Open Access Article
Anastasia O.
Maslova
ab and
I. Ming
Hsing
*ab
aDepartment of Chemical and Biological Engineering, The Hong Kong University of Science and Technology, Hong Kong, China. E-mail: kehsing@ust.hk
bBioengineering Graduate Program, The Hong Kong University of Science and Technology, Hong Kong, China
First published on 20th September 2018
Gold nanoparticles (AuNPs) decorated with thiol-modified DNA (HS-DNA) strands are an extensively studied, easily adjustable, and highly controllable material for constructing 3D nanostructures with various shapes and functions. However, few reproducible and robust methods involving DNA templates as a key reagent are available for obtaining 3D nanoparticle assemblies. It is still challenging to strictly control the number and location of DNA strands on the AuNP surface. Here, we introduce an efficient approach for the surface modification of AuNPs using unmodified DNA oligonucleotides by building DNA cages that trap the nanoparticles. This enables us to vary the process of nanostructure assembly and create anisotropic nanoparticles that are necessary for directed structure construction. This developed method simplifies the production process in comparison with conventional HS-DNA modification protocols and helps to precisely control the density and position of functional DNA strands designed for further hybridization with other AuNP conjugates.
Surface modification of gold nanoparticles is often required for the assembly of 1D/2D/3D nanoparticles. However, the process of synthesizing asymmetrically functionalized AuNPs is complex and the results, although reproducible, suffer from side products.8 The first method for surface modification was introduced independently by Mirkin et al.9 and Alivisatos et al.10 They developed approaches providing high-density DNA coverage of the nanoparticle surface and low-density coverage, respectively. Their method utilizes thiol chemistry, and an excess of single-stranded DNA (ssDNA) oligonucleotides is necessary for attaching the strands to the gold. ssDNA strands allow the aggregation of nanoparticles through the hybridization process when the target complimentary strand is introduced into solution. Although this method is highly reproducible, one might want to control the stoichiometry and the placement of the DNA strands, and reduce the number of oligonucleotides on the surface to achieve directed, and not random, structure growth and assembly. Several methods were introduced over the years, including dATP-assisted surface modification,11,12 and a modified13 Taton's protocol14 for low-density surface functionalization, but they still do not enable full control over the assembly of the nanoparticles. Furthermore, it is impossible to tailor-make multiple DNA strands in specific positions on a nanoparticle's surface based only on the optimized concentration ratios between thiol ssDNAs and AuNPs. The most that can be achieved is the attachment of several DNA strands in stochastic positions. To guide the assembly process, several methods were developed. Sleiman's group13 suggested the use of assisting DNA cages to place desired thiolated oligonucleotides in a designated pattern on the surface of the AuNP. This approach requires many steps, including washing, purification, and denaturation procedures, and is still limited to a template shape that directs the placement of functional DNA strands on the AuNP. Another low density approach introduced by Pei et al.15 where the number of functional ssDNA strands was controlled by polyA tails that served as an anchoring sequence without using thiol modification of DNA. Schreiber et al.16 came up with the idea of using DNA origami as a protective shell from high salt-induced aggregation and as an assistive structure for further nanostructure assembly. However, as in most origami procedures, this method requires a large amount of DNA.
Although DNA is a very good material for facilitating the formation of nanostructures from AuNPs at a nanoscale level, it remains challenging to grow nanostructures from 1D to 2D and 3D patterns.17 Encapsulating a nanoparticle in a DNA cage is an interesting approach. There are numerous reports on building DNA cages for cargo delivery that demonstrate the robustness and reproducibility of this method. AuNPs are known to be a good support material for DNA polyhedrons.18–21 Origami cages22 can accommodate nanoparticles inside, restrict the surface of nanoparticles, and form asymmetric hybridization sites for growing complexes.
Our approach uses unmodified DNA oligonucleotides to create anisotropic AuNPs with the further generation of nanostructures without using DNA origami-based structures as a lattice that supports the AuNPs. DNA oligonucleotides form a cage that traps the AuNP, can easily adapt to the form of the nanoparticle, and does not involve large amounts of DNA. The cage is octahedral in shape, with each edge consisting of double-stranded DNA (dsDNA) with ssDNA regions, which are used to help control the placement of reactant oligonucleotides. The construction of nanostructures depends on the hybridization process between hanging complementary regions of the DNA cage.
Functionalized DNA conjugates can then be used as building blocks for electronic devices based on linear chains and self-assembled monolayers (SAMs),23–25 where AuNPs bring electrical function to a non-conductive DNA scaffold. The advantage of this method over similar approaches is that the assembly process is consistent in design simplicity and in the reduced use of DNA in the supporting scaffold. Controlled nanoparticle-based nanostructures using nucleic acid circuits and functionalized AuNPs are likely to have useful applications in diagnostic and therapeutic fields.
000 rpm for 35 minutes at 4 °C) to remove excess reagents. The obtained conjugates were resuspended in 100 μL 10 mM PBS (pH 8.0) with 0.3 M NaCl.
000 rpm and 4 °C for 30 minutes and washed with 10 mM PBS with 0.1 M NaCl. The presence of DNA at the surface was demonstrated using 1% agarose gel electrophoresis (8 V cm−1, 1 h, 0.5× TBE), and the effective diameter was measured using dynamic light scattering and AFM/TEM imaging.
:
1 ratio, and incubated at room temperature for four hours. Structure verification was obtained using 1% agarose gel electrophoresis (8 V cm−1, 1 h, 0.5× TBE) and AFM/TEM imaging.
For the hybridization chain reaction, two hairpin probes were separately conjugated onto the DNA cage around the AuNPs, AuNP-H1 and AuNP-H2. Then, they were mixed together and incubated overnight at room temperature. An initiator strand was then added to trigger the reaction in a 1
:
3 ratio with the amount of each hairpin. After incubation for four hours, TEM imaging and 1% agarose gel electrophoresis were performed.
For TEM imaging, a JEM 2010 transmission electron microscope (JEOL) operated at 200 kV was used. The images were analyzed using a GATAN MSC 794 CCD Camera and GATAN Digital Microscopy software. Five μL AuNP assemblies were transferred to SPI® Supplies Holey carbon coated grids onto 400 mesh copper, incubated for three minutes, washed with 50 μL of MQ-pure water, and dried under nitrogen gas. Samples were then dried completely for at least 15 hours under ambient conditions in a vacuum desiccator.
The quality of the obtained structure was verified using 10% PAGE (Fig. 1a): several reaction mixtures were prepared with a different number of ssDNA strands ranging from one to eight. Line 8 in Fig. 1a corresponds to the mixture with all the necessary DNA strands to form the desired product, while the rest act as controls containing different subsets of the reactant strands. The octahedron can be formed without any additional pre-assembly steps, and the size of the edges is big enough to facilitate the building of the preferred structure.
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| Fig. 1 (a) 10% PAGE gel with DNA assemblies of octahedron parts. L1 and L2 – DNA ladders with 5 and 50 bp steps respectively, and the number of ssDNA oligonucleotides in the reaction mixture for octahedron assembly ranged from one to eight. (b) a photo of the two types of AuNPs, see text for details, and AFM image of type 2 AuNPs that does not show any aggregation signs. A picture with higher resolution can be seen in the ESI (Fig. S2).† (c) 2% agarose gel, from left to right: line 1 – control OEG-AuNPs, line 2 – OEG-AuNPs after mixing with the hemispheres and octahedron assembly; DLS measurement of the particle size: black – control AuNPs, red – AuNPs with octahedron assembly. | ||
The hemispheres were mixed (Fig. 1b, S3†) with 10 nm AuNPs of two types: bare AuNPs (type 1) and thiol-OEG coated AuNPs (type 2) for stability control using a published dATP protocol.12 Type 1 AuNPs were not stable in buffers with a sodium concentration larger than 0.2 M and in the presence of Mg2+ ions, due to large areas that were not protected by DNA. So, although it was possible to create an octahedron assembly around bare AuNPs, thiol-OEG-protected AuNPs were used for further reactions in order to ensure robust DNA assembly and to reduce of the number of side products it is necessary to use bivalent ions. Moreover, the neutral surface of type 2 AuNPs did not interfere with the assembly process compared with bare, citrate-stabilized AuNPs. Type 2 AuNPs also did not show any signs of aggregation in solutions with high ionic strength. The neutral charge in type 2 AuNPs allowed us to use dsDNA to form polyhedrons with more faces than octahedrons and make assemblies in more stringent conditions. In addition to the AFM data, DLS analysis was performed (Fig. 1c) to control the size of the particles.
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| Scheme 2 Hybridization scheme. (a) The composition of the octahedron (two hemispheres – green and red) with sticky toeholds (grey) for type D1, D2, T1 or T3 of the AuNPs; note: type 2 AuNPs have toeholds in positions A2 and A4, see S2.† (b) The resulting pair of AuNPs. (c) A trio of AuNPs. | ||
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| Fig. 2 (a) AFM image of AuNP pair assemblies with height profile and a 1% AGE control. A picture with higher resolution can be seen in the ESI (Fig. S4†). (b) The TEM image of triple AuNP assemblies; the scale bar corresponds to 50 nm (left) and 20 nm (right). | ||
Based on the TEM image analysis, the yield of triple assemblies for type 1 AuNPs was 40%. This yield was the consequence of the reaction conditions: low salt concentrations were used in order to prevent the random aggregation of nanoparticles, because only ∼34% of the nanoparticle's surface was protected by DNA. When type 2 AuNPs were used, the yield was nearly 70%. The yield was measured based on the band intensity in agarose gel electrophoresis.
The yield percentage may be further controlled by varying the toehold length. A long toehold makes hybridization more accessible, and the melting temperature for the assembly is higher, which increases the number of successful constructions.
Based on the control reaction without AuNPs (Fig. S6†), the estimated length of the product should correspond to a chain of 20–30 AuNPs. However, the maximum length that could be achieved was 8–10 AuNPs. This could be explained by the assumption that HCR product polymerization goes through a chain-growth mechanism with a very fast initiation rate and a slow propagation rate. Also, the distribution of chain length follows a Poisson distribution shape, meaning that the most probable product length to be observed in this condition is 5–7 AuNPs per chain.
The average length distribution of HCR chains was calculated based on the obtained TEM images (40
000× magnification) for AuNP assemblies (Fig. 4a and S7†) and PAGE gels for DNA controls. All calculations and curve-fitting processes were performed using Matlab. The degree of polymerization fits a Poisson distribution, which proves our assumption that the HCR follows a chain-growth mechanism.32,33 According to the DNA control lane in the PAGE gel (Fig. 4b), the longest chains should be equal to or longer than 10 monomers; however, the TEM image shows that the longest observed chain is eight AuNPs, which may be due to the fact that when the chain grows, the particle concentration decreases, and the possibility of a collision between the monomers and growing polymers drops too, so the probability of observing a long chain in the TEM image is low.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c8na00148k |
| This journal is © The Royal Society of Chemistry 2019 |