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Fig. 2.37 Molecular structure and temperature dependent 57 Fe Mössbauer spectra of the mixed
valence complex compound [Fe 3 O(O 2 CCH 3 ) 3 ) 6 (3-Et-py) 3 ] S with S = 0.5 benzene (a), CH 3 CN
(b) and CH 3 CCl 3 (c). Solvates A and B are ''valence-trapped'' (localized) with two HS-Fe III ions
(red doublet) and one HS-Fe II ion (green doublet) in the molecular unit; the quadrupole doublets
are well resolved without significant line-broadening. c Shows a transition from electron
localization to delocalization (valence-trapped to detrapped) with increasing temperature. The
sharp doublets of the trapped species begin to broaden on heating and finally disappear at the favor
of a time-averaged new signal (blue) from a species with averaged oxidation state, ''Fe 2.67+ '', due to
fast electron fluctuation within the Fe 3 O triangle [ 68 ]
The resonance lines of the two quadrupole doublets begin to broaden around 50 K.
Further increase of temperature leads to valence-detrapping (delocalization) near
room temperature, where the red and green doublets have disappeared at the favor
of a new doublet (blue) which is a time-averaged resonance signal of a species
with an ''average'' oxidation state of ''Fe 2.67+ '' due to rapid electron circulation
within the Fe 3 O triangle of the complex.
2.3.3.3 Valence Fluctuation in a Trinuclear Cationic Complex
Another interesting example of valence fluctuation and temperature dependent
transition between localized and delocalized electronic structures in a trinuclear
transition metal compound was reported by Glaser et al. [ 69 ]. In this case the
electron fluctuation takes place between two iron centers of different oxidation states
and separated by a diamagnetic Co III ion. The 57 Fe Mössbauer spectra clearly show
that at sufficiently low temperatures, i.e. 5 K, the two iron centers are reflected as
localized oxidation states with a well resolved doublet for LS-Fe III
(red) and a
poorly resolved doublet for LS-Fe II
(light-blue). At higher temperatures the
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