relation along the Γ-M direction just above TC. It is found that the transverse acoustic phonon at the M -point is of lower energy than the Γ -point optic mode and has a softening with temperature as T approaches TC from above that is much faster than that of the Γ -point optic mode. This behavior is inconsistent with the view that the Γ -point mode is responsible for triggering the phase transition. Rather the structural phase transition in benzil appears to be driven by a conventional soft TA mode at the M -point.
UR - http://www.scopus.com/inward/record.url?scp=33646237600&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.73.134116
DO - 10.1103/PhysRevB.73.134116
M3 - Article
SN - 1098-0121
VL - 73
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 13
M1 - 134116
ER -