C O M M U N I C A T I O N S
considerably from the data (dashed line). Thus the combined crystal-
lographic, spectroscopic, and magnetic data indicate that there are two
high-spin iron(II) centers, which are antiferromagnetically coupled to
give a diamagnetic ground state.
Because of the formal oxidation of iron(I) to iron(II) in the reaction
of LRFeNNFeLR to LRFe(µ-η2:η2-AdN6Ad)FeLR, we view the
hexazene ligand as being derived from reductive azide coupling. We
are not aware of any other published examples of reductive coupling
of two azides.
Figure 3. Two possible resonance structures for LRFe(µ-η2:η2-AdN6Ad)FeLR
To our knowledge, these are the first transition metal complexes
with a hexa-nitrogen R2N62- ligand. Although they contain a locally
high concentration of nitrogen atoms, they are remarkably inert as long
as they are protected from O2 and moisture. Under N2, the solid
complexes slowly decompose to a black residue only above 140 °C
in the solid state and do not explosively decompose when struck with
a hammer. This contrasts with several examples of explosive 1,4-
pentaazadien-3-ide complexes.15 Treatment of LMeFe(µ-η2:η2-
AdN6Ad)FeLMe with neutral donor ligands (tert-butylisocyanide,
4-tert-butylpyridine), irradiation (200 W mercury lamp for 70 min),16
or extended heating (100 °C for 5 days, slurry in C6D6) does not result
in a color change or the appearance of new paramagnetically shifted
peaks in the 1H NMR spectrum. This stability contrasts greatly with
metal-free hexazenes, which decompose within minutes upon heating
or irradiating.4a–c This difference demonstrates the importance of iron
coordination in stabilizing the catenated nitrogen atoms.
that assign the compound as a formal diiron(II) complex.
Figure 4. Mo¨ssbauer spectrum of LMeFe(µ-η2:η2-AdN6Ad)FeLMe. The majority
of the signal (98% of total iron) was fit with values of δ ) 0.75(1) mm/s and ∆EQ
) 3.12(2) mm/s, and the remaining impurity (2%) was fit with δ ) 0.06(4) mm/s
and ∆EQ ) 0.27(8) mm/s. The lines represent the Lorentzian doublets of the
subspectra and their superposition (red).
Acknowledgment. We thank the Petroleum Research Fund
(44942-AC to P.L.H.) and the National Science Foundation
(Graduate Research Fellowship to R.E.C. and CHE-0134658 to
P.L.H.) for funding. We thank Sebastian Stoian and Prof. Eckard
Mu¨nck for a preliminary Mo¨ssbauer spectrum.
Supporting Information Available: Synthetic, structural, and
crystallographic details. This material is available free of charge via
References
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Figure 5. Variable-temperature magnetic susceptibility of LMeFe(µ-η2:η2-
AdN6Ad)FeLMe. The simulation (solid red line) is obtained using Hexch
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2.2(1), and 3% paramagnetic impurity (S ) 5/2). The contribution from this
paramagnetic impurity is shown as a blue dashed line. The green dashed line is an
alternative fit with SFe ) 3/2 and the same parameters, showing that an iron(I)
model does not fit as well as an iron(II) model.
by tris(phosphino)borate ligands,12 and in iron-sulfur clusters.13 The
alternative high-spin iron(I) formulation cannot be excluded on the
basis of the Mo¨ssbauer measurements because low-valent iron(II) and
iron(I) sites can have similar isomer shifts,14 presumably because of
compensating effects originating from the changes in the number of
valence electrons and in back-bonding.
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Finally, the magnetic susceptibility of solid LMeFe(µ-η2:η2-
AdN6Ad)FeLMe was studied at temperatures from 2 to 290 K. Figure
5 shows that the value of µeff gradually decreases with lower
temperature to a minimum of less than 1 µB. The data were
successfully fit to a model of two exchange-coupled high-spin iron(II)
(SFe ) 2) with coupling constant J ) -21(1) cm-1 and large single-
ion zero-field splitting parameter DFe ) 24(1) cm-1 (Figure 5, red
line). The best fit for a high-spin iron(I) dimer with SFe ) 3/2 deviates
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Schu¨nemann, V.; Winkler, H. Rep. Prog. Phys. 2000, 63, 263–353.
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E.; Bominaar, E. L. J. Am. Chem. Soc. 2006, 128, 10181–10192.
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(b) Beck, J. Z. Naturforsch. B 1988, 43, 1029–1032. (c) Schmid, R.; Stra¨hle,
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(16) Extended irradiation for >24 h results in some decomposition to multiple
paramagnetic species, as judged by 1H NMR spectroscopy.
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