Angewandte
Chemie
DOI: 10.1002/anie.201002295
Nanotechnology
Nanoparticle Supracrystals and Layered Supracrystals as Chemical
Amplifiers**
Bartlomiej Kowalczyk, David A. Walker, Siowling Soh, and Bartosz A. Grzybowski*
One of the main applications of metal nanoparticles (NPs) is
in the detection of biologically important[1] or toxic substan-
ces,[2] usually by the spectral or surface plasmon resonance
(SPR) changes[3] accompanying particle aggregation[4] or
dispersion[2c,5] in the presence of an analyte. With the
exception of highly sensitive DNA-based methods,[6] how-
ever, most reported colorimetric detection schemes require
large excesses of analyte molecules per one NP (on the order
of one thousand,[2c,5] see the Supporting Information, Sec-
tion 1) to affect even small shifts in the nanoparticlesꢀ SPR
bands.[7] Improving the existing detection limits therefore
requires amplification of the assembly/disassembly process.
Unfortunately, the repertoire of amplification procedures
compatible with nanoparticle-based assays is currently lim-
ited to the catalytic deposition of silver on surface-immobi-
lized AuNPs.[8] Herein, we show that NP supracrystals and
previously unreported core–shell (CS) supracrystals
(Figure 1) stabilized by analyte-specific cross-linkers can
enhance dramatically (by over two orders of magnitude
compared to noncrystalline NP aggregates) the sensitivity of
NP-based detection. The cross-linked crystals are insoluble in
water and, owing to NP aggregation, do not exhibit SPR in the
visible regime. When, however, an analyte (an anion, a small
molecule, or an enzyme) is present, it cuts the cross-linkers so
that each crystal liberates, like a pinched “balloon” (Figure 2,
Figure 3), millions of individual NPs absorbing strongly in the
visible regime and effectively amplifying the molecular-scale
“cutting” events into pronounced color changes visible to a
naked eye (Figure 4). Moreover, in the CS supracrystals, the
“shell” and the “core” regions have different NP composi-
tions and are stabilized with different cross-linkers; conse-
quently, these crystals can dissolve in a step-wise fashion
under the action of two different analytes (Figure 5). This
property allows for spatially distributed sensing, whereby the
crystals release their cargo only if they travel through specific
concentration landscapes of the analytes.
We used AuNPs with an approximate diameter of (5.6 Æ
0.5) nm and AgNPs of diameter (5.6 Æ 1.2) nm coated with
self-assembled monolayers (SAMs) of either positively
charged N,N,N-trimethyl(11-mercaptoundecyl)ammonium
+
chloride (HS(CH2)11N(CH3)3 , TMA, ProChimia, Poland)
or negatively charged, deprotonated mercaptoundecanoic
acid (HS(CH2)10COOÀ, MUA, ProChimia; Figure 1a). The
AuNPs had a strong surface plasmon resonance (SPR) band
with maximum at lmax = 520 nm, and their aqueous solutions
appeared bright red; for AgNPs, lmax ꢀ 420 nm and particle
solutions appeared yellow. Supracrystals (henceforth, simply
“crystals”) were grown by slow evaporation of water from
DMSO/water mixtures containing equal numbers of oppo-
sitely charged NPs (see Ref. [9] and the Supporting Informa-
tion, Section 2 for details). The 1–2 mm crystals (Figure 1b)
thus assembled (ca. 2.2 ꢁ 107 crystals per mL) were held
together by electrostatic interactions between the NPs,
comprised several million nanoparticles each (ca. 2.5 ꢁ 106
NPs as determined by SEM imaging), and were soluble in
water. Upon exposure to alkane dithiols that cross-linked the
nearby NPs, however, the crystals became stable in water
(Figure 2a) and could be used as seeds or cores to epitaxially
deposit an additional shell of NPs. These shell NPs were again
deposited from an aqueous solution of oppositely charged
particles,[10] the material properties of which could be differ-
ent from those in the crystal core. In this way, core–shell
crystals (each up to ca. 2.5 mm across, Figure 1c, shell
thickness ca. 200–300 nm, Figure 5) were assembled and
could be stabilized and made insoluble in water by additional
dithiol cross-links. The presence of the core–shell architecture
was confirmed directly by EDX (energy dispersive X-ray
spectroscopy) scans of the crystalsꢀ composition (Figure 1c
and Figure 5) and indirectly by the fact that the shell regions
could be dissolved without destroying the crystalline core (see
Figure 5). Both the “regular” and the CS crystals slowly
(within hours) sedimented from solution and appeared as a
dark gray powder.
[*] Dr. B. Kowalczyk, D. A. Walker, S. Soh, Prof. B. A. Grzybowski
Department of Chemical and Biological Engineering
Northwestern University
2145 Sheridan Rd., Evanston, IL 60208 (USA)
Fax: (+1)847-491-3728
E-mail: grzybor@northwestern.edu
The crux of the amplified detection (Figure 2a) was to
prepare crystals stabilized by dithiols incorporating groups
that can be cleaved by desired analytes. We considered three
such dithiols (Figure 2b; see the Supporting Information,
Section 2 for synthetic details): 11-mercaptoundecyl-11-mer-
captoundecanoate (1) containing an ester moiety prone to
base hydrolysis; 11-mercapto-N-(pyridin-2-yl)undecanamide
held together by coordination of CuII to two pyridine and two
carbonyl groups (2), which cleaves upon addition of a stronger
chelating agent such as ethylenediaminetetraacetic acid
(EDTA), and N-(6-amino-1-(11-mercaptoundecylamino)-1-
Dr. B. Kowalczyk, Prof. B. A. Grzybowski
Department of Chemistry, Northwestern University
2145 Sheridan Rd., Evanston, IL 60208 (USA)
[**] This work was supported by the Non-equilibrium Energy Research
Center (NERC), which is an Energy Frontier Research Center funded
by the U.S. Department of Energy, Office of Science, Office of Basic
Energy Sciences under Award Number DE-SC0000989.
Supporting information for this article is available on the WWW
Angew. Chem. Int. Ed. 2010, 49, 5737 –5741
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
5737