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Bimetallic Sesquifulvalene Complexes–Compounds with Unusually Large Hyperpolarizability β
Author(s) -
Behrens Ulrich,
Brussaard Hugo,
Hagenau Ute,
Heck Jürgen,
Hendrickx Eric,
Körnich Jan,
Van Der Linden Johannes G. M.,
Persoons André,
Spek Anthony L.,
Veldman Nora,
Voss Bea,
Wong Hans
Publication year - 1996
Publication title -
chemistry – a european journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.687
H-Index - 242
eISSN - 1521-3765
pISSN - 0947-6539
DOI - 10.1002/chem.19960020117
Subject(s) - bimetallic strip , hyperpolarizability , chemistry , biochemistry , organic chemistry , catalysis , molecule , polarizability
In order to construct bimetallic organometallic donor–acceptor complexes with nonlinear optical (NLO) properties, the bimetallic sesquifulvalene complexes [{CpFe(η 5 ‐C 5 H 4 )}Z{η 7 ‐C 7 H 6 )Cr‐(CO) 3 }]BF 4 (2BF 4 ) have been synthesized with different bridging functions Z ( 2a : Z = ‐ 2b : Z = C 2 ; 2c : Z ( E )‐C 2 H 2 ). X‐ray structure determinations show that 2a BF 4 and 2c BF 4 crystallize in acentric space groups ( P 4 1 , P 2 1 2 1 2 1 ), whereas crystalline 2b BF 4 has the centric space group P 2 1 / c . The organometallic fragments in 2a adopt a transoid conformation, those in 2b and 2c are cisoid . The cyclo ‐C 5 and cyclo ‐C 7 rings of the sesquifulvalene ligands are almost coplanar; this allows an optimum electronic interaction between the ferrocenyl donor and the [η 7 ‐C 7 H 6 )Cr(CO) 3 ] + acceptor moiety in the crystalline state. Cyclovoltammetric studies show an electrochemically reversible one‐electron oxidation ( > 0 mV vs. FeH/FcH + , FcH = ferrocene) and an irreversible one‐electron reduction (≤–900 mV), which are assigned to the ferrocenyl and [(η 7 ‐C 7 H 6 )Cr(CO) 3 ] + units, respectively. UV/vis spectra reveal low‐energy absorptions for 2a –c at about λ=600 nm, showing strong negative solvatochromism. These absorption maxima are related to a charge‐transfer excitation between the ferrocenyl and the [(η 7 ‐C 7 H 6 )Cr(CO) 3 ] + groups, indicating considerable nonlinear optical properties. Determination of the first hyperpolarizability β by means of hyper Rayleigh scattering yields exceptionally large β values: β( 2b ) = 570 × 10 −30 esu and β( 2c ) = 320 × 10 −30 esu. These unexpectedly large β values are explained by resonance enhancement.