Gj. Redhammer et al., Structure and Mossbauer spectroscopy of barbosalite Fe2+Fe23+ (PO4)(2)(OH)(2) between 80 K and 300 K, PHYS CHEM M, 27(6), 2000, pp. 419-429
Natural barbosalite Fe2+Fe23+ (PO4)(2)(OH)(2) from Bull Moose Mine, South D
akota, U.S.A., having ideal composition, was investigated with single cryst
al X-ray diffraction techniques, Mossbauer spectroscopy and SQUID magnetome
try to redetermine crystal structure, valence state of iron and evolution o
f Fe-57 Mossbauer parameter and to propose the magnetic structure at low te
mperatures. At 298 K the title compound is monoclinic, space group P2(1)/n,
a(o) = 7.3294(16) Angstrom, b(o) = 7.4921(17) Angstrom, c(o) = 7.4148(18)
Angstrom, beta = 118.43(3)degrees, Z = 2. No crystallographic phase transit
ion was observed between 298 K and 110 K. Slight discontinuities in the tem
perature dependence of lattice parameters and bond angles in the range betw
een 150 K and 180 K are ascribed to the magnetic phase transition of the ti
tle compound. At 298 K the Mossbauer spectrum of the barbosalite shows two
paramagnetic components, typical for Fe2+ and Fe3+ in octahedral coordinati
on; the area ratio Fe3+/Fe2+ is exactly two, corresponding to the ideal val
ue. Both the Fe2+ and the Fe3+ sublattice order magnetically below 173 K an
d exhibit a fully developed magnetic pattern at 160 K. The electric field g
radient at the Fe site is distorted from axial symmetry with the direction
of the magnetic field nearly perpendicular to V-zz, the main component of t
he electric field gradient. The temperature dependent magnetic susceptibili
ty exhibits strong antiferromagnetic ordering within the corner-sharing Fe3
+-chains parallel to [101], whereas ferromagnetic coupling is assumed withi
n the face-sharing [110] and [-110] Fe3+-Fe2+-Fe3+ trimer, connecting the F
e3+-chains to each other.