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solutions mixed with compounds 1 or pyridine show only
minor changes. A small shift of approximately 2 nm and
dampening of the plasmon bands implies that the stabilizing
capping layer of the AuNPs was exchanged with these ligands.
However, no coupled plasmon band is observed, thus
indicating that the AuNPs mainly exist as independent
entities for these two compounds. Interestingly, the intensity
and broadening of the coupled surface plasmon band suggest
that formation of the AuNP assemblies is related to the
number of pyridyl moieties (between one and four), where
the degree of assembly formation increases in the order:
pyridine ꢀ 1 ! 2 < 4 < 3 (Figure 2). Other structural factors
also play a dominant role in the AuNP assembly formation.
For instance, the saturated analogue of 3 (compound 5)
results in a significantly higher degree of NP assembly
formation, which is similar to that obtained with the charged
CL 6.
Figure 3. Representative TEM images of the AuNP–CL assemblies. The
labels correspond to the molecular structures shown in Scheme 1 and
the UV/Vis spectra given in Figure 1. Additional TEM images are
provided in Figure S3 in the Supporting Information.
varying dimensions. This result clearly shows that a higher
number of pyridyl units is a requirement for aggregation of
the AuNPs. TEM analyses indicate that the level of aggrega-
tion for CLs 2–4, which have a structure with between two and
four binding sites, is somewhat similar (Figure 3), although
each of these systems has unique optical properties (Figure 1).
Significantly larger and denser assemblies are observed for
CLs 5 and 6.
To provide some insight into the origins of the exper-
imental findings, density functional theory (DFT) calculations
(at the M06/SDB-pc1//M06L/SDB-pc1/DFBS level of theory,
see the Supporting Information for details) were carried out.
The organic CLs 1–5 and pyridine were coordinated to one to
four Au8 clusters, and the binding energies (BEs) were
determined (Table 1). From these DFT results, it would seem
that electronic effects are minor and the BEs for CLs 2–5 are
very similar. It is interesting to note that the BEs decrease for
each additional gold cluster coordinated to the CL. Coordi-
nation of the fourth gold cluster to CL 4 is slightly
unfavorable. The small size of the gold cluster, which is
essential to make the calculations feasible, precludes steric
interactions in the AuNP–CL structures but, nonetheless,
should reproduce trends in the electronic nature of the Au–
CL binding. If one were to consider the geometric limitations
of this system, it is clear that none of CLs considered are large
enough for them to bind to more than two NPs simulta-
neously. (A full analysis is provided in the Supporting
Figure 2. Comparison of the UV/Vis spectra of the hybrid AuNP–CL-
based assemblies in aqueous solutions with a concentration of
compounds 1–6 of 1.5 mm. Spectra were recorded immediately after
mixing the components.
Compound 6 differs from the other cross-linkers in that it
has a + 2 charge. It is known that the use of charged species as
cross-linkers results in NP assemblies formed by Coulombic
interactions.[9] When CL 6 was added to the AuNP solutions,
extensive assemblies were formed. Similar results were
obtained with [Os(bpy)3]2+ (bpy = 4,4’-bipyridyl) complexes
that bear zero or one pendant pyridyl arms (Scheme S1 in the
Supporting Information), thus indicating that NP–pyridyl
coordination is, in this case, not a requirement for NP
assembly formation. Thus, in these charged systems, the level
of control that the CL structure has over the formation and
optical properties of the NP assembly seems minimal.
Table 1: DFT binding energies (BE) of 1–4 Au8 clusters bound to CLs 1–
5.[a]
The TEM images (Figure 3 and Figure S3 in the Support-
ing Information) show increasing AuNP aggregation as a
function of the number of pyridyl units and/or the molecular
geometry, which is in good agreement with the UV/Vis
analysis (see above). Solvent-free conditions were used for
these measurements and, therefore, only the qualitative
structures of the AuNP assemblies in solution are reflected
in these images. Systems formed with CL 1 or pyridine
showed isolated spheres and small aggregates on the grid,
whereas the other systems (2–6) form larger assemblies of
CL
BE per Au8
BE(1)[b]
BE(2)[b]
BE(3)[b]
BE(4)[b]
1
2
3
4
5
À22.4
À21.6
À20.5
À20.2
À20.9
À22.4
À22.0
À21.1
À21.2
À21.8
À21.1
À20.7
À20.9
À21.0
À19.7
À19.7
À19.9
1.0
[a] Binding energies reported in kcalmolÀ1. [b] Binding energy of the first,
second, third, and fourth cluster to the CL.
1220
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2010, 49, 1218 –1221