ChemComm
Communication
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to low-spin species. Meanwhile, chloride is a weak field ligand
and often leads to high spin Fe2+ complexes. Since the Fe2+ ion in
1ÁFeCl2 is in a tetrahedral coordination environment, thermally
accessible spin crossover would require that the ligand field
imparted by 1 and two ClÀ anions be significantly stronger
than what the combination of bipyridyl and chloride typically
generate in hexacoordinate complexes. This ligand field argument
is consistent with the data shown in Fig. 3.
´
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Another consideration is structural rigidity. The one tetra-
hedral Fe2+ species which undergoes spin crossover,
[PhB(MesIm)3Fe-NdPPh3], has a more flexible ligand set imparted
by a tris(carbene)borate and axial phosphoraniaminato ligands.30
These moieties allow for the proper ligand distortions necessary
to observe spin state changes. For 1ÁFeCl2, we postulate these
distortions are not favored due to the rigidity of the bipyridyl and
the intramolecular hydrogen-bonding network. Thus, the complex
remains trapped in the high-spin state even though the Fe–N
bond lengths suggest that the low-spin state should be accessible.
In conclusion, we have demonstrated that a bipyridyl bisurea-
based receptor designed to ditopically coordinate protic anions
provides a suitable framework as a ligand toward metal halide
salts. Solid state investigation of the Fe2+ complex reveals the
presence of intramolecular hydrogen bonds between 1 and the
metal-coordinated halide ligands. These findings demonstrate
the potential of this and related systems31–35 to affect coordinated
metal centres through non-covalent interactions. Additionally, the
helical nature of the formed ligand complex presented offers a
potential avenue for incorporating enantiospecific recognition
into future generations of ligand design.
13 T. S. Franczyk, K. R. Czerwinski and K. N. Raymond, J. Am. Chem.
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14 Crystallographic data for 1ÁFeCl2 (CCDC 978233): C48H42Cl2FeN8O6,
M = 953.65, 0.12 Â 0.07 Â 0.05 mm, T = 173(2) K, triclinic, space
%
group P1, a = 11.666(9) Å, b = 11.764(9) Å, c = 18.282(14) Å, a =
78.585(16)1, b = 88.896(19)1, g = 63.247(16)1, V = 2189(3) Å3, Z = 2,
Dc = 1.447 Mg mÀ3, m = 0.528 mmÀ1, F(000) = 988, 2ymax = 50.001,
17 504 reflections, 7664 independent reflections [Rint = 0.0971],
R1 = 0.0838, wR2 = 0.1879 and GOF = 1.006 for 7664 reflections
(586 parameters) with I 4 2s(I), R1 = 0.1693, wR2 = 0.2368 and
GOF = 1.006 for all reflections, max/min residual electron density
+1.126/À0.610 e Å3.
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This work was supported by NIH grant R01-GM087398, which
also funded early stage intellectual property that was licensed by
SupraSensor Technologies, a company co-founded by D.W.J and
M.M.H. M.P.S. and C.M.K. thank the NSF (CHE-1058889) and
Colorado State University for support of this work.
26 D. F. Evans, J. Chem. Soc., 1959, 2003–2005.
27 E. M. Schubert, J. Chem. Educ., 1992, 69, 62.
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