Communication
Dalton Transactions
expected from the relatively low and competing values of the
magnetic exchange constants.
In summary, this work is one of the notable examples of
utilizing in situ generated carbonato linkers to form a discrete
cubic coordination cluster of fascinating magnetic behavior,
revealing the flexibility and utility of this linker for future syn-
thesis and magnetic material applications. A new octanuclear
cubic coordination cluster type has been prepared through the
assembly of H2bpmp− chelated Ni(II) ions and imidazole
capping ligands. The four faces of the cubic cluster contain
four µ4-carbonato ligands, which are derived from atmospheric
CO2 fixation. Magnetic studies indicate the presence of com-
peting magnetic interactions mediated by the carbonate
bridge. The antiferromagnetic exchange across the face diag-
onal of the cubic cluster dominates the magnetic behavior,
resulting in the spin-singlet ground state.
Fig. 3 Temperature dependence of χT for 1. The solid red curve rep-
resents the best simulation of the experimental data. Inset: temperature
dependence of inverse magnetic susceptibility of 1, with the Curie–
Weiss fit shown as a solid red line.
(Fig. 3, inset). Fitting this part of the data to the Curie–Weiss
law resulted in the Curie constant of 10.39(2) emu K mol−1 per
cubic cluster, i.e. ∼1.30(2) emu K mol−1 per Ni2+ ion. This
value is larger than the spin-only value of 1.00 emu K mol−1
expected for the S = 1 Ni2+ ion, indicating orbital contribution
to the total magnetic moment, as is well known for Ni(II) com-
plexes.25 The Weiss constant obtained from the linear fit is
negative, θ = –37.3(3) K, suggesting the presence of dominant
antiferromagnetic interactions between Ni2+ ions. Neverthe-
less, the magnetic exchange coupling in this cluster is far
more complicated. This conjecture can be made based on the
earlier detailed work by Fondo et al.15 on the magnetic pro-
perties of a tetranuclear carbonato-bridged Ni(II) complex with
bonding topology that essentially represents one face of the
Ni8 cubic cluster discussed herein. According to the report on
the tetranuclear complex and using the high symmetry of our
complex, we can identify three magnetic exchange pathways: a
ferromagnetic exchange within each Ni2 dimer (J1 > 0), a ferro-
magnetic exchange along the long cube edge (J2 > 0), and an
antiferromagnetic exchange along the face diagonal of the
cube (J3 < 0). The latter two interactions are mediated by the
Acknowledgements
AKG is thankful to the Council of Scientific and Industrial
Research, New Delhi, India for financial support. The authors
also thank DST, New Delhi, for providing the Single Crystal
X-ray Diffractometer facility in the Department of Chemistry,
IIT Kharagpur under its FIST program. VB acknowledges the
Italian Ministry of University and Scientific Research (MIUR,
Rome). MS is grateful to the National Science Foundation for
the partial support of this work (award CHE-0911109).
Notes and references
1 T. N. Nguyen, W. Wernsdorfer, K. A. Abboud and
G. Christou, J. Am. Chem. Soc., 2011, 133, 20688.
2 C.
Papatriantafyllopoulou,
T.
C.
Stamatatos,
C. G. Efthymiou, L. Cunha-Silva, F. A. Almeida Paz,
S. P. Perlepes and G. Christou, Inorg. Chem., 2010, 49, 9743.
3 A. N. Georgopoulou, C. P. Raptopoulou, V. Psycharis,
R. Ballesteros, B. Abarca and A. K. Boudalis, Inorg. Chem.,
2009, 48, 3167.
4 J. C. Anderson, A. J. Blake, R. B. Moreno, G. Raynel and
J. V. Slageren, Dalton Trans., 2009, 9153.
5 K. Xiong, F. Jiang, Y. Gai, Y. Zhou, D. Yuan, K. Su, X. Wang
and M. Hong, Inorg. Chem., 2012, 51, 3283.
6 M. L. Tong, M. Monfort, J. M. C. Juan, X. M. Chen,
X. H. Bu, M. Ohba and S. Kitagawa, Chem. Commun., 2005,
233.
7 A. Graham, S. Meier, S. Parsons and R. E. P. Winpenny,
Chem. Commun., 2000, 811.
8 A. N. Georgopoulou, C. P. Raptopoulou, V. Psycharis,
R. Balles-teros, B. Abarca and A. K. Boudalis, Inorg. Chem.,
2009, 48, 3167.
9 C. Boskovic, M. Pink, J. C. Huffman, D. N. Hendrickson
and G. Christou, J. Am. Chem. Soc., 2001, 123, 9914.
2–
CO3 bridge. Consequently, the temperature dependence of
χT was modeled with the three magnetic exchange constants
restrained to have the corresponding signs. The simulation of
the χT vs. T curve (Fig. 3) was performed with Magpack,26
resulting in the values of J1 = 3.0(2) cm−1, J2 = 0.4(1) cm−1, and
J3 = –7.5(3) cm−1, with g = 2.24(1). The magnitude of the
exchange constants is well comparable to the values reported
by Fondo et al. for the tetranuclear Ni(II) complex mentioned
above. The antiferromagnetic exchange (J3) acting along the
face diagonal of the cube appears to dominate the magnetic
behavior of the Ni8 cluster, resulting in the ST = 0 ground state.
This notion is additionally confirmed by field-dependent mag-
netization measurements performed at 1.8 K. The magnetiza-
tion value observed in low fields is rather low, but the
magnetization curve is non-linear, suggesting that some cross-
ing of magnetic states takes place at higher fields, as could be
1972 | Dalton Trans., 2014, 43, 1970–1973
This journal is © The Royal Society of Chemistry 2014