Electronic structure of bispidine iron(IV) oxo complexes.
The electronic structure, based on DFT calculations, of a range of FeIV=O complexes with two tetra- (L1 and L2) and two isomeric pentadentate bispidine ligands (L3 and L4) is discussed with special emphasis on the relative stability of the two possible spin states (S = 1, triplet, intermediate-spin,...
Váldodahkkit: | , , , , |
---|---|
Materiálatiipa: | Journal article |
Giella: | English |
Almmustuhtton: |
2007
|
_version_ | 1826275610894270464 |
---|---|
author | Anastasi, A Comba, P Mcgrady, J Lienke, A Rohwer, H |
author_facet | Anastasi, A Comba, P Mcgrady, J Lienke, A Rohwer, H |
author_sort | Anastasi, A |
collection | OXFORD |
description | The electronic structure, based on DFT calculations, of a range of FeIV=O complexes with two tetra- (L1 and L2) and two isomeric pentadentate bispidine ligands (L3 and L4) is discussed with special emphasis on the relative stability of the two possible spin states (S = 1, triplet, intermediate-spin, and S = 2, quintet, high-spin; bispidines are very rigid diazaadamantane-derived 3,7-diazabicyclo[3.3.1]nonane ligands with two tertiary amine and two or three pyridine donors, leading to cis-octahedral [(X)(L)FeIV=O]2+ complexes, where X = NCCH3, OH2, OH-, and pyridine, and where X = pyridine is tethered to the bispidine backbone in L3, L4). The two main structural effects are a strong trans influence, exerted by the oxo group in both the triplet and the quintet spin states, and a Jahn-Teller-type distortion in the plane perpendicular to the oxo group in the quintet state. Due to the ligand architecture the two sites for substrate coordination in complexes with the tetradentate ligands L1 and L2 are electronically very different, and with the pentadentate ligands L3 and L4, a single isomer is enforced in each case. Because of the rigidity of the bispidine ligands and the orientation of the "Jahn-Teller axis", which is controlled by the sixth donor X, the Jahn-Teller-type distortion in the high-spin state of the two isomers is quite different. It is shown how this can be used as a design principle to tune the relative stability of the two spin states. |
first_indexed | 2024-03-06T23:01:23Z |
format | Journal article |
id | oxford-uuid:62415851-c377-4504-a7b2-3341f34684cc |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-06T23:01:23Z |
publishDate | 2007 |
record_format | dspace |
spelling | oxford-uuid:62415851-c377-4504-a7b2-3341f34684cc2022-03-26T18:04:59ZElectronic structure of bispidine iron(IV) oxo complexes.Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:62415851-c377-4504-a7b2-3341f34684ccEnglishSymplectic Elements at Oxford2007Anastasi, AComba, PMcgrady, JLienke, ARohwer, HThe electronic structure, based on DFT calculations, of a range of FeIV=O complexes with two tetra- (L1 and L2) and two isomeric pentadentate bispidine ligands (L3 and L4) is discussed with special emphasis on the relative stability of the two possible spin states (S = 1, triplet, intermediate-spin, and S = 2, quintet, high-spin; bispidines are very rigid diazaadamantane-derived 3,7-diazabicyclo[3.3.1]nonane ligands with two tertiary amine and two or three pyridine donors, leading to cis-octahedral [(X)(L)FeIV=O]2+ complexes, where X = NCCH3, OH2, OH-, and pyridine, and where X = pyridine is tethered to the bispidine backbone in L3, L4). The two main structural effects are a strong trans influence, exerted by the oxo group in both the triplet and the quintet spin states, and a Jahn-Teller-type distortion in the plane perpendicular to the oxo group in the quintet state. Due to the ligand architecture the two sites for substrate coordination in complexes with the tetradentate ligands L1 and L2 are electronically very different, and with the pentadentate ligands L3 and L4, a single isomer is enforced in each case. Because of the rigidity of the bispidine ligands and the orientation of the "Jahn-Teller axis", which is controlled by the sixth donor X, the Jahn-Teller-type distortion in the high-spin state of the two isomers is quite different. It is shown how this can be used as a design principle to tune the relative stability of the two spin states. |
spellingShingle | Anastasi, A Comba, P Mcgrady, J Lienke, A Rohwer, H Electronic structure of bispidine iron(IV) oxo complexes. |
title | Electronic structure of bispidine iron(IV) oxo complexes. |
title_full | Electronic structure of bispidine iron(IV) oxo complexes. |
title_fullStr | Electronic structure of bispidine iron(IV) oxo complexes. |
title_full_unstemmed | Electronic structure of bispidine iron(IV) oxo complexes. |
title_short | Electronic structure of bispidine iron(IV) oxo complexes. |
title_sort | electronic structure of bispidine iron iv oxo complexes |
work_keys_str_mv | AT anastasia electronicstructureofbispidineironivoxocomplexes AT combap electronicstructureofbispidineironivoxocomplexes AT mcgradyj electronicstructureofbispidineironivoxocomplexes AT lienkea electronicstructureofbispidineironivoxocomplexes AT rohwerh electronicstructureofbispidineironivoxocomplexes |