C O M M U N I C A T I O N S
measured by Evan’s method from room temperature to 190 K
(Figure S5 in SI); SQUID data show no change in the magnetic
moment between 300 and 10 K. EPR data of both frozen halocarbon
solutions and the crystalline [FeIII(TipsiPP)]+[CB11H6Br6]- have a
g ) 4.2 signal (Figure S4 in SI). Mo¨ssbauer spectra were obtained
with the 57Fe-enriched sample at 6 K, with an isomer shift of 0.33
mm/s (a typical value for Fe(III)), but with a very large quadrupole
splitting value of 5.16 mm/s (Figure S6 in SI). Solid-state NMR
also gives an upfield signal at -80 ppm for the â-pyrrole hydrogens,
confirming that the four-coordinate Fe(III) porphyrin is stable both
in solid and solution phases.
Although four-coordinate Fe(III) heme is unlikely in any heme
protein, the intermediate spin state of Fe(III) porphyrins has an
interesting counterpart in nature.11-17 In cytochrome c′, the heme
5
3
is believed to be a quantum admixed S ) /2 and S ) /2 spin
state.18-20 Depending on the field strength of the ligand coordinated
to the iron, the ratio of S ) /2 to S ) /2 character varies: as the
5
3
ligand strength becomes weaker, the spin state of iron approaches
3
the pure intermediate spin state of /2.
In summary, the first four-coordinate Fe(III) porphyrin complex
has been isolated and fully characterized in both solution and solid
3
state and shows a pure S )
/ intermediate spin state. The
2
combination of steric hindrance of a bis-pocket porphyrin with
weakly coordinating anions has proved essential in isolation of this
highly elusive species, whose reactivity we are still exploring.
Figure 3. X-ray single-crystal structure of (a) [FeIII(TipsiPP)]+[CB11H6Br6]-
and (b) FeIII(TipsiPP)(CF3SO3). Figure S9 in SI provides a crystal packing
diagram for [FeIII(TipsiPP)]+[CB11H6Br6]- showing a layered salt structure
with alternating planes of positive and negative charges.
Acknowledgment. We gratefully acknowledge the assistance
of Alexandre Anasta´cio and Prof. J. W. Stucki (Mo¨ssbauer), Prof.
C. M. Rienstra, and Dr. Donghua Zhou (SSNMR), Dr. M. J. Nilges
(EPR), and Jin Ho Bang (SQUID). These studies were supported
by National Science Foundation (CHE03-15494).
methane/heptane solution inside an inert atmosphere box. The single
crystals were redissolved in dry CD2Cl2 and tested by NMR to
confirm no contamination with water during the crystal growing
process. The crystal structure (Figure 3) confirms the absence of
axial ligation to the iron porphyrin. The average Fe-N bond length
is 1.94 ( 0.01 Å with the iron sitting in the porphyrin plane. This
very short bond length is consistent with the removal of the unpaired
Supporting Information Available: Synthesis, characterization,
and X-ray crystallographic details in CIF format. This material is
electron from the dx -y orbital.1,10 The porphyrin is slightly ruffled,
with meso-carbons above and below the average nitrogen plane by
0.23 Å. The carborane anion is definitiVely not coordinated to the
iron and is fully outside of the porphyrin pocket. The resulting salt
has a layered structure with alternating planes of positive and
negative charges (a crystal packing diagram is given as Figure S9
in SI). A similar packing structure has been reported for [FeTPP]-
[Ag(CB11H6Br6)2]‚4(p-xylene) with the exception of the coordina-
tion of the xylene to the iron center.2,3
2
2
References
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Further characterization data on the four-coordinate [FeIII-
(TipsiPP)]+[CB11H6Br6]- are all consistent with a 3/2 intermediate
spin ground state. The solution magnetic susceptibility of the four-
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