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Fig. 2.25 a Projection showing the crystal structure of [Fe 3 (iptrz) 6 (H 2 O) 6 ](CF 3 SO 3 ) 6 [ 42 ].
b Temperature dependent 57 Fe Mössbauer spectra of [Fe 3 (iptrz) 6 (H 2 O) 6 ](CF 3 SO 3 ) 6 [ 42 ]. The
yellow, red and green doublets correspond to HS 0 ,HS c and HS SC , respectively. The blue signal
corresponds to LS c
intensity of the blue LSc resonance signal. This 2:1 intensity ratio for HS S o : LSc
(green to blue) remains on further lowering the temperature. The same 2:1
intensity ratio remains for HSo: HSc (yellow to red) at any temperature until they
entirely disappear after the ST is complete. The Mössbauer spectrum recorded at
120 K shows only the resonance signals for HS-LS-HS species. Clearly, the outer
Fe II -HS sites ''feel'' the process of thermal ST at the center, which is being
communicated through the three rigid 1,2,4-triazole bridges and cause a noticeable
structural distortion at the outer Fe II -HS sites without influencing the spin state.
This is another ''textbook example'' for the high sensitivity of Mössbauer
spectroscopy similar to the Mössbauer study of the
BF ð Þ 4 •DMF
discussed above. The tiny small distortion felt by the outer Fe II -HS sites, which is
caused by the ST from HS to LS in the center, is hardly detectable by diffraction
techniques. Similarly, HS $ LS relaxation effects that are not seen by magnetic
susceptibility measurements were detected at room temperature for the trinuclear
Fe I 2
ð
pmatrz
Þ 2
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