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Structural transition at 225 K of the trinuclear Fe(III) heptanoate [Fe3O(O2CC6H13)6(H2O)3]NO3

The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and...

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Published in:Solid state sciences 2005-10, Vol.7 (10), p.1236-1246
Main Authors: FRANCOIS, M, SALEH, M. I, RABU, P, SOUHASSOU, M, MALAMAN, B, STEINMETZ, J
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STEINMETZ, J
description The trinuclear iron (III) heptanoate [Fe30(O2CC6H13)6(H2O)3]NO3 compound is synthesized and studied by single crystal X-ray diffraction as a function of the temperature, also by Fe57 Mossbauer spectroscopy, electrochemical and magnetic measurements. Its thermal behavior is determined by DSC, TGA and X-ray diffraction. The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. A Heisenberg model of interaction based on triangular Fe(III) units of quantum S = 5/2 spins is used for simulating the variation of the susceptibility between room temperature and 2 K.
doi_str_mv 10.1016/j.solidstatesciences.2005.05.008
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The compound undergoes a structural phase transition at Ts = 225 K giving a superstructure of order two (above Ts: P -1, a = 11.1393(2) A, b = 14.2757(3) A, c = 18.2088(4) A, a = 80.607(1)DG, B = 84.175(l)DG, y = 83.464(1)DG; below Ts: P -1, a = 11.0122(2) A, b = 14.2723(3) A, c = 35.5222(7) A, a = 94.138(1)DG, 0 = 97.136(1)DG, y = 96.779(l)DG). The origin of the transition is interpreted as being due to a 60DG rotation of the nitrate groups of one sheet out of two of the lamellar structure. Analysis of the Fe57 Mossbauer spectra as a function of the temperature does not show electronic transition such as valence trapped phenoma below Ts. The compound has a paramagnetic behavior in the temperature range 300-2 K. 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subjects Condensed matter: electronic structure, electrical, magnetic, and optical properties
Condensed matter: structure, mechanical and thermal properties
Crystalline state (including molecular motions in solids)
Diamagnetism, paramagnetism and superparamagnetism
Exact sciences and technology
Magnetic properties and materials
Magnetic resonances and relaxations in condensed matter, mössbauer effect
Mössbauer effect
other γ-ray spectroscopy
Physics
Structure of solids and liquids
crystallography
Structure of specific crystalline solids
Theory of crystal structure, crystal symmetry
calculations and modeling
title Structural transition at 225 K of the trinuclear Fe(III) heptanoate [Fe3O(O2CC6H13)6(H2O)3]NO3
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