A green
complex [Fe(L3)] (1), supported
by the deprotonated form of a hexadentate noninnocent redox-active
thioether-appended 2-aminophenolate ligand (H4L3 = N,N′-bis(2-hydroxy-3,5-di-tert-butylphenyl)-2,2′-diamino(diphenyldithio)ethane),
has been synthesized and structurally characterized at 100(2) K and
298(2) K. In CH2Cl2, 1 displays
two oxidative and a reductive one-electron redox processes at E
1/2 values of −0.52 and 0.20 V, and −0.85
V versus the Fc+/Fc redox couple, respectively. The one-electron
oxidized 1
+ and one-electron reduced 1
– forms, isolated as a blackish-blue solid 1(PF6)·CH2Cl2 (2) and a gray solid [Co(η
5–C5H5)2]1·DMF
(3), have been structurally characterized at 100(2) K.
Structural parameters at 100 K of the ligand backbone and metrical
oxidation state values unambiguously establish the electronic states
as [FeIII{(LAP
O,N
)2–}{(LISQ
O,N
)•–}{(L
S,S
)0}] (1) (two tridentate halves are electronically asymmetric–ligand
mixed-valency), [FeIII{(LISQ
O,N
)•–}{(LISQ
O,N
)•–}{(L
S,S
)0}]+ (1
+), and [FeIII{(LAP
O,N
)2–}{(LAP
O,N
)2–}{(L
S,S
)0}]− (1
−) [dianionic 2-amidophenolate(2−) (LAP
O,N
)2– and monoanionic
2-iminobenzosemiquinonate(1−) π-radical (S
rad = 1/2) (LISQ)•– redox level]. Mössbauer spectral data of 1 at
295, 200, and 80 K reveal that it has a major low-spin (ls)-Fe(III)
and a minor ls-Fe(II) component (redox isomers), and at 7 K, the major
component exists exclusively. Thus, in 1, the occurrence
of a thermally driven valence-tautomeric (VT) equilibrium (asymmetric)
[FeIII{(LAP
O,N
)2–}{(LISQ
O,N
)•–}{(L
S,S
)0}] ⇌ (symmetric)
[FeII{(LISQ
O,N
)•–}{(LISQ
O,N
)•–}{(L
S,S
)0}] (80–295
K) is implicated. Mössbauer spectral parameters unequivocally
establish that 1
+ is a ls-Fe(III) complex.
In contrast, the monoanion 1
– contains
a high-spin (hs)-Fe(III) center (S
Fe =
5/2), as is deduced from its Mössbauer and EPR spectra. Complexes 1–3 possess total spin ground states S
t = 0, 1/2, and 5/2, respectively, based on 1H NMR and EPR spectra, the variable-temperature (2–300
K) magnetic behavior of 2, and the μ
eff value of 3 at 300 K. Broken-symmetry
density functional theory (DFT) calculations at the B3LYP-level of
theory reveal that the unpaired electron in 1
+/2 is due to the (LISQ)•– redox level [ls-Fe(III) (S
Fe = 1/2)
is strongly antiferromagnetically coupled to one of the (LISQ)•– radicals (S
rad = 1/2)], and 1
–/3 is
a hs-Fe(III) complex, supported by (L3)4– with two-halves in the (LAP)2– redox
level. Complex 1 can have either a symmetric or asymmetric
electronic state. As per DFT calculation, the former state is stabilized
by −3.9 kcal/mol over the latter (DFT usually stabilizes electronically
symmetric structure). Time-dependent (TD)-DFT calculations shed light
on the origin of observed UV–vis–NIR spectral absorptions
for 1–3 and corroborate the results
of spectroelectrochemical experiments (300–1100 nm) on 1 (CH2Cl2; 298 K). Variable-temperature
(218–298 K; CH2Cl2) absorption spectral
(400–1000 nm) studies on 1 justify the presence
of VT equilib...