THE IMPORTANCE OF MAGNETIC COUPLING THROUGH ATOMS WITH LARGE SPIN-DENSITIES - STRUCTURE AND MAGNETIC-PROPERTIES OF AKIS-(4'-TERT-BUTYLPHENYL)PORPHINATOMANGANESE(III) HEXACYANOBUTADIENIDE, [MN(III)TTBUPP](-4(CN)(6)](.-)()[C)

Citation
K. Sugiura et al., THE IMPORTANCE OF MAGNETIC COUPLING THROUGH ATOMS WITH LARGE SPIN-DENSITIES - STRUCTURE AND MAGNETIC-PROPERTIES OF AKIS-(4'-TERT-BUTYLPHENYL)PORPHINATOMANGANESE(III) HEXACYANOBUTADIENIDE, [MN(III)TTBUPP](-4(CN)(6)](.-)()[C), Chemistry, 3(1), 1997, pp. 138-142
Citations number
48
Categorie Soggetti
Chemistry
Journal title
ISSN journal
09476539
Volume
3
Issue
1
Year of publication
1997
Pages
138 - 142
Database
ISI
SICI code
0947-6539(1997)3:1<138:TIOMCT>2.0.ZU;2-I
Abstract
[Mn(III)TtBuPP](+)[C-4(CN)(6)](.-) . [(MnTrBuPP)-Tr-III = akis(4'-tert -butylphenyl)porphinatomanganese(III)] has been prepared and structura lly and magnetically characterized. The uniform, linear-chain (1-D) co ordination polymer comprises alternating cations and anions. The bond lengths in planar ion [C-4(CN)(6)](.-) are 1.377(10) (CC-CC), 1.418(7) (C-CCC), 1.414 (C-CN), 1.457 (C-CNMn), 1.150 (C=N), and 1.134 Angstro m (C=NMn). The Mn-N-C angle is 172.3 (4)degrees, and the intrachain Mn ... Mn separation is 10.655 Angstrom. Each [C-4(CN)(6)](.-) unit is b onded to two Mn-III atoms through the interior nitrogen atoms in a tim es-mu(2)-N-sigma manner with N-Mn bond lengths of 2.353 Angstrom. The <(nu)over tilde>(CN) absorptions are at 2217 (w,br) and 2190 (m) cm(-1 ). Above 50 K the magnetic susceptibility of [Mn(III)TtBuPP](+)[C-4(CN )(6)](.-) can be fitted to the Curie-Weiss expression, chi proportiona l to 1/(T - theta), with an effective theta of -13 K. This is consiste nt with weak antiferromagnetic coupling, which is in contrast to the e ffective theta of + 67 K for the uniform chain [(MnOEP)-O-III](+)[C-4( CN)(6)](.-) [OEP = octaethylporphinato]. Here, the [C-4(CN)(6)](.-) un its are bonded to the Mn-III centers through endo CN nitrogen atoms in a similar trans-mu(2) manner. Density functional theory MO calculatio ns reveal that the spin density of the CN nitrogen atom bound to [Mn-I II- TtBuPP](+) (0.019 mu(B) Angstrom(-3)) is significantly lower than that of the N atom bound to [(MnOEP)-O-III]+ (0.102 mu(B) Angstrom(-3) ). This is consistent with the reduced spin coupling observed for [Mn( III)TtBuPP](+)[C-4(CN)(6)](.-) with respect to [(MnOEP)-O-III](+)[C-4( CN)(6)](.-), as evidenced by the lower theta value. The different orie ntations of the [C-4(CN)(6)](.-) units-almost perpendicular (84.72 deg rees) for [Mn(III)TtBuPP](+)[C-4(CN)(6)](.-) and substantially tilted (32.1 degrees) for [(MnOEP)-O-III](+)[C-4(CN)(6)](.-)-may also contrib ute to the poorer overlap and weaker spin coupling. Hence, binding bet ween sites with large spin densities is needed to stabilize strong fer romagnetic coupling.