Communications
optimal docking of the reactants with the template, template
duplexes are conformationallyrestricted in their finding of an
optimal orientation of the recognition units. A similar ration-
ale was reported to explain the nearlyexponential growth of a
peptide replicator.[14] Our replicator theorypredicts that for
systems with a negligible background channel, the question of
parabolic versus exponential growth is solelyanswerable by
the stabilities of the ground-state and not the transition-state
complexes involved.[2] Further cases are needed to prove that
exponential growth can be literallydesigned bytaking into
account the conformational control of ground states. If this
recipe can be generalized, it could open a door to a field that
may be termed “systems chemistry”, namely, the design of
prespecified dynamic behavior.
Received: May4, 2005
Revised: July5, 2005
Published online: September 27, 2005
Keywords: chirality · computer chemistry · molecular modeling ·
.
supramolecular chemistry · template synthesis
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ski, Angew. Chem. 1998, 110, 489 – 492; Angew. Chem. Int. Ed.
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Figure 8. Energy profiles correlated to the corresponding structures
(B3LYP/6-31G*) of the reaction of 4 and 5a through the a) autocata-
lytic and b) nontemplate-directed pathways.
[11] Crystallographic data for rac-6b: crystal size = 0.2 0.2
0.3 mm3; crystal system = monoclinic; space group = P21/n;
unit cell dimensions: a = 5.8973(17), b = 26.318(8), c =
V= 2929.1(15) 3;
1calcd =
ature dependence of rates and equilibria in a slightlymodified
self-replicating system has revealed evidence that the above
enthalpic preference is not overcompensated bythe respec-
18.881(5) ,
b = 91.693(6)8;
2qmax = 458; lMoKa = 0.71073 ; T= 213(2) K;
0.931 gcmÀ3
;
reflections collected = 10714, unique reflections = 3803, for
2983 reflections observed (I > 2s(I)); The structure was solved
bydirect methods and refined byfull-matrix least squares by
using SHELXTL-97; 271 parameters; the non-H atoms were
refined anisotropically, H atoms were included but not refined;
final R indices: R1 = 0.0670, wR2 = 0.1893; R indices (all data):
R1 = 0.0785, wR2 = 0.1998; goodness-of-fit on j F2 j = 1.079; max-
[13]
tive entropydifferences.
In summary, our re-evaluation of the Wang–Sutherland
replicator with simplified variants reveals that the exponen-
tial dynamics arise from conformational constraints. Whereas
the termolecular complexes offer enough freedom for an
6754
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Angew. Chem. Int. Ed. 2005, 44, 6750 –6755