1974
DOI: 10.1016/s0022-3697(74)80010-7
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Phonon coupled cooperative low-spin 1A1high-spin 5T2 transition in [Fe(phen)2(NCS)2] and [Fe(phen)2(NCSe)2] crystals

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Cited by 486 publications
(387 citation statements)
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“…The energy loss arising at the boundary surface between the two phases may be quite small and the energy gain due to mixing entropy would compensate for it, giving rise to the coexistence of the two phases. This phenomenon might correspond to the model proposed by Frenkel (1947) and Sorai & Seki (1974). The twinning observed in the low-temperature modification is suggestive of a small energy loss.…”
Section: Structural Change With the Transitionsupporting
confidence: 87%
“…The energy loss arising at the boundary surface between the two phases may be quite small and the energy gain due to mixing entropy would compensate for it, giving rise to the coexistence of the two phases. This phenomenon might correspond to the model proposed by Frenkel (1947) and Sorai & Seki (1974). The twinning observed in the low-temperature modification is suggestive of a small energy loss.…”
Section: Structural Change With the Transitionsupporting
confidence: 87%
“…The overall variations DH = 8.4 kJ mol À1 and DS = 53 J K À1 mol À1 are within the experimental range generally observed for iron(ii) SCO compounds. [30] It is worth noting that a symmetric distribution of DS between the two steps should be expected. However, DS 1 is significantly smaller than DS 2 .…”
Section: Differential Scanning Calorimetry (Dsc) Measurementsmentioning
confidence: 99%
“…This results in a drastic change in the density of vibrational states, mainly in the metal-ligand skeletal vibrational modes. This leads, of course, to significantly higher vibrational entropy in the HS state [31]. The entropy change accompanying the SC can be represented as the sum of electronic, configurational and motional, i.e.…”
Section: Hs Lsmentioning
confidence: 99%