Temperature dependence of the magnetic excitations in the modified triangular induced moment antiferromagnet RbFeBr3 at the soft mode point (abstract)

1991 ◽  
Vol 69 (8) ◽  
pp. 6232-6232 ◽  
Author(s):  
D. Visser ◽  
B. Dorner ◽  
A. Harrison
2019 ◽  
Vol 33 (08) ◽  
pp. 1950061
Author(s):  
K. A. Brekhov ◽  
N. A. Ilyin ◽  
E. D. Mishina ◽  
P. A. Prudkovskii ◽  
G. Kh. Kitaeva

In this paper, we present the results of the temperature dependence studies of the photoinduced phonon mode which appears in a ferroelectric-semiconductor Sn2P2S6 (SPS) crystal under the influence of femtosecond laser pulses. We show that its behavior reminds the soft mode one near the phase transition. However, the observed decrease in the oscillation frequency in the vicinity of Curie temperature Tc is much weaker than previously reported. This can be explained by the shadowing of the pure soft mode by its interaction with other photoinduced modes.


1999 ◽  
Vol 196-197 ◽  
pp. 473-474
Author(s):  
A. Metz ◽  
N.M. Pyka ◽  
M. Loewenhaupt ◽  
A.A. Menovsky ◽  
R. van de Kamp

2002 ◽  
Vol 718 ◽  
Author(s):  
Yizhak Yacoby ◽  
Yakov Girshberg

AbstractWe present a comprehensive model of ferroelectricity in oxygen perovskite crystals that account quantitatively for both displacive like and order-disorder like properties. The model assumes that in the paraelectric phase, the system has a soft mode, interacting with spontaneous disordered off-center displacements. The resulting theory is shown to quantitatively explain the properties of two representative perovskites: KNbO3 and PbTiO3. We have further extended this theory to explain the properties of mixed incipient ferroelectrics with small concentrations of ferroelectricity inducing ions such as KTa1-xNbxO3. The model quantitatively reproduces the basic experimental data in the quantum regime: the temperature dependence of the inverse dielectric function, the impurity and temperature dependence of the renormalized soft mode vibrational frequency and the impurity concentration dependence of the transition temperature Tc. In particular we show that, the critical concentration for Tc=0 is determined by the ion tunneling frequency, the bare soft mode parameters and the pseudospin - phonon coupling constant.


2005 ◽  
Vol 364 (1-4) ◽  
pp. 55-70 ◽  
Author(s):  
U. Köbler ◽  
A. Hoser ◽  
W. Schäfer

1981 ◽  
Vol 52 (3) ◽  
pp. 2231-2233 ◽  
Author(s):  
J. W. Cable ◽  
N. Wakabayashi ◽  
R. M. Nicklow

2011 ◽  
Author(s):  
Trilok Chandra Upadhayay ◽  
Mayank Joshi ◽  
P. K. Bajpai ◽  
K. S. Ojha ◽  
K. N. Singh

2012 ◽  
Vol 2012 ◽  
pp. 1-5 ◽  
Author(s):  
Hamit Yurtseven ◽  
Sema Şen

The temperature dependence of the spontaneous polarizationPis calculated in the ferroelectric phase of KH2PO4(KDP) at atmospheric pressure (TC= 122 K). Also, the dielectric constantεis calculated at various temperatures in the paraelectric phase of KDP at atmospheric pressure. For this calculation ofPandε, by fitting the observed Raman frequencies of the soft mode, the microscopic parameters of the pure tunnelling model are obtained. In this model, the proton-lattice interaction is not considered and the collective proton mode is identified with the soft-mode response of the system. Our calculations show that the spontaneous polarization decreases continuously in the ferroelectric phase as approaching the transition temperatureTC. Also, the dielectric constant decreases with increasing temperature and it diverges in the vicinity of the transition temperature (TC= 122 K) for KDP according to the Curie-Weiss law.


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