meso–meso-Linked ZnII Diporphyrins
COMMUNICATION
A, B, and C, but the aggregates
A and B are thermally more
labile and tend to be fragment-
ed, contributing to the accumu-
lation of C. As a consequence,
one-way atropisomerism to
3inÀin is entropically driven.
Note that the heating of 3outÀout
,
3
inÀout, and 3inÀin in pyridine at
808C for 5 h led to the nonse-
lective statistical population of
3
outÀout, 3inÀout, and 3inÀin in a
1:2:1 ratio. These results indi-
cate a relatively low rotational
barrier for a meso-butoxy-3-pyr-
idyl substituent in nonaggregat-
ed dimers, whereas such barri-
Figure 4. a) Analytical GPC-HPLC chromatograms (eluent: CHCl3; c=the pristine mixture of 3; g=2; ers become higher in the aggre-
gates.[13] More importantly, the
one-way atropisomerism to
c=A, B, and, C. The band intensities of A, B, and C were adjusted to simulate the pristine mixture).
b) Thermal conversion of the pristine mixture to C in toluene at 1108C for 24 h.
1
tively simple and sharp H NMR spectrum in which the sig-
nals due to the Ha, Hb, and Hc protons are observed at 1.93,
3.14, and 5.53 ppm, respectively, indicating the coordination
of pyridyl groups to zinc ions.
The aggregates A, B, and C are considered to be all race-
mic. Although the optical resolutions of A and B were un-
successful, C was actually separated through a chiral HPLC
column (SUMICHIRAL OA-3100) into two fractions C1
and C2 in the order of elution. These two fractions are
mirror images of each other in the circular dichromism
(CD) spectra (see Figure S12 in the Supporting Informa-
tion). The structure of C1 was determined by single-crystal
X-ray diffraction analysis (Figure 5),[6b] indicating that C
consists of two molecules of 3inÀin that are complementarily
coordinated in a face-to-face fashion. The meso-substituted
pyridine rings are inclined by 17.88 towards the coordinating
direction, the central zinc atoms are displaced by 0.4 ꢀ from
the porphyrin mean plane, the dihedral angle of the meso–
meso-linked diporphyrin is 83.48, and the interplanar dis-
tance of the two porphyrin planes is 4.8 ꢀ. This X-ray struc-
ture revealed that C1 consists of two R isomers.
Figure 5. X-ray crystal structure of C1. The meso-aryl groups and hydro-
gen atoms are omitted for clarity. The thermal ellipsoids were at the
50% probability level.
The aggregates, A, B, and C were stable at room tempera-
ture, but upon heating at 1108C in toluene, the large aggre-
gates A and B were converted into the small aggregate C as
monitored by analytical GPC–HPLC (Figure 4 b) and
1H NMR spectroscopic measurements (see the Supporting
Information), whereas C was quite stable under the heating
conditions.[12] This thermal conversion to C can be rational-
ized in terms of the entropy increase associated with the
fragmentary reconstitution of the larger aggregates A and B
to the small one C. Considering the dynamic supramolecular
nature of these aggregates, the most probable mechanism is
the dissociation of the aggregates to the respective mono-
mers and subsequent random atropisomerization to give
3inÀin has been achieved only through thermal fragmentary
reconstitutions of A and B to C. Another requirement for
this process is that the aggregate C is thermodynamically
more stable than its fragments at 1108C. Finally, the synthet-
ic merit of this process has been shown by isolation of 3inÀin
in more than 90% yield after full one-way atropisomerism.
In summary, meso-(4-butoxypyrid-3-yl)-substituted ZnII
porphyrins quantitatively assemble to form a discrete hex-
americ macroring and the meso–meso-linked ZnII diporphyr-
ins undergo self-sorting self-assembly to form the respective
discrete aggregates dictated by the orientation of meso-
pyrid-3-yl substituents with respect to meso–meso connec-
3
outÀout, 3inÀout, and 3inÀin, which all form respective aggregates
Chem. Eur. J. 2009, 15, 9681 – 9684
ꢁ 2009 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
9683