Solid state electrochemistry, X-ray powder diffraction, magnetic susceptibility, electron spin resonance, Mossbauer and diffuse reflectance spectroscopy of mixed iron(III)-cadmium(II) hexacyanoferrates
Nf. Zakharchuk et al., Solid state electrochemistry, X-ray powder diffraction, magnetic susceptibility, electron spin resonance, Mossbauer and diffuse reflectance spectroscopy of mixed iron(III)-cadmium(II) hexacyanoferrates, J SOL ST EL, 3(5), 1999, pp. 264-276
Coprecipitates of Cd-II, K-I and Fe-III with hexacyanoferrate ions [Fe(CN)(
6)](4-) have been studied by solid-state electrochemistry (voltammetry of i
mmobilized microparticles), magnetic susceptibility measurements, X-ray pow
der diffraction, electron spin resonance, Mossbauer and diffuse reflectance
spectroscopy. Most suprisingly? all experimental results point to the form
ation of a continuous series of complex mixed phases without the formation
of phase mixtures. Although Cd-II and Fe-III ions differ too much in their
ionic radii to allow the formation of simple substitution mixed hexacyanofe
rrates, they are capable of forming different kinds of complex insertion an
d substitution mixed crystals because of the zeolitic structure of both the
iron and the cadmium hexacyanoferrate. Low cadmium concentrations can be f
ound in the zeolitic cavities of iron hexacyanoferrate (Prussian blue), and
they start to widen the lattice and facilitate, at higher concentrations,
the direct substitution of high-spin iron(III) ions by cadmium ions. In cas
es of an excess of cadmium, the formation of cadmium hexacyanoferrate with
iron(III) ions in the interstitials of the zeolitic structure is observed.
These mixed phases show strong charge transfer bands in the visible range a
nd have the appearance of "diluted" Prussian blue. For the first time, this
indicates that the charge transfer between the carbon-coordinated low-spin
iron(II) ions and the high-spin iron(III) ions can also occur when the lat
ter are situated in the cavities of a host hexacyanoferrate. In Prussian bl
ue the interstitial iron(III) ions are responsible for a very strong charge
transfer interaction between the low-spin iron(II) ions and the nitrogen-c
oordinated high-spin iron(III) ions. Upon substitution of the very small am
ount of interstitial iron(III) ions in Prussian blue by potassium and cadmi
um ions the Kubellca-Munk function diminishes by more than 30%, indicating
a tremendous decrease in iron(III)-iron(II) interaction.