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 |
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| Main Authors: | , , , |
| Format: | Journal Article |
| Language: | English Japanese |
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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. |
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| 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 |
| Author_xml | – sequence: 1 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 – sequence: 2 givenname: Panida surname: Surawatanawong fullname: Surawatanawong, Panida organization: Department of Chemistry, Faculty of Science, Mahidol University, 272 Rama VI Road, Ratchathewi, Bangkok 10400, Thailand – sequence: 3 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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| CitedBy_id | crossref_primary_10_1002_anie_201606165 crossref_primary_10_1007_s12043_021_02086_0 crossref_primary_10_1016_j_ccr_2015_09_004 crossref_primary_10_1039_C4CP05148C crossref_primary_10_1007_s00269_013_0645_x crossref_primary_10_1134_S0036023615140041 crossref_primary_10_1007_s11243_015_0016_1 crossref_primary_10_1039_D4SC04880F crossref_primary_10_1002_ange_201606165 crossref_primary_10_1016_j_synthmet_2015_02_020 crossref_primary_10_1016_j_ica_2015_01_029 crossref_primary_10_1039_C6CP01620K crossref_primary_10_1038_ncomms14099 crossref_primary_10_1080_00958972_2022_2126770 crossref_primary_10_1002_ejic_201402295 |
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| Copyright | 2012 Elsevier B.V. |
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| 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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► 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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