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Spin Crossover in a 3,5‐Bis(2‐pyridyl)‐1,2,4‐triazolate‐Bridged Dinuclear Iron(II) Complex [{Fe(NCBH3)(py)}2(μ‐L1)2] – Powder versus Single Crystal Study

Identifieur interne : 004957 ( Main/Exploration ); précédent : 004956; suivant : 004958

Spin Crossover in a 3,5‐Bis(2‐pyridyl)‐1,2,4‐triazolate‐Bridged Dinuclear Iron(II) Complex [{Fe(NCBH3)(py)}2(μ‐L1)2] – Powder versus Single Crystal Study

Auteurs : Caspar J. Schneider ; John D. Cashion [Australie] ; Nicholas F. Chilton ; Céline Etrillard [France] ; Mauricio Fuentealba [Royaume-Uni] ; Judith A. K. Howard [Royaume-Uni] ; Jean-François Létard [France] ; Carsten Milsmann [États-Unis] ; Boujemaa Moubaraki ; Hazel A. Sparkes [Royaume-Uni] ; Stuart R. Batten ; Keith S. Murray [États-Unis]

Source :

RBID : ISTEX:51A5236732D9FD366F5E79B45EC2C9673EE8A0EE

English descriptors

Abstract

The structural characteristics and physical properties of the 3,5‐bis(2‐pyridyl)‐1,2,4‐triazolate (L1) bridged dinuclear iron(II) spin‐crossover complex [{Fe(NCBH3)(py)}2(μ‐L1)2] (1) in both powder (1p) and single crystal (1c) forms have been investigated. Both forms of [{Fe(NCBH3)(py)}2(μ‐L1)2] display a thermally induced spin transition; however, the transitions have different T1/2 values and different degrees of spin conversion. Both forms display the photomagnetic light‐induced excited spin‐state trapping (LIESST) effect as well as reverse LIESST and have been compared by Raman spectral and powder X‐ray diffraction methods, which indicate that they are polymorphs. The single crystal form 1c shows a “half” spin transition and has been further characterised at temperatures above and below the spin transition by low temperature crystallographic methods including single crystal LIESST experiments (at 40 K) and by Mössbauer spectroscopy; thus, the nature of the [HS‐LS] form and the different spin isomers were revealed. To complement the experimental results, compound 1 and several other related FeII dinuclear spin‐crossover compounds have been evaluated by quantum‐chemical DFT calculations. Additionally, the susceptibilities for the powder form 1p, which displays a complete two‐step spin‐crossover, were also fitted to a phenomenological model for dinuclear spin‐crossover complexes.

Url:
DOI: 10.1002/ejic.201201075


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Le document en format XML

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<term>Apical ligands</term>
<term>Asymmetric unit</term>
<term>Australian synchrotron</term>
<term>B3lyp level</term>
<term>Behaviour</term>
<term>Bond lengths</term>
<term>Borshch</term>
<term>Bousseksou</term>
<term>Bulk powder</term>
<term>Centre</term>
<term>Chem</term>
<term>Coordination sphere</term>
<term>Crucial role</term>
<term>Crystal form</term>
<term>Crystal lattice</term>
<term>Crystal structure</term>
<term>Crystalline forms</term>
<term>Crystalline samples</term>
<term>Crystallographic data</term>
<term>Dalton trans</term>
<term>Density plots</term>
<term>Differential scanning calorimetry</term>
<term>Diffraction data</term>
<term>Dinuclear</term>
<term>Dinuclear complexes</term>
<term>Dinuclear molecule</term>
<term>Dinuclear molecules</term>
<term>Dinuclear systems</term>
<term>Doublet</term>
<term>Durham university</term>
<term>Energy difference</term>
<term>Experimental data</term>
<term>Experimental observation</term>
<term>Experimental parameters</term>
<term>Feii</term>
<term>Feii centre</term>
<term>Feii centres</term>
<term>Feii site</term>
<term>Feii sites</term>
<term>Full paper</term>
<term>Gmbh</term>
<term>Good agreement</term>
<term>Green laser</term>
<term>Ground sample</term>
<term>Inorg</term>
<term>Intermolecular interactions</term>
<term>Inversion centre</term>
<term>Isomer</term>
<term>Isomer shift</term>
<term>Isomer shifts</term>
<term>Kaizaki</term>
<term>Kgaa</term>
<term>Laser</term>
<term>Liesst</term>
<term>Liesst effect</term>
<term>Liesst state</term>
<term>Liesst studies</term>
<term>Ligand</term>
<term>Light irradiation</term>
<term>Light source</term>
<term>Lith effect</term>
<term>Magnetic properties</term>
<term>Magnetic susceptibility</term>
<term>Magnetic susceptibility data</term>
<term>Magnetic susceptibility studies</term>
<term>Metastable</term>
<term>Metastable state</term>
<term>Methanolic solution</term>
<term>Monash university</term>
<term>Moubaraki</term>
<term>Octahedral distortion parameter</term>
<term>Other dinuclear</term>
<term>Paper figure</term>
<term>Phenomenological model</term>
<term>Photoinduced metastable state</term>
<term>Phys</term>
<term>Plateau region</term>
<term>Powder diffraction</term>
<term>Powder form</term>
<term>Powder sample</term>
<term>Pxrd</term>
<term>Pxrd data</term>
<term>Pxrd measurements</term>
<term>Pxrd patterns</term>
<term>Pyridine</term>
<term>Quadrupole</term>
<term>Quadrupole splitting</term>
<term>Quantum chemical calculations</term>
<term>Raman</term>
<term>Raman spectra</term>
<term>Raman spectroscopic data</term>
<term>Relative energies</term>
<term>Room temperature</term>
<term>Second transition</term>
<term>Several weeks</term>
<term>Single crystal</term>
<term>Single crystals</term>
<term>Space group</term>
<term>Susceptibility</term>
<term>Thermal hysteresis</term>
<term>Thermogravimetric analysis</term>
<term>Triazolate ring</term>
<term>Unit cell volume</term>
<term>Verlag</term>
<term>Verlag gmbh</term>
<term>Version bruker</term>
<term>Weak bands</term>
<term>Weinheim</term>
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<term>Apical ligands</term>
<term>Asymmetric unit</term>
<term>Australian synchrotron</term>
<term>B3lyp level</term>
<term>Behaviour</term>
<term>Bond lengths</term>
<term>Borshch</term>
<term>Bousseksou</term>
<term>Bulk powder</term>
<term>Centre</term>
<term>Chem</term>
<term>Coordination sphere</term>
<term>Crucial role</term>
<term>Crystal form</term>
<term>Crystal lattice</term>
<term>Crystal structure</term>
<term>Crystalline forms</term>
<term>Crystalline samples</term>
<term>Crystallographic data</term>
<term>Dalton trans</term>
<term>Density plots</term>
<term>Differential scanning calorimetry</term>
<term>Diffraction data</term>
<term>Dinuclear</term>
<term>Dinuclear complexes</term>
<term>Dinuclear molecule</term>
<term>Dinuclear molecules</term>
<term>Dinuclear systems</term>
<term>Doublet</term>
<term>Durham university</term>
<term>Energy difference</term>
<term>Experimental data</term>
<term>Experimental observation</term>
<term>Experimental parameters</term>
<term>Feii</term>
<term>Feii centre</term>
<term>Feii centres</term>
<term>Feii site</term>
<term>Feii sites</term>
<term>Full paper</term>
<term>Gmbh</term>
<term>Good agreement</term>
<term>Green laser</term>
<term>Ground sample</term>
<term>Inorg</term>
<term>Intermolecular interactions</term>
<term>Inversion centre</term>
<term>Isomer</term>
<term>Isomer shift</term>
<term>Isomer shifts</term>
<term>Kaizaki</term>
<term>Kgaa</term>
<term>Laser</term>
<term>Liesst</term>
<term>Liesst effect</term>
<term>Liesst state</term>
<term>Liesst studies</term>
<term>Ligand</term>
<term>Light irradiation</term>
<term>Light source</term>
<term>Lith effect</term>
<term>Magnetic properties</term>
<term>Magnetic susceptibility</term>
<term>Magnetic susceptibility data</term>
<term>Magnetic susceptibility studies</term>
<term>Metastable</term>
<term>Metastable state</term>
<term>Methanolic solution</term>
<term>Monash university</term>
<term>Moubaraki</term>
<term>Octahedral distortion parameter</term>
<term>Other dinuclear</term>
<term>Paper figure</term>
<term>Phenomenological model</term>
<term>Photoinduced metastable state</term>
<term>Phys</term>
<term>Plateau region</term>
<term>Powder diffraction</term>
<term>Powder form</term>
<term>Powder sample</term>
<term>Pxrd</term>
<term>Pxrd data</term>
<term>Pxrd measurements</term>
<term>Pxrd patterns</term>
<term>Pyridine</term>
<term>Quadrupole</term>
<term>Quadrupole splitting</term>
<term>Quantum chemical calculations</term>
<term>Raman</term>
<term>Raman spectra</term>
<term>Raman spectroscopic data</term>
<term>Relative energies</term>
<term>Room temperature</term>
<term>Second transition</term>
<term>Several weeks</term>
<term>Single crystal</term>
<term>Single crystals</term>
<term>Space group</term>
<term>Susceptibility</term>
<term>Thermal hysteresis</term>
<term>Thermogravimetric analysis</term>
<term>Triazolate ring</term>
<term>Unit cell volume</term>
<term>Verlag</term>
<term>Verlag gmbh</term>
<term>Version bruker</term>
<term>Weak bands</term>
<term>Weinheim</term>
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<front>
<div type="abstract">The structural characteristics and physical properties of the 3,5‐bis(2‐pyridyl)‐1,2,4‐triazolate (L1) bridged dinuclear iron(II) spin‐crossover complex [{Fe(NCBH3)(py)}2(μ‐L1)2] (1) in both powder (1p) and single crystal (1c) forms have been investigated. Both forms of [{Fe(NCBH3)(py)}2(μ‐L1)2] display a thermally induced spin transition; however, the transitions have different T1/2 values and different degrees of spin conversion. Both forms display the photomagnetic light‐induced excited spin‐state trapping (LIESST) effect as well as reverse LIESST and have been compared by Raman spectral and powder X‐ray diffraction methods, which indicate that they are polymorphs. The single crystal form 1c shows a “half” spin transition and has been further characterised at temperatures above and below the spin transition by low temperature crystallographic methods including single crystal LIESST experiments (at 40 K) and by Mössbauer spectroscopy; thus, the nature of the [HS‐LS] form and the different spin isomers were revealed. To complement the experimental results, compound 1 and several other related FeII dinuclear spin‐crossover compounds have been evaluated by quantum‐chemical DFT calculations. Additionally, the susceptibilities for the powder form 1p, which displays a complete two‐step spin‐crossover, were also fitted to a phenomenological model for dinuclear spin‐crossover complexes.</div>
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<name sortKey="Murray, Keith S" sort="Murray, Keith S" uniqKey="Murray K" first="Keith S." last="Murray">Keith S. Murray</name>
<name sortKey="Murray, Keith S" sort="Murray, Keith S" uniqKey="Murray K" first="Keith S." last="Murray">Keith S. Murray</name>
</country>
</tree>
</affiliations>
</record>

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