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Fig. 2.38 Schematized molecular structure of a trinuclear cationic complex which accommo-
dates LS-Fe III (red) and LS-Fe II (blue) ions separated by bridging LS-Co III ion. At low
temperatures two well resolved spectra are observed assigned to the localized LS-Fe III and the
LS-Fe II species. With increasing temperature the intensities of these two doublets decrease at the
favor of a new doublet (green) from a time-averaged species with intermediate oxidation state of
the two iron sites. This species is the only one remaining at room temperature [ 69 ]
intensities of these two resonance signals decrease at the favor of a new resonance
signal, another quadrupole doublet (blue), arising from a time-averaged species
where both iron centers are in an intermediate oxidation state as a result of fast
electron fluctuation through the bridging diamagnetic central Co III ion (Fig. 2.38 ).
2.3.3.4 Valence Fluctuation in EuNiP
Mixed-valency and thermally induced transition between localized and delocalized
valence states was observed with 151 Eu Mössbauer spectroscopy of the interme-
tallic compound EuNiP [ 70 ] (Fig. 2.39 ).
High temperature 151 Eu Mössbauer measurements between room temperature
and ca. 500 K provide proof for mixed-valent behavior in the pnictide EuNiP. Two
well resolved signals are observed at room temperature, one being typical for Eu 2+
(dark grey) and the other one for Eu III (light grey). With increasing temperature the
electron fluctuation between Eu II and Eu III becomes faster than the time-window
of 151 Eu Mössbauer spectroscopy and above ca. 450 K the resonance signals of
localized Eu II (dark grey) and Eu III (light grey) gradually disappear at the favor of
a new signal with time-averaged oxidation state of Eu 2.5+
(non shaded) [ 70 ].
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