ic960167m_si_001.pdf (274.4 kB)
Download fileSyntheses, Structural Analyses, and Unusual Magnetic Properties of Ba2CoSi2O7 and BaCo2Si2O7
journal contribution
posted on 1996-06-05, 00:00 authored by Richard D. Adams, Christophe Payen, Timir DattaThe compounds Ba2CoSi2O7,
1, and BaCo2Si2O7,
2, were obtained by heating mixtures of BaCO3,
CoCO3, and
SiO2 in the proper stoichiometries to 1300 °C for 48 h.
Both materials were characterized by single-crystal
X-ray diffraction and magnetization measurements on powder and
partially oriented single crystals. Each cobalt
ion in 1 is surrounded by four oxygen atoms derived from the
[Si2O7]6- groups in
the form of a distorted tetrahedron.
The cobalt ions are bridged by O−Si−O and O−Si−O−Si−O
groups from the
[Si2O7]6- ions in
an extended
two-dimensional arrangement. The barium ions are arranged in
layers that run parallel to the
Co[Si2O7] layers.
In 2 each cobalt ion is also surrounded by an
arrangement of four oxygen atoms derived from the
Si2O7 groups
in a distorted tetrahedral shape. These tetrahedra are linked into
chains through the sharing of one of the oxygen
atoms from the Si2O7 groups. The
CoO4 chains are crosslinked via O−Si−O−Si−O bridges
from the Si2O7
groups. The barium ions occupy channels that run parallel to the
crystallographic c-axis. Curie−Weiss
behaviors
and temperature independent paramagnetisms (TIP) coexist in the ranges
40−300 K and 100−300 K for 1 and
2, respectively. For both compounds the values of the
Curie constant and TIP are consistent with tetrahedral
Co(II) ions having three unpaired electrons. While compound
1 remains paramagnetic down to 5 K, 2
undergoes
a transition into a state having a field-induced weak ferromagnetic
response at Tc = 21 K. The weak
ferromagnetic
properties below Tc can be explained by spin
canting and spontaneous domain formation. The canting angle
is
estimated to be about 5° at 5 K. Interestingly, 2
could represent the first example among the tetrahedral
Co(II)
compounds with the transition temperature (Tc
= 21 K) being higher than the zero-field splitting of the
4A2
electronic ground state. Crystal data: for 1, formula
Ba2CoSi2O7, a =
8.450(1) Å, b = 10.729(1) Å, c =
8.474(1) Å, β = 111.365(8)°, monoclinic, space group =
C2/c, Z = 4; for 2,
formula BaCo2Si2O7,
a = 7.2131(6) Å,
b = 12.781(1) Å, c = 13.762(1) Å,
β = 90.299(8)°, monoclinic, space group =
C2/c, Z = 8.