Crystal structure and magnetic behavior of the decamethylferrocenium and decamethylchromocenium salts of bis(ethylenedithiolato)nickel, [M(Cp*)(2)][Ni(edt)(2)] - Magnetic anisotropy and metamagnetic behavior of [Fe(Cp*)(2)[Ni(edt)(2)]
V. Da Gama et al., Crystal structure and magnetic behavior of the decamethylferrocenium and decamethylchromocenium salts of bis(ethylenedithiolato)nickel, [M(Cp*)(2)][Ni(edt)(2)] - Magnetic anisotropy and metamagnetic behavior of [Fe(Cp*)(2)[Ni(edt)(2)], EUR J INORG, (9), 2000, pp. 2101-2110
New electron-transfer salts, [M(Cp*)(2)] [Ni(edt)(2)], with M = Fe and Cr,
were prepared and shown to be isostructural by Xray crystallographic studie
s. The molecular structure of [Ni(edt)(2)](-) is reported here for the firs
t time. The solid-state structure consists of an array of parallel alternat
ing donors, [Fe(Cp*)(2)](. c), and accepters, [Ni(edt)(2)](.-), ..DADADA..
stacks along [101]. At high temperatures (T > 50-100 K), the magnetic susce
ptibility obeys the Curie-Weiss expression, with the theta values of -5 and
-6.7 K for the Ni and Cr compounds respectively, revealing dominant AFM in
teractions. At low temperatures metamagnetic behavior was observed in case
of [Fe(Cp*)(2)][Ni(edt)(2)], with T-N = 4.2 K and H-C = 14 kG at 2 K, resul
ting from high magnetic anisotropy, due to the coexistence of strong FM DA
intrachain interactions and strong AFM (DA and AA) interchain interactions.
Single-crystal magnetization measurements with [Fe(Cp*)(2)][Ni(edt)(2)] sh
owed that the transition from the AFM state to the FM high-field state was
induced by the application of a magnetic field parallel to the stacking axi
s. In these compounds the AFM interchain (DA and AA) interactions play a do
minant role, due to the large spin density on the periphery of the acceptor
and the close AA and DA interchain contacts. Above 4.2 K the Fe-57 Mossbau
er spectra of [Fe(Cp*)(2)] [Ni(edt)(2)] exhibit the classical low spin Fe-I
II ferrocenium singlet. Below this temperature a poorly resolved hyperfine
pattern is observed (estimated hyperfine field ca. 350 kG at 3.5 K). The an
alysis of the spectra obtained in applied fields of 20 kG and 50 kG is cons
istent with a strongly anisotropic g tensor. A pronounced temperature depen
dence of the spectra in a field of 50 kG suggests the presence of spin-latt
ice relaxation effects.