From Positive to Negative Zero-Field Splitting in a Series of Strongly Magnetically Anisotropic Mononuclear Metal Complexes

A series of mononuclear [M(hfa) (pic) ] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = Fe , Co , Ni , Zn ) compounds were obtained and characterized. The structures of the complexes have been resolved by single-crystal X-ray diffraction, indicating that, apart from the...

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Veröffentlicht in:Inorganic chemistry Jg. 56; H. 24; S. 14809
Hauptverfasser: Novitchi, Ghénadie, Jiang, Shangda, Shova, Sergiu, Rida, Fatima, Hlavička, Ivo, Orlita, Milan, Wernsdorfer, Wolfgang, Hamze, Rana, Martins, Cyril, Suaud, Nicolas, Guihéry, Nathalie, Barra, Anne-Laure, Train, Cyrille
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Sprache:Englisch
Veröffentlicht: United States 18.12.2017
ISSN:1520-510X, 1520-510X
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Abstract A series of mononuclear [M(hfa) (pic) ] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = Fe , Co , Ni , Zn ) compounds were obtained and characterized. The structures of the complexes have been resolved by single-crystal X-ray diffraction, indicating that, apart from the zinc derivative, the complexes are in a trans configuration. Moreover, a dramatic lenghthening of the Fe-N distances was observed, whereas the nickel(II) complex is almost perfectly octahedral. The magnetic anisotropy of these complexes was thoroughly studied by direct-current (dc) magnetic measurements, high-field electron paramagnetic resonance, and infrared (IR) magnetospectroscopy: the iron(II) derivative exhibits an out-of-plane anisotropy (D = -7.28 cm ) with a high rhombicity, whereas the cobalt(II) and nickel(II) complexes show in-plane anisotropy (D ∼ 92-95 cm ; D = 4.920 cm ). Ab initio calculations were performed to rationalize the evolution of the structure and identify the excited states governing the magnetic anisotropy along the series. For the iron(II) complex, an out-of-phase alternating-current (ac) magnetic susceptibility signal was observed using a 0.1 T dc field. For the cobalt(II) derivative, the ac magnetic susceptibility shows the presence of two field-dependent relaxation phenomena: at low field (500 Oe), the relaxation process is beyond single-ion behavior, whereas at high field (2000 Oe), the relaxation of magnetization implies several mechanisms including an Orbach process with U = 25 K and quantum tunneling of magnetization. The observation by μ-SQUID magnetization measurements of hysteresis loops of up to 1 K confirmed the single-ion-magnet behavior of the cobalt(II) derivative.
AbstractList A series of mononuclear [M(hfa) (pic) ] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = Fe , Co , Ni , Zn ) compounds were obtained and characterized. The structures of the complexes have been resolved by single-crystal X-ray diffraction, indicating that, apart from the zinc derivative, the complexes are in a trans configuration. Moreover, a dramatic lenghthening of the Fe-N distances was observed, whereas the nickel(II) complex is almost perfectly octahedral. The magnetic anisotropy of these complexes was thoroughly studied by direct-current (dc) magnetic measurements, high-field electron paramagnetic resonance, and infrared (IR) magnetospectroscopy: the iron(II) derivative exhibits an out-of-plane anisotropy (D = -7.28 cm ) with a high rhombicity, whereas the cobalt(II) and nickel(II) complexes show in-plane anisotropy (D ∼ 92-95 cm ; D = 4.920 cm ). Ab initio calculations were performed to rationalize the evolution of the structure and identify the excited states governing the magnetic anisotropy along the series. For the iron(II) complex, an out-of-phase alternating-current (ac) magnetic susceptibility signal was observed using a 0.1 T dc field. For the cobalt(II) derivative, the ac magnetic susceptibility shows the presence of two field-dependent relaxation phenomena: at low field (500 Oe), the relaxation process is beyond single-ion behavior, whereas at high field (2000 Oe), the relaxation of magnetization implies several mechanisms including an Orbach process with U = 25 K and quantum tunneling of magnetization. The observation by μ-SQUID magnetization measurements of hysteresis loops of up to 1 K confirmed the single-ion-magnet behavior of the cobalt(II) derivative.
A series of mononuclear [M(hfa)2(pic)2] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = FeII, CoII, NiII, ZnII) compounds were obtained and characterized. The structures of the complexes have been resolved by single-crystal X-ray diffraction, indicating that, apart from the zinc derivative, the complexes are in a trans configuration. Moreover, a dramatic lenghthening of the Fe-N distances was observed, whereas the nickel(II) complex is almost perfectly octahedral. The magnetic anisotropy of these complexes was thoroughly studied by direct-current (dc) magnetic measurements, high-field electron paramagnetic resonance, and infrared (IR) magnetospectroscopy: the iron(II) derivative exhibits an out-of-plane anisotropy (DFe = -7.28 cm-1) with a high rhombicity, whereas the cobalt(II) and nickel(II) complexes show in-plane anisotropy (DCo ∼ 92-95 cm-1; DNi = 4.920 cm-1). Ab initio calculations were performed to rationalize the evolution of the structure and identify the excited states governing the magnetic anisotropy along the series. For the iron(II) complex, an out-of-phase alternating-current (ac) magnetic susceptibility signal was observed using a 0.1 T dc field. For the cobalt(II) derivative, the ac magnetic susceptibility shows the presence of two field-dependent relaxation phenomena: at low field (500 Oe), the relaxation process is beyond single-ion behavior, whereas at high field (2000 Oe), the relaxation of magnetization implies several mechanisms including an Orbach process with Ueff = 25 K and quantum tunneling of magnetization. The observation by μ-SQUID magnetization measurements of hysteresis loops of up to 1 K confirmed the single-ion-magnet behavior of the cobalt(II) derivative.A series of mononuclear [M(hfa)2(pic)2] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = FeII, CoII, NiII, ZnII) compounds were obtained and characterized. The structures of the complexes have been resolved by single-crystal X-ray diffraction, indicating that, apart from the zinc derivative, the complexes are in a trans configuration. Moreover, a dramatic lenghthening of the Fe-N distances was observed, whereas the nickel(II) complex is almost perfectly octahedral. The magnetic anisotropy of these complexes was thoroughly studied by direct-current (dc) magnetic measurements, high-field electron paramagnetic resonance, and infrared (IR) magnetospectroscopy: the iron(II) derivative exhibits an out-of-plane anisotropy (DFe = -7.28 cm-1) with a high rhombicity, whereas the cobalt(II) and nickel(II) complexes show in-plane anisotropy (DCo ∼ 92-95 cm-1; DNi = 4.920 cm-1). Ab initio calculations were performed to rationalize the evolution of the structure and identify the excited states governing the magnetic anisotropy along the series. For the iron(II) complex, an out-of-phase alternating-current (ac) magnetic susceptibility signal was observed using a 0.1 T dc field. For the cobalt(II) derivative, the ac magnetic susceptibility shows the presence of two field-dependent relaxation phenomena: at low field (500 Oe), the relaxation process is beyond single-ion behavior, whereas at high field (2000 Oe), the relaxation of magnetization implies several mechanisms including an Orbach process with Ueff = 25 K and quantum tunneling of magnetization. The observation by μ-SQUID magnetization measurements of hysteresis loops of up to 1 K confirmed the single-ion-magnet behavior of the cobalt(II) derivative.
Author Rida, Fatima
Suaud, Nicolas
Orlita, Milan
Novitchi, Ghénadie
Hlavička, Ivo
Martins, Cyril
Shova, Sergiu
Guihéry, Nathalie
Jiang, Shangda
Wernsdorfer, Wolfgang
Hamze, Rana
Barra, Anne-Laure
Train, Cyrille
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  surname: Novitchi
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  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
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  givenname: Shangda
  orcidid: 0000-0003-0204-9601
  surname: Jiang
  fullname: Jiang, Shangda
  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
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  givenname: Sergiu
  surname: Shova
  fullname: Shova, Sergiu
  organization: "Petru Poni" Institute of Macromolecular Chemistry , Aleea Gr. Ghica Voda 41A, 700487 Iasi, Romania
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  givenname: Ivo
  surname: Hlavička
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  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
– sequence: 6
  givenname: Milan
  surname: Orlita
  fullname: Orlita, Milan
  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
– sequence: 7
  givenname: Wolfgang
  surname: Wernsdorfer
  fullname: Wernsdorfer, Wolfgang
  organization: Physikalisches Institut and Institute of Nanotechnology, Karlsruhe Institute of Technology , Wolfgang-Gaede-Strasse 1, 76131 Karlsruhe, Germany
– sequence: 8
  givenname: Rana
  surname: Hamze
  fullname: Hamze, Rana
  organization: Laboratoire de Chimie et Physique Quantiques, UMR 5626, Université de Toulouse 3, Paul Sabatier , 118 route de Narbonne, 31062 Toulouse, France
– sequence: 9
  givenname: Cyril
  surname: Martins
  fullname: Martins, Cyril
  organization: Laboratoire de Chimie et Physique Quantiques, UMR 5626, Université de Toulouse 3, Paul Sabatier , 118 route de Narbonne, 31062 Toulouse, France
– sequence: 10
  givenname: Nicolas
  surname: Suaud
  fullname: Suaud, Nicolas
  organization: Laboratoire de Chimie et Physique Quantiques, UMR 5626, Université de Toulouse 3, Paul Sabatier , 118 route de Narbonne, 31062 Toulouse, France
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  givenname: Nathalie
  surname: Guihéry
  fullname: Guihéry, Nathalie
  organization: Laboratoire de Chimie et Physique Quantiques, UMR 5626, Université de Toulouse 3, Paul Sabatier , 118 route de Narbonne, 31062 Toulouse, France
– sequence: 12
  givenname: Anne-Laure
  surname: Barra
  fullname: Barra, Anne-Laure
  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
– sequence: 13
  givenname: Cyrille
  orcidid: 0000-0002-6726-2086
  surname: Train
  fullname: Train, Cyrille
  organization: Laboratoire National des Champs Magnétiques Intenses, UPR CNRS 3228, Université Grenoble-Alpes , 25 rue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France
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Snippet A series of mononuclear [M(hfa) (pic) ] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = Fe , Co , Ni , Zn ) compounds were...
A series of mononuclear [M(hfa)2(pic)2] (Hhfa = 1,1,1,5,5,5-hexafluoro-2,4-pentanedione; pic = 4-methylpyridine; M = FeII, CoII, NiII, ZnII) compounds were...
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Title From Positive to Negative Zero-Field Splitting in a Series of Strongly Magnetically Anisotropic Mononuclear Metal Complexes
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