A theoretical study of zero-field splitting in Fe(IV)S6 (S=1) and Fe(III)S6 (S=1/2) core complexes, [FeIV(Et2dtc)3−n(mnt)n](n−1)− and [FeIII(Et2dtc)3−n(mnt)n]n− (n=0, 1, 2, 3): The origin of the magnetic anisotropy

[Display omitted] ► Ab initio based ligand field analysis of the electronic structure of FeIVS6 and FeIIIS6 chelate complexes are reported. ► Magnetic anisotropy results from non-additive contributions to the ligand field. ► Isothermal magnetizations are rationalized using a concept put forward by L...

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Published in:Coordination chemistry reviews Vol. 257; no. 1; pp. 27 - 41
Main Authors: Atanasov, Mihail, Surawatanawong, Panida, Wieghardt, Karl, Neese, Frank
Format: Journal Article
Language:English
Japanese
Published: Elsevier B.V 01.01.2013
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ISSN:0010-8545, 1873-3840
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Abstract [Display omitted] ► Ab initio based ligand field analysis of the electronic structure of FeIVS6 and FeIIIS6 chelate complexes are reported. ► Magnetic anisotropy results from non-additive contributions to the ligand field. ► Isothermal magnetizations are rationalized using a concept put forward by L. Orgel. ► The potential of state-of-art ab initio calculations to explore magneto structural correlations is demonstrated. Multireference ab initio calculations and ligand field analysis of a series of complexes with Fe(IV)S6 (S=1) [FeIV(Et2dtc)3−n(mnt)n](n−1)− and Fe(III)S6 (S=1/2) [FeIII(Et2dtc)3−n(mnt)n]n− cores ((mnt)2−=maleonitriledithiolate (2−), (Et2dtc)1−=diethyldithiocarbamato (1−) ligands, n=0, 1, 2, 3) are reported and used to understand their magnetic and spectroscopic (ESR) properties. These systems feature large and variable values of D for the S=1 complexes of Fe(IV) and strongly anisotropic g-tensors for the S=1/2 complexes of Fe(III). The calculations are in good to excellent agreement with experiment. We utilize a historic concept put forward by Orgel as early as 1961 [39] in order to analyze the computational data. The non-additive contributions to ligand field due to the π-conjugated systems of the chelate ligands mnt2− and Et2dtc− are responsible for the large magnetic anisotropy. These contributions are even more important than geometric distortions imposed by the rigid ligand cores. The correlations have been demonstrated and quantified using an extended ligand field (LF) model with parameters adjusted to complete active space self-consistent field (CASSCF) calculations corrected for dynamic correlation with the second order N-electron valence perturbation theory (NEVPT2). According to this analysis, the topology of the intrinsic π-electron system of the mnt2− and Et2dtc− ligands causes a splitting of the octahedral t2g orbitals of different sign for mnt2− (e>a1, in-phase coupling) and Et2dtc1− (a1>e, out-of-phase coupling). When combined with the π-donor ability of the mnt2− and Et2dtc− shown by theory and experiment to be much stronger in mnt2− compared to Et2dtc1− this leads to large orbital contributions to the magnetic moment and to a negative D for [Fe(mnt)(dtc)2] with an easy axis of magnetization bisecting the SFeS(mnt) bite angle. Using this ab initio based renewed concept, field dependent isothermal magnetizations reported previously (Milsmann et al., 2010 [25]) have been re-interpreted. We show that the orthorhombic anisotropy for [FeIV(Et2dtc)(mnt)2]1− (2ox) and [FeIV(Et2dtc)2(mnt)]0 (3ox), that has never been discussed before, leads to large zero-field splitting parameter E. At the same time it is pointed out, that the D and E spin-Hamiltonian parameters cannot be uniquely extracted from a fit to the magnetic susceptibility data, unless combined with other sophisticated spectroscopic experiments. Applying the same anisotropic π-bonding model, orbital contributions leading to strongly anisotropic g-tensors reported from simulation of ESR data of the Fe(III)S6 (S=1/2) cores in complexes [FeIII(Et2dtc)3−n(mnt)n]n− (n=0, 1, 2, 3) have been rationalized.
AbstractList [Display omitted] ► Ab initio based ligand field analysis of the electronic structure of FeIVS6 and FeIIIS6 chelate complexes are reported. ► Magnetic anisotropy results from non-additive contributions to the ligand field. ► Isothermal magnetizations are rationalized using a concept put forward by L. Orgel. ► The potential of state-of-art ab initio calculations to explore magneto structural correlations is demonstrated. Multireference ab initio calculations and ligand field analysis of a series of complexes with Fe(IV)S6 (S=1) [FeIV(Et2dtc)3−n(mnt)n](n−1)− and Fe(III)S6 (S=1/2) [FeIII(Et2dtc)3−n(mnt)n]n− cores ((mnt)2−=maleonitriledithiolate (2−), (Et2dtc)1−=diethyldithiocarbamato (1−) ligands, n=0, 1, 2, 3) are reported and used to understand their magnetic and spectroscopic (ESR) properties. These systems feature large and variable values of D for the S=1 complexes of Fe(IV) and strongly anisotropic g-tensors for the S=1/2 complexes of Fe(III). The calculations are in good to excellent agreement with experiment. We utilize a historic concept put forward by Orgel as early as 1961 [39] in order to analyze the computational data. The non-additive contributions to ligand field due to the π-conjugated systems of the chelate ligands mnt2− and Et2dtc− are responsible for the large magnetic anisotropy. These contributions are even more important than geometric distortions imposed by the rigid ligand cores. The correlations have been demonstrated and quantified using an extended ligand field (LF) model with parameters adjusted to complete active space self-consistent field (CASSCF) calculations corrected for dynamic correlation with the second order N-electron valence perturbation theory (NEVPT2). According to this analysis, the topology of the intrinsic π-electron system of the mnt2− and Et2dtc− ligands causes a splitting of the octahedral t2g orbitals of different sign for mnt2− (e>a1, in-phase coupling) and Et2dtc1− (a1>e, out-of-phase coupling). When combined with the π-donor ability of the mnt2− and Et2dtc− shown by theory and experiment to be much stronger in mnt2− compared to Et2dtc1− this leads to large orbital contributions to the magnetic moment and to a negative D for [Fe(mnt)(dtc)2] with an easy axis of magnetization bisecting the SFeS(mnt) bite angle. Using this ab initio based renewed concept, field dependent isothermal magnetizations reported previously (Milsmann et al., 2010 [25]) have been re-interpreted. We show that the orthorhombic anisotropy for [FeIV(Et2dtc)(mnt)2]1− (2ox) and [FeIV(Et2dtc)2(mnt)]0 (3ox), that has never been discussed before, leads to large zero-field splitting parameter E. At the same time it is pointed out, that the D and E spin-Hamiltonian parameters cannot be uniquely extracted from a fit to the magnetic susceptibility data, unless combined with other sophisticated spectroscopic experiments. Applying the same anisotropic π-bonding model, orbital contributions leading to strongly anisotropic g-tensors reported from simulation of ESR data of the Fe(III)S6 (S=1/2) cores in complexes [FeIII(Et2dtc)3−n(mnt)n]n− (n=0, 1, 2, 3) have been rationalized.
Author Neese, Frank
Surawatanawong, Panida
Wieghardt, Karl
Atanasov, Mihail
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  givenname: Mihail
  surname: Atanasov
  fullname: Atanasov, Mihail
  email: mihail.atanasov@mpi-mail.mpg.de
  organization: Max-Planck Institut für Bioanorganische Chemie, Stiftstrasse 34-36, D-45470 Mülheim an der Ruhr, Germany
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  givenname: Panida
  surname: Surawatanawong
  fullname: Surawatanawong, Panida
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  givenname: Karl
  surname: Wieghardt
  fullname: Wieghardt, Karl
  organization: Max-Planck Institut für Bioanorganische Chemie, Stiftstrasse 34-36, D-45470 Mülheim an der Ruhr, Germany
– sequence: 4
  givenname: Frank
  surname: Neese
  fullname: Neese, Frank
  email: neese@mpi-mail.mpg.de
  organization: Max-Planck Institut für Bioanorganische Chemie, Stiftstrasse 34-36, D-45470 Mülheim an der Ruhr, Germany
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Issue 1
Keywords Ab initio multireference methods
Spin-Hamiltonian (SH)
Magnetization
Ligand field theory (LFT)
Single molecule magnetism (SMM)
N-electron valence second order perturbation theory (NEVPT2)
Geometric
Electronic
Zero-field splitting
Magnetic susceptibility
d–d absorption spectra
Angular overlap model (AOM)
Structure
Complete active space self-consistent field (CASSCF)
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Japanese
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Snippet [Display omitted] ► Ab initio based ligand field analysis of the electronic structure of FeIVS6 and FeIIIS6 chelate complexes are reported. ► Magnetic...
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SubjectTerms Ab initio multireference methods
Angular overlap model (AOM)
Complete active space self-consistent field (CASSCF)
d–d absorption spectra
Electronic
Geometric
Ligand field theory (LFT)
Magnetic susceptibility
Magnetization
N-electron valence second order perturbation theory (NEVPT2)
Single molecule magnetism (SMM)
Spin-Hamiltonian (SH)
Structure
Zero-field splitting
Title A theoretical study of zero-field splitting in Fe(IV)S6 (S=1) and Fe(III)S6 (S=1/2) core complexes, [FeIV(Et2dtc)3−n(mnt)n](n−1)− and [FeIII(Et2dtc)3−n(mnt)n]n− (n=0, 1, 2, 3): The origin of the magnetic anisotropy
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