The hydrate of a neutral iron(iii) complex based on the pyruvic acid thiosemicarbazone ligand with abrupt spin-crossover with T1/2 = 340 K and a wide hysteresis loop of 45 K

The hydrate of a neutral iron(iii) complex based on the pyruvic acid thiosemicarbazone ligand [FeIII(Hthpy)(thpy)]·H2O (1) was synthesized and characterized using FT-IR spectroscopy, powder and single-crystal X-ray diffraction, dc magnetic measurements, EPR and 57Fe Mössbauer spectroscopy. The cryst...

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Veröffentlicht in:Dalton transactions : an international journal of inorganic chemistry 2024-12, Vol.54 (1), p.346-356
Hauptverfasser: Blagov, Maxim A, Akimov, Alexander V, Lobach, Anatoly S, Zorina, Leokadiya V, Simonov, Sergey V, Zakharov, Konstantin V, Vasiliev, Alexander N, Spitsyna, Nataliya G
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container_title Dalton transactions : an international journal of inorganic chemistry
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creator Blagov, Maxim A
Akimov, Alexander V
Lobach, Anatoly S
Zorina, Leokadiya V
Simonov, Sergey V
Zakharov, Konstantin V
Vasiliev, Alexander N
Spitsyna, Nataliya G
description The hydrate of a neutral iron(iii) complex based on the pyruvic acid thiosemicarbazone ligand [FeIII(Hthpy)(thpy)]·H2O (1) was synthesized and characterized using FT-IR spectroscopy, powder and single-crystal X-ray diffraction, dc magnetic measurements, EPR and 57Fe Mössbauer spectroscopy. The crystal structure of 1 was determined for the first time. Two distinct chelating ligands Hthpy− and thpy2− coordinate the Fe(iii) ion to form the FeN2O2S2 octahedron which shows a low spin geometry at 150–350 K. The crystal packing contains infinite chains of the Fe(iii) complexes as well as water molecules located in cavities. Along the chain, π–π interacting pairs of the Fe complexes are linked by H-bonding. According to the dc magnetic measurements, the complete abrupt spin-crossover with half-transition temperature T1/2 = 340 K and a hysteresis loop of 45 K occurs in the temperature range of 300–363 K. Based on the X-ray structure of 1, the Bleaney–Bowers equation for the isolated dimer model was used to approximate the temperature dependence of the magnetic susceptibility in the range of 2–50 K. The defined intradimer exchange constant Jexp = −0.498(1) K corresponds to a weak antiferromagnetic exchange between the iron(iii) magnetic centers. DFT calculations of H- and π–π bonded fragments of the crystal structure of 1 in the HS and LS states were carried out. Moreover, BS-DFT calculations confirm the presence of antiferromagnetic exchange Jcalc = −0.92 K in the π–π bonded pairs of the ferric complexes and show the exchange pathway between Fe(iii) ions by the calculated spin density distribution.
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The crystal structure of 1 was determined for the first time. Two distinct chelating ligands Hthpy− and thpy2− coordinate the Fe(iii) ion to form the FeN2O2S2 octahedron which shows a low spin geometry at 150–350 K. The crystal packing contains infinite chains of the Fe(iii) complexes as well as water molecules located in cavities. Along the chain, π–π interacting pairs of the Fe complexes are linked by H-bonding. According to the dc magnetic measurements, the complete abrupt spin-crossover with half-transition temperature T1/2 = 340 K and a hysteresis loop of 45 K occurs in the temperature range of 300–363 K. Based on the X-ray structure of 1, the Bleaney–Bowers equation for the isolated dimer model was used to approximate the temperature dependence of the magnetic susceptibility in the range of 2–50 K. The defined intradimer exchange constant Jexp = −0.498(1) K corresponds to a weak antiferromagnetic exchange between the iron(iii) magnetic centers. DFT calculations of H- and π–π bonded fragments of the crystal structure of 1 in the HS and LS states were carried out. 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The crystal structure of 1 was determined for the first time. Two distinct chelating ligands Hthpy− and thpy2− coordinate the Fe(iii) ion to form the FeN2O2S2 octahedron which shows a low spin geometry at 150–350 K. The crystal packing contains infinite chains of the Fe(iii) complexes as well as water molecules located in cavities. Along the chain, π–π interacting pairs of the Fe complexes are linked by H-bonding. According to the dc magnetic measurements, the complete abrupt spin-crossover with half-transition temperature T1/2 = 340 K and a hysteresis loop of 45 K occurs in the temperature range of 300–363 K. Based on the X-ray structure of 1, the Bleaney–Bowers equation for the isolated dimer model was used to approximate the temperature dependence of the magnetic susceptibility in the range of 2–50 K. The defined intradimer exchange constant Jexp = −0.498(1) K corresponds to a weak antiferromagnetic exchange between the iron(iii) magnetic centers. 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DFT calculations of H- and π–π bonded fragments of the crystal structure of 1 in the HS and LS states were carried out. Moreover, BS-DFT calculations confirm the presence of antiferromagnetic exchange Jcalc = −0.92 K in the π–π bonded pairs of the ferric complexes and show the exchange pathway between Fe(iii) ions by the calculated spin density distribution.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d4dt02901a</doi><tpages>11</tpages></addata></record>
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source Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection
subjects Antiferromagnetism
Chelation
Crossovers
Crystal structure
Density distribution
Differential geometry
Hysteresis loops
Infrared spectroscopy
Iron
Ligands
Magnetic measurement
Magnetic permeability
Molecular structure
Mossbauer spectroscopy
Single crystals
Spectrum analysis
Temperature dependence
Transition temperature
title The hydrate of a neutral iron(iii) complex based on the pyruvic acid thiosemicarbazone ligand with abrupt spin-crossover with T1/2 = 340 K and a wide hysteresis loop of 45 K
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