Fe<sup>II</sup>(pap-5NO<sub>2</sub>)<sub>2</sub> and
Fe<sup>II</sup>(qsal-5NO<sub>2</sub>)<sub>2</sub> Schiff-Base Spin-Crossover
Complexes: A Rare Example with Photomagnetism and Room-Temperature
Bistability
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Abstract
We
focus here on the properties of Fe complexes formed with Schiff
bases involved in the chemistry of Fe<sup>III</sup> spin-transition
archetypes. The neutral Fe(pap-5NO<sub>2</sub>)<sub>2</sub> (<b>1</b>) and Fe(qsal-5NO<sub>2</sub>)<sub>2</sub>·Solv (<b>2</b> and <b>2·Solv</b>) compounds (<b>Solv</b> = 2H<sub>2</sub>O) derive from the reaction of Fe<sup>II</sup> salts
with the condensation products of pyridine-2-carbaldehyde with 2-hydroxy-5-nitroaniline
(Hpap-5NO<sub>2</sub>) or 5-nitrosalicylaldehyde with quinolin-8-amine
(Hqsal-5NO<sub>2</sub>), respectively. While the Fe(qsal-5NO<sub>2</sub>)<sub>2</sub>·Solv solid is essentially low spin (S = 0) and
requires temperatures above 300 K to undergo a S = 0 ↔ S =
2 spin-state switching, the Fe(pap-5NO<sub>2</sub>)<sub>2</sub> one
presents a strongly cooperative first-order transition (<i>T</i>↓ = 291 K, <i>T</i>↑ = 308 K) centered at
room temperature associated with a photomagnetic effect at 10 K (<i>T</i><sub>LIESST</sub> = 58 K). The investigation of these magnetic
behaviors was conducted with single-crystal X-ray diffraction (<b>1</b>, 100 and 320 K; <b>2</b>, 100 K), Mössbauer,
IR, UV–vis (<b>1</b> and <b>2·Solv</b>), and
differential scanning calorimetry (<b>1</b>) measurements. The
Mössbauer analysis supports a description of these compounds
as Fe<sup>II</sup> Schiff-base complexes and the occurrence of a metal-centered
spin crossover process. In comparison with Fe<sup>III</sup> analogues,
it appears that an expanded coordination sphere stabilizes the valence
2+ state of the Fe ion in both complexes. Strong hydrogen-bonding
interactions that implicate the phenolato group bound to Fe<sup>II</sup> promote the required extra-stabilization of the S = 2 state and
thus determines the spin transition of <b>1</b> centered at
room temperature. In the lattice, the hydrogen-bonded sites form infinite
chains interconnected via a three-dimensional network of intermolecular
van der Waals contacts and π–π interactions. Therefore,
the spin transition of <b>1</b> involves the synergetic influence
of electrostatic and elastic interactions, which cause the enhancement
of cooperativity and result in the bistability at room temperature