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J. A. SERTH-GUZZO ET AL.
is within the range (24°–45°) apparently required to form
low-spin pyridine complexes. The absolute orientation
of imidazole ligands in observed in low-spin complexes
encompasses the entire possible range of 0°–45° and thus
no particular absolute orientation is needed to form a low-
spin imidazole complex (even with an S4-ruffled core).
Thus there appears to be no steric constraints on either
the absolute or relative imidazole orientation in order to
form the low-spin complex [Fe(TMP)(4-CNPy)(HIm)]
ClO4. We therefore believe that the relative perpendicular
orientation of the imidazole and pyridine ligands in low-
spin [Fe(TMP)(4-CNPy)(HIm)]ClO4 are the result of
bonding considerations and are not required by steric
considerations. The relative perpendicular orientation
is in agreement with the bonding requirements of the
p-acceptor ligand which requires a filled orbital (dxz) and
the p-donor ligand which interacts with the orthogonal
half-filled orbital (dyz).
Axial bond distance comparisons are also consistent
with the idea that the relative ligand orientation is
controlled by bonding. The axial Fe–N(imidazole)
distance of 1.945 (4) Å is shorter than that observed in
any bis-imidazole iron(III) derivative (Table 2), while
the axial Fe–N(pyridine) distance of 2.021 (4) Å is as
long as or longer than the Fe–N(pyridine) distances
observed in the bis-pyridine derivatives. The short
Fe–N(imidazole) distance is most consistent with very
strong p-bonding between the iron(III) and imidazole.
The Fe–N(imidazole) distance is also much shorter than
the 2.068 (4) Å distance found for the five-coordinate
high-spin complex [Fe(OEP)(2-MeHIm)]ClO4 where
strong axial bonding might be expected [42].
interesting and possibly distinctive ground state. A final
system with two strong p-accepting ligands ([Fe(TPP)
(4-CNPy)2]ClO4) has a quadrupole splitting value of
0.65 mm/s and an axial EPR spectrum [9].
EPR spectra of low-spin bis-ligated iron(III)
porphyrinates have been shown to be particularly
informative about the electronic structure. The relative
energies of the three d-orbitals lowest in energy can be
determined from the EPR g-values utilizing the Taylor
formulation [48, 49]. Moreover, the EPR spectral type
provides additional information. The observed type of
EPR spectrum for all complexes listed in Table 2 are also
given in the table when the spectrum has been measured.
When the two planar axial ligands have a relative parallel
orientation, rhombic spectra, with three distinct g-values,
are observed. This is the result of a modest energy
difference between the dxy and dyz orbitals since both
axial ligands interact with only one of the two. However,
when the two axial ligands planes have a dihedral angle
close to 90°, i.e. a relative perpendicular orientation, a
spectral type called gmax is observed. In this case, the
two d orbitals interact more or less equivalently with the
perpendicularly aligned ligands, leading to a very small
energy gap between the dxy and dxz orbitals. A third type,
with two strong p-acceptor ligands such as isocyanides,
leads to an axial spectrum being observed. This is the
result of the dxy orbital becoming the highest energy
orbital of the three t2g orbitals as the energies of two dp
orbitals are lowered because of the interaction with the
p-acceptor ligands. We know of no case where a relative
orientation of the two planar ligands leads to a rhombic
EPR spectrum.
Although we have found and characterized two
different crystalline forms of [Fe(TMP)(4-CNPy)(HIm)]
ClO4, it is to be noted that the crystal structure, as well as
the molecular structure, of both forms are quite similar.
The cell packing diagrams for form A and form B (see
Fig. 5) show that the packing of [Fe(TMP)(4-CNPy)
(HIm)]+ cations is essentially identical even though
the solvent content in the two lattices clearly requires
different cell volumes. Thus the two forms of [Fe(TMP)
(4-CNPy)(HIm)]ClO4 represent an additional set of
cases of lattice packing dominated by the large metallo-
porphyrin species [43–46].
The Mössbauer spectrum of polycrystalline form A
taken at 170 K is shown in Fig. 3. The spectrum illustrates
a doublet with a quadrupole splitting of ∆Eq = 1.935 (9)
mm/s and an isomer shift δ of 0.189 (7) mm/s. The isomer
shift is similar to values reported for other low-spin ferric
hemes [5, 6, 10, 47]. Quadrupole splitting values less than
~1.75mm/saretypicalforlow-spiniron(III)porphyrinates
with axial ligands in the perpendicular orientation and a
“pure” (dxy)2(dxz, dyz)3 ground state [5, 6, 10], while values
greater than ~2.00 mm/s are typical for species with
relative parallel orientation [5, 6]. With a quadrupole
splitting value for form A in the middle (between) of
the two limiting set of values, this is consistent with an
What type of EPR spectrum will [Fe(TMP)(4-CNPy)
(HIm)]ClO4 display? From the data of Table 2, two
distinct possibilities can be envisioned. The perpendicular
orientation of the two ligands in [Fe(TMP)(4-CNPy)
(HIm)]ClO4 suggests that a strong gmax spectrum would
be expected. However, the expected synergic bonding
of the two ligands, one p accepting and one p donating,
leads to a different prediction. The axial ligands and the
metal dxy and dxz orbitals are 90° apart. Thus, one ligand
(the p acceptor) will interact with the filled dxz orbital and
the other ligand (the p donor) will interact with the singly
occupied dyz orbital to give the two orbitals differing
energies and an expected rhombic EPR spectrum.
Single-crystal EPR spectral measurements for [Fe(TMP)
(4-CNPy)(HIm)]ClO4 reveal a rhombic spectrum with g
values of 3.05, 2.07 and 1.22. This clearly shows that the
dxz and dyz orbitals are separated in energy.
With the available g-values for [Fe(TMP)(4-CNPy)
(HIm)]ClO4 the Taylor formalism [48] can now be used
to evaluate the relative energies of the three lowest d
orbitals. These values, expressed in terms of the energy
of spin orbit coupling constant λ are shown on the right
hand side of Fig. 6. For comparison, the energies of a
bis-ligated 1-methylimidazole complex is shown at the
left [6]. Although the energy difference between the dxz
Copyright © 2016 World Scientific Publishing Company
J. Porphyrins Phthalocyanines 2016; 20: 8–11