Molecular Design of Anionic Phthalocyanines with π–π
Stacking Columnar Arrangement. Crystal Structures, Optical, and Magnetic
Properties of Salts with the Iron(I) Hexadecachlorophthalocyanine
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Abstract
Ionic
compounds containing iron(I) hexadecachlorophthalocyanine
anions have been obtained for the first time as single crystals: (PPN<sup>+</sup>){[Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup>}
(<b>1</b>), (Ph<sub>3</sub>MeP<sup>+</sup>)<sub>2</sub>{[Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup>}(Br<sup>–</sup>)·C<sub>6</sub>H<sub>4</sub>Cl<sub>2</sub> (<b>2</b>), and (PPN<sup>+</sup>)<sub>2</sub>[Fe(I, II)Cl<sub>16</sub>Pc(−2)]<sub>3</sub><sup>(2−)</sup>·4C<sub>6</sub>H<sub>4</sub>Cl<sub>2</sub> (<b>3</b>), where PPN<sup>+</sup> is the cation of bis(triphenylphosphoranylidene)ammonium
and Ph<sub>3</sub>MeP<sup>+</sup> is the triphenylmethylphosphonium
cation. The [Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup> anions form closely packed π–π stacking columns
in <b>1</b>–<b>3</b>. Salts <b>1</b> and <b>2</b> with integer −1 charge on iron phthalocyanines have
uniform and weakly dimerized columns, respectively. Salt <b>3</b> has two cations per three iron phthalocyanine molecules which are
arranged in trimers within the columns. Different shift of phthalocyanines
at the same interplanar distances of 3.33–3.38 Å provides
essentially shorter Fe···Fe distances in <b>3</b> (3.62–3.84 Å) than those in <b>1</b> and <b>2</b> (5.07–5.45 Å). Calculations show a strong LUMO–LUMO
overlapping between [Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup> in <b>1</b>–<b>3</b> with the overlap integrals
of 4.1–7.6 × 10<sup>–3</sup>. Weak signals attributed
to the [Fe(II)Cl<sub>16</sub>Pc(−3)]<sup>−</sup> species
with the delocalization of electron on the phthalocyanine macrocycles
are observed in the EPR spectra of <b>1</b>–<b>3</b>. The content of this admixture is less than 1% in all salts. Nevertheless,
static magnetic susceptibility measurements for <b>3</b> detected
significant magnetization. The effective magnetic moment is 4.05 μ<sub>B</sub> per formula unit at 300 K. It can originate from the spins
localized on the iron atoms of [Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup>. The Weiss temperature of −53 K in the 60–300
K range indicates a strong antiferromagnetic interaction of spins
which results in the decreases of magnetic moment of <b>3</b> with temperature below 220 K down to 2.72 μ<sub>B</sub> at
6 K. Optical spectra of <b>1</b>–<b>3</b> show
bands ascribed to [Fe(I)Cl<sub>16</sub>Pc(−2)]<sup>−</sup> at 339–349, 538–548, 685–691, and 805–821
nm. The bands in the NIR range at 1740–1810 nm were attributed
to charge transfer excitations within phthalocyanine columns associated
with the unpaired electrons on the iron atoms