Temperature- and pressure-dependent lattice behaviour of RbFe(MoO₄)₂

TY - JOUR

T1 - Temperature- and pressure-dependent lattice behaviour of RbFe(MoO4)2

AU - Waskowska, A.

AU - Gerward, L.

AU - Olsen, Janus Staun

AU - Morgenroth, W.

AU - Maczka, M.

AU - Hermanowicz, K.

PY - 2010/2/10

Y1 - 2010/2/10

N2 - Trigonal RbFe(MoO4)2 is a quasi-two-dimensional antiferromagnet on a triangular lattice below TN = 3.8K, The crystal exhibits also a structural phase transition at Tc = 190K related to symmetry change from P3̄m1 to P3̄. We present the temperature-and pressure-dependent characteristics of this material in the context of ambiguous opinions on the symmetry and crystal properties below Tc. A single-crystal x-ray diffraction shows that the temperature-dependent evolution of the unit cell in the range 100-300K is strongly anisotropic with markedly discontinuous changes at Tc. The transition is connected with a spontaneous strain developing in effect of the volume decrease. The structure releases the strain by rotation of corner-sharing rigid MoO4 and FeO6 polyhedra in the (a,b) basal plane. The temperature dependence of the IR vibrational wavenumbers exhibits weak changes near Tc, which are consistent with the symmetry transformation from P3̄m1 to P3̄. High-pressure x-ray powder diffraction indicates that the material is extremely soft but with some stiffening at high pressure. The zero-pressure bulk modulus is B0 = 7.9(6)GPa and the pressure derivative is B 0′ = 10(1). The compression curve can be described by a single equation of state, corresponding to the trigonal cell, up to 5GPa. An amorphization appearing above 5GPa and increasing gradually on further pressure increase suggests the thermodynamic instability of the high-pressure structure.

AB - Trigonal RbFe(MoO4)2 is a quasi-two-dimensional antiferromagnet on a triangular lattice below TN = 3.8K, The crystal exhibits also a structural phase transition at Tc = 190K related to symmetry change from P3̄m1 to P3̄. We present the temperature-and pressure-dependent characteristics of this material in the context of ambiguous opinions on the symmetry and crystal properties below Tc. A single-crystal x-ray diffraction shows that the temperature-dependent evolution of the unit cell in the range 100-300K is strongly anisotropic with markedly discontinuous changes at Tc. The transition is connected with a spontaneous strain developing in effect of the volume decrease. The structure releases the strain by rotation of corner-sharing rigid MoO4 and FeO6 polyhedra in the (a,b) basal plane. The temperature dependence of the IR vibrational wavenumbers exhibits weak changes near Tc, which are consistent with the symmetry transformation from P3̄m1 to P3̄. High-pressure x-ray powder diffraction indicates that the material is extremely soft but with some stiffening at high pressure. The zero-pressure bulk modulus is B0 = 7.9(6)GPa and the pressure derivative is B 0′ = 10(1). The compression curve can be described by a single equation of state, corresponding to the trigonal cell, up to 5GPa. An amorphization appearing above 5GPa and increasing gradually on further pressure increase suggests the thermodynamic instability of the high-pressure structure.

U2 - 10.1088/0953-8984/22/5/055406

DO - 10.1088/0953-8984/22/5/055406

M3 - Journal article

C2 - 21386344

SN - 0953-8984

VL - 22

SP - 055406

JO - Journal of Physics: Condensed Matter

JF - Journal of Physics: Condensed Matter

IS - 5

ER -