Many useful principles of self-assembly have been elucidated through studies of systems where multiple components combine to create a single structure. More complex systems, where multiple product structures self-assemble in parallel from a shared set of precursors, are also of great interest, as biological systems exhibit this behavior. The greater complexity of such systems leads to an increased likelihood that discrete species will not be formed, however. Here we show how the kinetics of self-assembly govern the formation of multiple metal-organic architectures from a mixture of five building blocks, preventing the formation of a discrete structure of intermediate size. By varying ligand symmetry, denticity, and orientation, we explore how five distinct polyhedra-a tetrahedron, an octahedron, a cube, a cuboctahedron, and a triangular prism-assemble in concert around CoII template ions. The underlying rules dictating the organization of assemblies into specific shapes are deciphered, explaining the formation of only three discrete entities when five could form in principle.
Many useful principles of self-assembly have been elucidated through studies of systems where multiple components combine to create a single structure. More complex systems, where multiple product structures self-assemble in parallel from a shared set of precursors, are also of great interest, as biological systems exhibit this behavior. The greater complexity of such systems leads to an increased likelihood that discrete species will not be formed, however. Here we show how the kinetics of self-assembly govern the formation of multiple metal-organic architectures from a mixture of five building blocks, preventing the formation of a discrete structure of intermediate size. By varying ligand symmetry, denticity, and orientation, we explore how five distinct polyhedra-a tetrahedron, an octahedron, a cube, a cuboctahedron, and a triangular prism-assemble in concert around CoII template ions. The underlying rules dictating the organization of assemblies into specific shapes are deciphered, explaining the formation of only three discrete entities when five could form in principle.
Molecules may follow complex
pathways during self-assembly processes that generate multiple products.
Understanding the self-sorting processes that occur within these pathways
may allow us to decipher how simple prebiotic chemicals developed
into life,[1−3] and also how to design synthetic chemical systems
that may be of practical use.[4−14]When different molecules self-assemble,
one
of three outcomes may result: social sorting,[15,16] where a statistical distribution of products is observed, narcissistic sorting,[17−19] where components self-recognize
and generate homoleptic architectures, or integrative self-sorting,[20−24] during which all components are assimilated into a single product.
Other sorting modes have recently been discovered, including biased
sorting regimes[25] and those driven by kinetic
trapping,[26] stereochemical differences,[27,28] or template-induced sorting.[29]Metal–organic cages have displayed a wealth of sorting behaviors
that can be understood in terms of thermodynamic and geometric parameters.[30−35] We hypothesized that combinations of ligands with different denticities
and symmetries would yield complex, but potentially predictable sorting
behavior. We thus explored the sorting characteristics of three- and
fourfold symmetric polyamine subcomponents with bidentate and tridentate
aldehyde subcomponents, using CoII as the metal ion template
during subcomponent self-assembly.Four polyhedral coordination
cages were prepared using CoII as a template ion, as shown
in Figure , and as
described in Supporting Information (SI) Section 2. Tritopic A and tetratopic B thus
generated threefold and fourfold
symmetry axes, respectively, and 2-formylpyridine P1 and
2-formylphenanthroline P2 created bidentate and tridentate
coordination sites upon condensation with these two polyamines, allowing
the CoII centers to serve as three- or twofold symmetry
axes. The relative orientations of these ligand- and metal-generated
symmetry elements thus brought about the geometries of CoII4L4 tetrahedron 1, CoII6L4 octahedron 2, CoII8L6 cube 3, and CoII12L6 cuboctahedron 4.[25,29,36,37]
Figure 1
Four
different architectures can be synthesized by CoII-templated
imine condensation of amine A or B with
aldehyde P1 or P2. (a) Threefold
symmetric subcomponent A generated (i) CoII4L4 tetrahedron 1 and (ii) CoII6L4 octahedron 2. (b)
Fourfold symmetric subcomponent B generated (iii) CoII8L6 cube 3 and (iv) CoII12L6 cuboctahedron 4.
Lines connect nearest-neighbor metal ions.
Four
different architectures can be synthesized by CoII-templated
imine condensation of amine A or B with
aldehyde P1 or P2. (a) Threefold
symmetric subcomponent A generated (i) CoII4L4 tetrahedron 1 and (ii) CoII6L4 octahedron 2. (b)
Fourfold symmetric subcomponent B generated (iii) CoII8L6 cube 3 and (iv) CoII12L6 cuboctahedron 4.
Lines connect nearest-neighbor metal ions.When two different polyamines self-assemble with a single aldehyde,
possible outcomes include narcissistic and integrative self-sorting.
When tetratopic and tritopic amines B and C reacted with aldehyde P1 and CoII (Figure a), both narcissistic
and integrative processes were observed to occur in parallel. The
narcissistically sorted cube 3 and tetrahedron 5 were thus observed to form in equilibrium with the integrative
product 6, a heteroleptic trigonal prism containing two
residues of C and three of B (SI Section 3.3.2). The structure of 6 (Figure b) is similar
to that of a reported analog,[21] although
the free base porphyrin faces of 6 do not adapt the inward-
and outward-facing conformations observed for their NiII-centered congeners.[21]
Figure 2
(a) Subcomponents B and C underwent both
narcissistic self-sorting to produce a mixture of cube 3 (from B) and tetrahedron 5 (from C), and integrative self-assembly to produce trigonal prism 6, which incorporates both B and C. Product ratios were determined to be 23% cube 3, 51%
triangular prism 6, and 26% tetrahedron 5 by 1H NMR integration. (b) X-ray crystal structure of 6, viewed facing the tritopic (top) and tetratopic (bottom)
ligands. The void space inside the structure is displayed as a gray solid (Co, orange; C, gray; N,
blue; H, white).
(a) Subcomponents B and C underwent both
narcissistic self-sorting to produce a mixture of cube 3 (from B) and tetrahedron 5 (from C), and integrative self-assembly to produce trigonal prism 6, which incorporates both B and C. Product ratios were determined to be 23% cube 3, 51%
triangular prism 6, and 26% tetrahedron 5 by 1H NMR integration. (b) X-ray crystal structure of 6, viewed facing the tritopic (top) and tetratopic (bottom)
ligands. The void space inside the structure is displayed as a gray solid (Co, orange; C, gray; N,
blue; H, white).When both aldehydes P1 and P2 reacted
with CoII and either amine A or B, clean narcissistic self-sorting was observed (Figure a, SI Sections 3.1 and 3.2). Tritopic A produced 1 and 2, and tetratopic B produced 3 and 4, with product ratios depending on the
amounts of P1 and P2 used initially.[38]
Figure 3
(a) Narcissistic self-sorting was observed when the two
aldehyde
subcomponents P1 and P2 were both employed
with either (i) A or (ii) B during self-assembly.
(b) More complex outcomes resulted from the self-assembly of both
amines A and B with either or both of the
aldehydes. (iii) A, B, and P1 combined to form homoleptic 1 and 3 and
heteroleptic 7. (iv) A, B,
and P2 yielded no discrete products, and (v) A, B, P1, and P2 gave 1, 3, and 4.
(a) Narcissistic self-sorting was observed when the two
aldehyde
subcomponents P1 and P2 were both employed
with either (i) A or (ii) B during self-assembly.
(b) More complex outcomes resulted from the self-assembly of both
amines A and B with either or both of the
aldehydes. (iii) A, B, and P1 combined to form homoleptic 1 and 3 and
heteroleptic 7. (iv) A, B,
and P2 yielded no discrete products, and (v) A, B, P1, and P2 gave 1, 3, and 4.Different behavior was observed when only one of the aldehyde subcomponents P1 or P2 reacted with both amine subcomponents A and B and CoII (Figure b). When triamine A and tetramine B were combined with 2-formylpyridine P1 in a 1:1 mixture of DMF/MeCN, only tetrahedron 1 and cube 3 were observed (Figures S14, S15). However, when pure MeCN was used as the reaction
solvent, a third product 7 was also observed by ESI-MS
(Figure S17). Product 7 incorporates
three residues of B and two of A, and we
infer it to have a similar trigonal-prismatic framework to structurally
characterized 6 (Figure b).The combination of amines A and B with
2-formylphenanthroline P2 (Figure b, pathway (iv)) resulted in a mixture of
products that gave a complex NMR spectrum (Figure S21) that did not display peaks corresponding to any isolated
discrete product. Multiple different products may thus form, integrating
both A and B, without a strong thermodynamic
preference for any single outcome. The lack of narcissistic sorting
of octahedron 2 and cuboctahedron 4 may
also contribute to the lack of observation of the former species in
the five-component sorting experiment described below.When
all five building blocks (A, B,
CoII, P1, and P2) were combined
in the correct ratio so as to allow an equimolar mixture of cages 1:2:3:4 to form, octahedron 2 was not observed to form (Figure b, pathway (v)). Instead, tetrahedron 1, cube 3, and cuboctahedron 4 were
the only species observed by both 1H NMR (Figure ) and ESI-MS (Figure S24). Monitored over 3 days of heating, 2 was not observed to form at any time (Figure S25).
Figure 4
1H NMR spectra (400 MHz, 298 K, CD3CN) of
each separate cage (bottom four spectra) compared to the mixture generated
(Figure b, pathway
(v)) when A, B, P1, and P2 were mixed with CoII (topmost spectrum).
1H NMR spectra (400 MHz, 298 K, CD3CN) of
each separate cage (bottom four spectra) compared to the mixture generated
(Figure b, pathway
(v)) when A, B, P1, and P2 were mixed with CoII (topmost spectrum).In contrast with reported systems,[38,39] the mixtures
of products obtained in the system of Figure b, pathway (v) is not determined uniquely
by the stoichiometry of subcomponents employed.[38] A subset of only two or three of the four cages (1, 2, 3, 4) will be
able to consume all of a balanced set of building blocks, i.e., where
the total number of aldehyde groups is equal to the total number of
amine groups, and where all CoII is coordinatively saturated.
Thus, the selectivity observed when all subcomponents are present
together (Figure b,
pathway (v)) must be a result of further factors acting upon the system.The rates of formation of the four cages were gauged, as shown
in Figure . At regular
intervals during self-assembly at 60 °C, we extracted aliquots
and measured the degree of completion of assembly by UV–vis
spectroscopy (SI Section 4). For all cages,
we monitored the evolution of MLCT transitions (which often overlapped
with ligand π → π* transitions, and porphyrin Soret
bands in the cases of 3 and 4) as a function
of time. A plateau in the intensity of the absorbance marked complete
formation of the cage, which was then verified by 1H NMR
spectroscopy. As the assembly kinetics of these structures are complex,
we fitted our data to a simple exponential rate equation, enabling
a comparison of assembly half-lives between cages.
Figure 5
Plots showing the rate
of formation of each homoleptic architecture,
monitored by UV–vis spectroscopy, following the principal optical
bands of 1 (346 nm) and 2 (370 nm), and
the MLCT transitions of 3 (430 nm) and 4 (445 nm), which overlapped with porphyrin Soret bands. Black lines
represent the best fits to an exponential rate equation (Absorbance
= A0 + Aeλt), from which t1/2 = ln 2/λ.
Plots showing the rate
of formation of each homoleptic architecture,
monitored by UV–vis spectroscopy, following the principal optical
bands of 1 (346 nm) and 2 (370 nm), and
the MLCT transitions of 3 (430 nm) and 4 (445 nm), which overlapped with porphyrin Soret bands. Black lines
represent the best fits to an exponential rate equation (Absorbance
= A0 + Aeλt), from which t1/2 = ln 2/λ.The data of Figure show clear differences between the rates of formation of the four
structures. Tetrahedron 1 forms most rapidly, followed
by octahedron 2, cube 3, and cuboctahedron 4. This sequence reflects the increasing structural complexity
of these assemblies.These rate differences (Figure ) shed light upon the selectivity
exhibited by the
system of Figure b,
pathway (v), as shown in Figure . As tetrahedron 1 forms most rapidly,
it consumes all of the A and most of the P1 from the initial mixture. The remaining P1 must react
with B to form cube 3, leaving additional B to react with the P2 to form cuboctahedron 4. Structures 3 and 4 may form in
either order, as the system becomes deterministic[38] following the conversion of all A into 1, with only one fate possible for each of the remaining subcomponents.
The relative rates of 3 and 4 formation
(Figure ) suggest
that 3 will be formed ahead of 4, however.
Figure 6
An outline
of the process inferred to occur when A, B, P1, P2, and CoII are mixed
in the proportions shown. (a) Tetrahedron 1 forms first,
sequestering all A. (b) Cuboctahedron 4 may
then form, consuming all P2, followed by
(c) cube 3, or else (d) cube 3 may form
first, consuming all P1, followed by cuboctahedron 4. Both paths lead to an identical final state in which only 1, 3, and 4 are observed.
An outline
of the process inferred to occur when A, B, P1, P2, and CoII are mixed
in the proportions shown. (a) Tetrahedron 1 forms first,
sequestering all A. (b) Cuboctahedron 4 may
then form, consuming all P2, followed by
(c) cube 3, or else (d) cube 3 may form
first, consuming all P1, followed by cuboctahedron 4. Both paths lead to an identical final state in which only 1, 3, and 4 are observed.The first structure to form, tetrahedron 1, thus sets
the scene for the system’s subsequent self-assembly by preferentially
consuming all of A that octahedron 2 would
have otherwise required. This system appears quite sensitive to subtle
effects, given the relatively small (less than a factor of 2) difference
between the formation times of the competing structures 1 and 2. Notably, 2 was never observed when
different reactant stoichiometries were employed during the reaction
described in Figure b, pathway (v) (Figures S26–28).Host–guest binding can influence the kinetics of cage formation.[40,41] This study thus lays the foundations to direct the self-assembly
of systems of cages that share building blocks through the addition
of guests, and other “cofactors” whose influence on
one component of the system may propagate through its entirety, amplifying
certain structures and suppressing others. In systems where cages
are serving useful functions, such as catalysis[42,43] or cargo transport,[44,45] such an understanding may allow
the development of these functions to be programmed in a complex way
from a simple set of input stimuli.
Authors: Alan Ferguson; Robert W Staniland; Christopher M Fitchett; Marie A Squire; Bryce E Williamson; Paul E Kruger Journal: Dalton Trans Date: 2014-10-21 Impact factor: 4.390
Authors: Philippe Wagner; Frank Rominger; Wen-Shan Zhang; Jürgen H Gross; Sven M Elbert; Rasmus R Schröder; Michael Mastalerz Journal: Angew Chem Int Ed Engl Date: 2021-03-08 Impact factor: 15.336