Synthesis, Characterisation and Molecular Hyperpolarisabilities of Pseudo‐Octahedral Hydrido(nitrile)iron( II ) Complexes for Nonlinear Optics: X‐ray Structure of [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ]·CH 2 Cl 2

A series of ionic pseudo‐octahedral trans ‐hydrido(nitrile)iron( II ) complexes with the general formula [Fe(H)(dppe) 2 (4‐NCR)][PF 6 ] [dppe = 1,2‐bis(diphenylphosphanyl)ethane; R = acceptor‐substituted conjugated ligand] have been synthesised by chloride abstraction from the starting compound tran...

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Veröffentlicht in:European journal of inorganic chemistry 2006-06, Vol.2006 (11), p.2175-2185
Hauptverfasser: Robalo, Maria Paula, Teixeira, António P. S., Garcia, Maria Helena, Minas da Piedade, M. Fátima, Duarte, M. Teresa, Dias, Alberto Romão, Campo, Jochen, Wenseleers, Wim, Goovaerts, Etienne
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container_issue 11
container_start_page 2175
container_title European journal of inorganic chemistry
container_volume 2006
creator Robalo, Maria Paula
Teixeira, António P. S.
Garcia, Maria Helena
Minas da Piedade, M. Fátima
Duarte, M. Teresa
Dias, Alberto Romão
Campo, Jochen
Wenseleers, Wim
Goovaerts, Etienne
description A series of ionic pseudo‐octahedral trans ‐hydrido(nitrile)iron( II ) complexes with the general formula [Fe(H)(dppe) 2 (4‐NCR)][PF 6 ] [dppe = 1,2‐bis(diphenylphosphanyl)ethane; R = acceptor‐substituted conjugated ligand] have been synthesised by chloride abstraction from the starting compound trans ‐[FeHCl(dppe) 2 ] and fully characterised. First hyperpolarisabilities ( β ) have been determined by hyper‐Rayleigh scattering (HRS) at the fundamental wavelength of 1072 nm and the high near‐resonant values obtained (up to 1130 × 10 –30 esu) are interpreted in terms of the two‐level model (TLM) and are correlated with IR and NMR spectroscopic data. Wavelength‐dependent HRS has been performed in the 1072–1580 nm range for two of the compounds, namely [Fe(H)(dppe) 2 {4‐NC(CH)(CH)C 6 H 4 NO 2 }][PF 6 ] and [Fe(H)(dppe) 2 {4‐NCC 6 H 4 (CH)(CH)C 6 H 4 NO 2 }][PF 6 ]. These results clearly show the two‐photon resonance but also the shortcomings of the TLM when it comes to deriving reliable static β values. A structural study of the compound [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ] by X‐ray diffraction shows that it crystallises in the centrosymmetric monoclinic space group P 2 1 / n , with four molecules in the unit cell and a pairwise antiparallel alignment of the dipoles. (© Wiley‐VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, Germany, 2006)
doi_str_mv 10.1002/ejic.200501050
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First hyperpolarisabilities ( β ) have been determined by hyper‐Rayleigh scattering (HRS) at the fundamental wavelength of 1072 nm and the high near‐resonant values obtained (up to 1130 × 10 –30 esu) are interpreted in terms of the two‐level model (TLM) and are correlated with IR and NMR spectroscopic data. Wavelength‐dependent HRS has been performed in the 1072–1580 nm range for two of the compounds, namely [Fe(H)(dppe) 2 {4‐NC(CH)(CH)C 6 H 4 NO 2 }][PF 6 ] and [Fe(H)(dppe) 2 {4‐NCC 6 H 4 (CH)(CH)C 6 H 4 NO 2 }][PF 6 ]. These results clearly show the two‐photon resonance but also the shortcomings of the TLM when it comes to deriving reliable static β values. A structural study of the compound [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ] by X‐ray diffraction shows that it crystallises in the centrosymmetric monoclinic space group P 2 1 / n , with four molecules in the unit cell and a pairwise antiparallel alignment of the dipoles. (© Wiley‐VCH Verlag GmbH &amp; Co. 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First hyperpolarisabilities ( β ) have been determined by hyper‐Rayleigh scattering (HRS) at the fundamental wavelength of 1072 nm and the high near‐resonant values obtained (up to 1130 × 10 –30 esu) are interpreted in terms of the two‐level model (TLM) and are correlated with IR and NMR spectroscopic data. Wavelength‐dependent HRS has been performed in the 1072–1580 nm range for two of the compounds, namely [Fe(H)(dppe) 2 {4‐NC(CH)(CH)C 6 H 4 NO 2 }][PF 6 ] and [Fe(H)(dppe) 2 {4‐NCC 6 H 4 (CH)(CH)C 6 H 4 NO 2 }][PF 6 ]. These results clearly show the two‐photon resonance but also the shortcomings of the TLM when it comes to deriving reliable static β values. A structural study of the compound [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ] by X‐ray diffraction shows that it crystallises in the centrosymmetric monoclinic space group P 2 1 / n , with four molecules in the unit cell and a pairwise antiparallel alignment of the dipoles. (© Wiley‐VCH Verlag GmbH &amp; Co. 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First hyperpolarisabilities ( β ) have been determined by hyper‐Rayleigh scattering (HRS) at the fundamental wavelength of 1072 nm and the high near‐resonant values obtained (up to 1130 × 10 –30 esu) are interpreted in terms of the two‐level model (TLM) and are correlated with IR and NMR spectroscopic data. Wavelength‐dependent HRS has been performed in the 1072–1580 nm range for two of the compounds, namely [Fe(H)(dppe) 2 {4‐NC(CH)(CH)C 6 H 4 NO 2 }][PF 6 ] and [Fe(H)(dppe) 2 {4‐NCC 6 H 4 (CH)(CH)C 6 H 4 NO 2 }][PF 6 ]. These results clearly show the two‐photon resonance but also the shortcomings of the TLM when it comes to deriving reliable static β values. A structural study of the compound [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ] by X‐ray diffraction shows that it crystallises in the centrosymmetric monoclinic space group P 2 1 / n , with four molecules in the unit cell and a pairwise antiparallel alignment of the dipoles. (© Wiley‐VCH Verlag GmbH &amp; Co. 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title Synthesis, Characterisation and Molecular Hyperpolarisabilities of Pseudo‐Octahedral Hydrido(nitrile)iron( II ) Complexes for Nonlinear Optics: X‐ray Structure of [Fe(H)(dppe) 2 (4‐NCC 6 H 4 NO 2 )][PF 6 ]·CH 2 Cl 2
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