Nanoparticle Supracrystals and Layered Supracrystals as Chemical Amplifiers
Nanoparticle Supracrystals and Layered Supracrystals as Chemical Amplifiers
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DOI:
10.1002/anie.201002295
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发表时间:
2010-01-01
影响因子:
16.6
通讯作者:
Grzybowski, Bartosz A.
中科院分区:
文献类型:
--
作者:
Kowalczyk, Bartlomiej;Walker, David A.;Grzybowski, Bartosz A.
One of the main applications of metal nanoparticles (NPs) is in the detection of biologically important [1] or toxic substances,[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] however, 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, Section 1) to affect even small shifts in the nanoparticles 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 limited to the catalytic deposition of silver on surface-immobilized AuNPs.[8] Herein, we show that NP supracrystals and previously unreported core–shell (CS) supracrystals (Figure1) 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 compositions and are stabilized with different cross-linkers; consequently, 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 Æ1. 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 oppositely charged NPs (see Ref.[9] and the Supporting Information, Section 2 for details). The 1–2 μm 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 different from those in the crystal core. In this way, core–shell crystals (each up to ca. 2.5 μm across …