Spin crossover in iron(II) tris(2-(2′-pyridyl)benzimidazole) complex monitored by variable temperature methods: Synchrotron powder diffraction, DSC, IR spectra, mössbauer spectra, and magnetic susceptibility

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Authors

  • R. Boča
  • M. Boča
  • H. Ehrenberg
  • H. Fuess
  • W. Linert
  • F. Renz
  • I. Svoboda

External Research Organisations

  • Slovak University of Technology in Bratislava
  • Technische Universität Darmstadt
  • TU Wien (TUW)
  • Johannes Gutenberg University Mainz
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Details

Original languageEnglish
Pages (from-to)375-395
Number of pages21
JournalChemical physics
Volume293
Issue number3
Publication statusPublished - 15 Sept 2003
Externally publishedYes

Abstract

The thermal expansion of the spin crossover system [Fe(pybzim) 3](ClO4)2 · H2O (pybzim = 2-(2′-pyridyl)benzimidazole) has been determined from powder X-ray data between 50 and 250 K; the wavelength of the synchrotron source was 1.21888(1) Å. The unit cell parameters of the triclinic crystal system were a = 12.091 Å, b = 12.225 Å, c = 14.083 Å, α = 77.70°, β = 80.35°, Yγ = 74.35°, and V = 1944.9 Å3 at 250 K. In addition to the linear thermal expansion of the unit cell volume, an extra expansion due to the low-spin (LS) to high-spin (HS) transition is observed. The V(T) function shows a sudden increase comparable with the step in the effective magnetic moment at the transition region (140 K). A similar behavior is obtained on the basis of the infrared spectra. The absorption bands corresponding to the metal-ligand stretching modes change their intensities upon heating: the bands corresponding to the low-spin molecules (at ca. 409, 430, 443, and 460 cm-1) disappear in the gain of the high-spin bands (at 259 and 285 cm-1). The variable-temperature data obtained by different techniques (powder diffraction, EXAFS, IR spectra, Mössbauer spectra, magnetic susceptibility, DSC) have been transformed to a common basis - the temperature dependence of the high-spin mole fraction xHS(T). The application of the Ising-like (two-level) model of the spin crossover led to the thermodynamic data ΔH = 2.6 kJ mol-1 and ΔS = 19 J K-1 mol-1 as well as to the cooperativeness J/kæ 110 K (subtracted from the susceptibility data) that characterizes the abruptness of the spin crossover in the solid state.

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Spin crossover in iron(II) tris(2-(2′-pyridyl)benzimidazole) complex monitored by variable temperature methods: Synchrotron powder diffraction, DSC, IR spectra, mössbauer spectra, and magnetic susceptibility. / Boča, R.; Boča, M.; Ehrenberg, H. et al.
In: Chemical physics, Vol. 293, No. 3, 15.09.2003, p. 375-395.

Research output: Contribution to journalArticleResearchpeer review

Download
@article{b28cb84d84354b70912a68fe23256013,
title = "Spin crossover in iron(II) tris(2-(2′-pyridyl)benzimidazole) complex monitored by variable temperature methods: Synchrotron powder diffraction, DSC, IR spectra, m{\"o}ssbauer spectra, and magnetic susceptibility",
abstract = "The thermal expansion of the spin crossover system [Fe(pybzim) 3](ClO4)2 · H2O (pybzim = 2-(2′-pyridyl)benzimidazole) has been determined from powder X-ray data between 50 and 250 K; the wavelength of the synchrotron source was 1.21888(1) {\AA}. The unit cell parameters of the triclinic crystal system were a = 12.091 {\AA}, b = 12.225 {\AA}, c = 14.083 {\AA}, α = 77.70°, β = 80.35°, Yγ = 74.35°, and V = 1944.9 {\AA}3 at 250 K. In addition to the linear thermal expansion of the unit cell volume, an extra expansion due to the low-spin (LS) to high-spin (HS) transition is observed. The V(T) function shows a sudden increase comparable with the step in the effective magnetic moment at the transition region (140 K). A similar behavior is obtained on the basis of the infrared spectra. The absorption bands corresponding to the metal-ligand stretching modes change their intensities upon heating: the bands corresponding to the low-spin molecules (at ca. 409, 430, 443, and 460 cm-1) disappear in the gain of the high-spin bands (at 259 and 285 cm-1). The variable-temperature data obtained by different techniques (powder diffraction, EXAFS, IR spectra, M{\"o}ssbauer spectra, magnetic susceptibility, DSC) have been transformed to a common basis - the temperature dependence of the high-spin mole fraction xHS(T). The application of the Ising-like (two-level) model of the spin crossover led to the thermodynamic data ΔH = 2.6 kJ mol-1 and ΔS = 19 J K-1 mol-1 as well as to the cooperativeness J/k{\ae} 110 K (subtracted from the susceptibility data) that characterizes the abruptness of the spin crossover in the solid state.",
author = "R. Bo{\v c}a and M. Bo{\v c}a and H. Ehrenberg and H. Fuess and W. Linert and F. Renz and I. Svoboda",
note = "Funding Information: Thanks are to the grant agencies (VEGA: 1/9252/02, APVT: 20-009902, Slovakia; DAAD and DFG, Germany) for financial support. The authors are thankful to Dr. R{\"u}diger Werner (TU Darmstadt, Germany), Dr. Martina Vrbov{\'a} and Ing. Rastislav Jaro{\v s}{\v c}iak (STU Bratislava, Slovakia) for help in taking and analyzing some experimental data.",
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doi = "10.1016/S0301-0104(03)00375-6",
language = "English",
volume = "293",
pages = "375--395",
journal = "Chemical physics",
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Download

TY - JOUR

T1 - Spin crossover in iron(II) tris(2-(2′-pyridyl)benzimidazole) complex monitored by variable temperature methods

T2 - Synchrotron powder diffraction, DSC, IR spectra, mössbauer spectra, and magnetic susceptibility

AU - Boča, R.

AU - Boča, M.

AU - Ehrenberg, H.

AU - Fuess, H.

AU - Linert, W.

AU - Renz, F.

AU - Svoboda, I.

N1 - Funding Information: Thanks are to the grant agencies (VEGA: 1/9252/02, APVT: 20-009902, Slovakia; DAAD and DFG, Germany) for financial support. The authors are thankful to Dr. Rüdiger Werner (TU Darmstadt, Germany), Dr. Martina Vrbová and Ing. Rastislav Jaroščiak (STU Bratislava, Slovakia) for help in taking and analyzing some experimental data.

PY - 2003/9/15

Y1 - 2003/9/15

N2 - The thermal expansion of the spin crossover system [Fe(pybzim) 3](ClO4)2 · H2O (pybzim = 2-(2′-pyridyl)benzimidazole) has been determined from powder X-ray data between 50 and 250 K; the wavelength of the synchrotron source was 1.21888(1) Å. The unit cell parameters of the triclinic crystal system were a = 12.091 Å, b = 12.225 Å, c = 14.083 Å, α = 77.70°, β = 80.35°, Yγ = 74.35°, and V = 1944.9 Å3 at 250 K. In addition to the linear thermal expansion of the unit cell volume, an extra expansion due to the low-spin (LS) to high-spin (HS) transition is observed. The V(T) function shows a sudden increase comparable with the step in the effective magnetic moment at the transition region (140 K). A similar behavior is obtained on the basis of the infrared spectra. The absorption bands corresponding to the metal-ligand stretching modes change their intensities upon heating: the bands corresponding to the low-spin molecules (at ca. 409, 430, 443, and 460 cm-1) disappear in the gain of the high-spin bands (at 259 and 285 cm-1). The variable-temperature data obtained by different techniques (powder diffraction, EXAFS, IR spectra, Mössbauer spectra, magnetic susceptibility, DSC) have been transformed to a common basis - the temperature dependence of the high-spin mole fraction xHS(T). The application of the Ising-like (two-level) model of the spin crossover led to the thermodynamic data ΔH = 2.6 kJ mol-1 and ΔS = 19 J K-1 mol-1 as well as to the cooperativeness J/kæ 110 K (subtracted from the susceptibility data) that characterizes the abruptness of the spin crossover in the solid state.

AB - The thermal expansion of the spin crossover system [Fe(pybzim) 3](ClO4)2 · H2O (pybzim = 2-(2′-pyridyl)benzimidazole) has been determined from powder X-ray data between 50 and 250 K; the wavelength of the synchrotron source was 1.21888(1) Å. The unit cell parameters of the triclinic crystal system were a = 12.091 Å, b = 12.225 Å, c = 14.083 Å, α = 77.70°, β = 80.35°, Yγ = 74.35°, and V = 1944.9 Å3 at 250 K. In addition to the linear thermal expansion of the unit cell volume, an extra expansion due to the low-spin (LS) to high-spin (HS) transition is observed. The V(T) function shows a sudden increase comparable with the step in the effective magnetic moment at the transition region (140 K). A similar behavior is obtained on the basis of the infrared spectra. The absorption bands corresponding to the metal-ligand stretching modes change their intensities upon heating: the bands corresponding to the low-spin molecules (at ca. 409, 430, 443, and 460 cm-1) disappear in the gain of the high-spin bands (at 259 and 285 cm-1). The variable-temperature data obtained by different techniques (powder diffraction, EXAFS, IR spectra, Mössbauer spectra, magnetic susceptibility, DSC) have been transformed to a common basis - the temperature dependence of the high-spin mole fraction xHS(T). The application of the Ising-like (two-level) model of the spin crossover led to the thermodynamic data ΔH = 2.6 kJ mol-1 and ΔS = 19 J K-1 mol-1 as well as to the cooperativeness J/kæ 110 K (subtracted from the susceptibility data) that characterizes the abruptness of the spin crossover in the solid state.

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U2 - 10.1016/S0301-0104(03)00375-6

DO - 10.1016/S0301-0104(03)00375-6

M3 - Article

AN - SCOPUS:0042830493

VL - 293

SP - 375

EP - 395

JO - Chemical physics

JF - Chemical physics

SN - 0301-0104

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