with an acetate counterion, and is established owing to the
6s2 stereochemically active lone pair that favorably orients the
bound anion. The out-of-plane, outside-the-strap geometry,
binding of Pb2 should favour the inward orientation of the
HAT Pb(II), of which the 6s2 lone pair can ‘accommodate’ in
the dome-shaped porphyrin core. This coordination mode is
responsible for a unique translocation-coupled transmetalation
process, in which a lead cation bound to the N-core can be
formally switched from an inside to an outside position, or in
other words, can be stereoselectively incorporated in the
strapped macrocycle, in a dynamic way. The hanging carboxylic
acid approach provides a new opportunity to further extend the
frontiers of porphyrin-like coordination chemistry.
Fig. 3 (a) DFT-optimized structure of 1PbÁPbOAc (hydrogen atoms
removed) and deformation electron-density isosurface for the coordi-
nation sphere of Pb1 (contour value: +0.008 e bohrÀ3). (b) Structural
type observed for 1PbÁPbOAc (second coordination sphere omitted).
Notes and references
inward orientation of Pb1 in solution as in the crystal structure.
Density functional calculations (DFT) were performed to
probe the role of the lone pair of the lead cations in this new
HAT binding mode. Calculations were carried out at the
B88P86/LANL2DZ12,13 level of theory using Gaussian09.14
A full in vacuo geometry optimization of 1PbÁPbOAc was first
performed starting from the X-ray structure. The computed
geometry does not show significant modifications of the
complex (Fig. 3a). The lone pair of each lead cation was
indirectly localized using the deformation electron-density
map.15 In a hemidirected coordination geometry, the observed
residual electron density in the vicinity of a lead atom is
attributed to a trans deformation of the lone pair orbital
relative to the proximal ligands.16 Logically, the lone pair of
Pb1 and Pb2 points towards and away from the N-core of the
macrocycle, respectively (Fig. 3a, ESIw). Because of a quasi-
symmetrical N4 environment, the lone pair of Pb2 keeps an
axial symmetry whereas that of Pb1 appears distorted and
slightly directed towards the N2 atom, but without effect on
Pb1–N2 length. Therefore, there is evidence neither for a
specific interaction between the lone pair of Pb1 and the
N-core of the macrocycle, nor for any repulsion, and a faithful
structural type for 1PbÁPbOAc can be drawn as in Fig. 3b. The
role of the counteranion was also investigated by DFT. First,
the H-bonding interaction between the AcOÀ and the NHCO
was evaluated to be B10 kcal molÀ1. Second, the bound AcOÀ
was replaced by a nitrate and DFT calculations of the complex
1PbÁPbNO3 did not evidence significant differences with
1PbÁPbOAc, the bound nitrate being at a distance of the strap
compatible with H-bonding interaction with the NHCO
(ESIw).17 In contrast, in the optimized structure of a hypo-
thetical complex 1PbÁPbCl, the chloride anion is standing B6 A
away from the NHCO of the strap and does not exhibit any
intramolecular stabilizing interactions. Therefore, this second
sphere of coordination defined by the intramolecular H-bond
with the strap could be stronger with the AcOÀ, if not specific,
and explains why the formation of a dinuclear complex relies
on the presence of this counterion.
1 (a) I. Beletskaya, V. S. Tyurin, A. Y. Tsivadze, R. Guilard and
C. Stern, Chem. Rev., 2009, 109, 1659; (b) J. K. Sanders, Coordination
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2 References for metal ion translocation with synthetic receptors:
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S. Patroni, P. Pallavicini and A. Taglietti, Angew. Chem., Int.
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O. Reinaud, J. Am. Chem. Soc., 2010, 132, 4393.
3 C. M. Lemon, P. J. Brothers and B. Boitrel, Dalton Trans., 2011,
40, 6591.
4 (a) K. M. Barkigia, J. Fajer, A. Adler and G. J. B. Williams, Inorg.
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B. Boitrel, Dalton Trans., 2007, 3684; (d) Z. Halime, M. Lachkar,
T. Roisnel, P. Richard and B. Boitrel, Inorg. Chem., 2007, 46, 6338.
5 Z. Halime, M. Lachkar, T. Roisnel, E. Furet, J.-F. Halet and
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7 1M (1M) refers to a metal ion coordinated in an inside (outside)
position relative to the strap.
8 HRMS (ESI-TOF) measurements: at a 1 : 1 1/Pb(OAc)2 ratio (negative
ion mode), m/z calcd for C66H49N6O8Pb: 1261.3384 [1-3H+Pb]À;
found: 1261.3389. At a 1 : 3 1/Pb(OAc)2 ratio (positive ion mode),
m/z calcd for C66H49N6O8Pb2: 1469.3143 [1-3H+2Pb]+; found:
1469.3149 (AcOÀ is loss in the ionisation process).
9 (a) C. Jr. Grant and P. Hambright, J. Am. Chem. Soc., 1969,
91, 4195; (b) M. Tabata, W. Miyata and N. Nahar, Inorg. Chem.,
1995, 34, 6492.
10 P. Hambright and P. B. Chock, J. Am. Chem. Soc., 1974, 96, 3123.
11 S. Le Gac, B. Najjari, N. Motreff, P. Remaud-Le Saec, A. Faivre-
Chauvet, M.-T. Dimanche-Boitrel, A. Morgenstern, F. Bruchertseifer,
M. Lachkar and B. Boitrel, Chem. Commun., 2011, 47, 8554.
12 (a) A. D. Becke, Phys. Rev. A, 1988, 38, 3098; (b) J. P. Perdew,
Phys. Rev. B: Condens. Matter Mater. Phys., 1986, 33, 8822.
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14 M. J. Frisch, et al., Gaussian 09, revision A.02, Gaussian Inc.,
Wallingford, CT, 2009.
15 Deformation electron-density isosurfaces were obtained by subtracting
from the molecular density of 1PbÁPbOAc, the self-consistent com-
puted densities of the [Pb]2+ and [1Pb+DMSO+AcO]2À (for Pb2) or
[1+DMSO+PbOAc]2À (for Pb1) units, kept with their respective
geometries in the dinuclear complex optimized with Gaussian 09 (ESIw).
16 L. Shimoni-Livny, J. P. Glusker and C. W. Bock, Inorg. Chem.,
1998, 37, 1853.
In summary, we have described a new hanging-atop (HAT)
coordination mode in a dinuclear lead complex with an over-
hanging carboxylic acid porphyrin. The HAT lead cation does
not interact with the N-core but adopts an inward geometry
stabilized through a second sphere of coordination with the strap.
This intramolecular secondary interaction is best achieved
17 The minor species observed with 1Pb in the NMR titration with
Pb(NO3)2 could therefore correspond to a dinuclear species.
c
3726 Chem. Commun., 2012, 48, 3724–3726
This journal is The Royal Society of Chemistry 2012