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Fig. 2.20 LIESST effect at A sites of [Fe(mtz) 6 ](BF 4 ) 2 (LS to metastable HS conversion with green
light, 514 nm) and at B sites (HS to metastable LS conversion with red light, 820 nm). Thermal
relaxation from HS to LS at A sites and from LS to HS at B sites sets in at ca. 65 K in both cases [ 31 ]
Fig. 2.21 a View of the crystal structure of [Fe(bpym)(NCS) 2 ] 2 bpym [ 32 ]. b Plot of | M T vs. T for
[Fe(bpym)(NCSe) 2 ] 2 bpym, where | M is the magnetic susceptibility corrected for diamagnetic
contributions [ 33 ]
v M T value of ca. 3.5 cm 3 mol -1 K which indicates that about 50 % of the Fe II ions
have undergone ST to the LS state (Fig. 2.21 b) [ 33 ]. The question, however, arises
concerning the nature of the plateau region: Does the plateau originate from only
[HS-LS] pairs or from a 1:1 mixture of [HS-HS] and [LS-LS] pairs?
Neither can this question be answered by magnetic susceptibility measurements
nor by conventional Mössbauer spectroscopy. The latter would yield identical
spectra for the HS state of Fe II atoms in [HS-LS] and [HS-HS] spin pairs as seen
in Fig. 2.22 a. However, the Mössbauer spectrum recorded in applied magnetic
field can give a conclusive answer based on the different effective hyperfine
magnetic fields arising from different expectation values of the spin state of the
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