Chun-Pong
Chak
a,
Josie M. Y.
Lai
b,
Kathy W. Y.
Sham
b,
Christopher H. K.
Cheng
*b and
Ken Cham-Fai
Leung
*ac
aCentre of Novel Functional Molecules and Institute of Molecular Functional Materials, Department of Chemistry, The Chinese University of Hong Kong, Shatin, NT, Hong Kong SAR, P.R. China. E-mail: cfleung@cuhk.edu.hk
bSchool of Biomedical Sciences, The Chinese University of Hong Kong, Shatin, NT, Hong Kong SAR, P.R. China
cInstitute of Creativity and Department of Chemistry, The Hong Kong Baptist University, Kowloon Tong, Kowloon, Hong Kong SAR, P.R. China
First published on 6th October 2011
Short single-strand (ss) DNA sensors that involve mono-functionalized gold nanoparticles are reported for the first time. By way of an example, the hybridization and detection of a 10 base-pair oligonucleotide (TGACTCTTAA), which relates to the pathogenicity island of vancomycin-resistant Enterococcus faecalis, has been demonstrated in the organic solvent mixture (DMF/CHCl3/H2O/NaCl) at sub-nanomole concentrations. The formation of the resulting double-strand (ds) DNA–AuNP complexes which involve either tail-to-tail or head-to-head alignment, are sensitive to salt (NaCl) and solvent (CHCl3) concentrations. By UV/visible absorption measurements, it has been found that the melting temperature of the dsDNA–AuNP complexes increases with increasing salt concentrations as well as the chloroform ratio, for both tail-to-tail and head-to-head alignments. Transmission electron microscopic images of the dsDNA–AuNP complexes with mono-functionalized AuNPs reveal significant amounts of dimeric AuNP species while that of randomly functionalized AuNPs reveal an agglomerated AuNP nanostructures.
Gold nanoparticles (AuNP) are a desirable and outstanding candidate for this application because it is (1) relatively stable; (2) non-aggregated compared to other nanoparticles (e.g., magnetic particles); (3) size tunable (down to sub-nanometre); (4) shape tunable (e.g., spheres, cubes, rods, etc.); and (5) size/shape/distance-dependent to their optical properties.8–10
Most of the sensor applications employ the use of randomly functionalized AuNPs as the components for further DNA attachments.11–15DNA primers are usually attached to the surface of AuNPs by a place exchange reaction of thiolate. After addition of the target DNA, there exists a change of UV absorbance at the characteristic gold–DNA complex bands at 260 nm, 520 nm and beyond, which are corresponded to the formation of the gold–DNA complexes and hence, a decrease in the interparticle distance between AuNPs.13,14
However, there exist particle–particle repulsions between bulky and negatively charged DNA, thereby affecting the ‘melting point’ of the gold–DNA complexes in randomly functionalized AuNPs.16 Such deviations may be different batch-by-batch and depend on different lengths and sequences of DNA used. Calibration of such AuNP-based sensors would be required for individual experiment when different lengths and sequences of DNA are used.
It was also found that the probe density of the AuNPs alters the properties of gold–DNA complexes,16i.e., the ‘melting point’ of the gold–DNA complexes decreased with the decrease in probe density. Such a probe density change was achieved by the addition of some diluent strands onto the AuNPs via place exchange reaction, which was an average (by estimation) in all of the AuNPs present. It is unsure that all AuNPs possess the same or very close probe density and that the probe density would approximately decrease to 33%.
The preparation of mono-functionalized AuNPs has been explored in recent years.17–19 Recently, the synthesis of such mono-functionalized AuNPs with an average diameter of 2.0–2.2 nm can be achieved using supramolecular and solid phase supported chemistry.20 Herein, we report the use of mono-functionalized AuNPs for the attachment of short single-strand DNA (10 base pairs) by a simple and quantitative thiol–maleimide click reaction to afford the mono-functionalized AuNP-based DNA sensors. It is not necessary to synthesize any additional mercaptoalkyl-oligonucleotide or to use a longer sequence of DNA, which is essential for randomly functionalized AuNPs to generate ample space for effective agglomeration.16 Hence, commercially available mercapto-oligonucleotide can be used. Moreover, a relatively short sequence of DNA (10 base pairs) was attached to the mono-functionalized AuNPs to provide minimal steric and electrostatic repulsion between AuNPs during DNA assembly. In this paper, we report for the first time the use of mono-functionalized oligonucleotide AuNPs as a sensor for a polynucleotide related to the pathogenicity island of vancomycin-resistant Enterococcus faecalis21 at sub-nanomole concentrations. Tail-to-tail and head-to-head dsDNA–AuNP dimeric assemblies can be formed and characterized by UV/visible absorption spectroscopy, providing future nano-medicinal applications.21–25
The dsDNA–AuNP complexes of this study were dissolved in a mixture of organic solvents (N,N′-dimethylformamide (DMF) and CHCl3) with specific amounts of NaCl solution. The use of organic solvents for the DNA assembly provides new approaches for novel structural gene delivery.26,27 Moreover, dsDNA–AuNP sensors could be operated in alcoholic solvents.28 Because of the DNA denaturing nature of DMF, dsDNA–AuNP sensors that are compatible with DMF have not yet been reported. However, it was found that DNA assemblies of short sequences (21 base pairs) were basically intact even in 95% DMF solution, while longer DNA sequences were denatured.29 Such findings support that our target double stranded DNA (10 base pairs) AuNPs would be stable in organic solvent systems.
Entry | ssPrimer A (5′→3′) | ssPrimer B (5′→3′) | ssTarget A′B′ (5′→3′) | dsDNA–AuNP alignment |
---|---|---|---|---|
1–6 | HS-TTAAG | AGTCA-SH | TGACTCTTAA | Tail-to-tail |
7–12 | TTAAG-SH | HS-AGTCA | TGACTCTTAA | Head-to-head |
Entry | ssPrimer A (5′→3′) | ssPrimer B (5′→3′) | ssTarget A′B′ (5′→3′) | dsDNA–AuNP alignment |
---|---|---|---|---|
13–15 | TTAAG-SH | HS-AGTCA | TGACTCTTAA | Head-to-head |
Entry | [Primer A] = [Primer B] = [Target A′B′] (μM) | [AuNP] (μg mL−1) |
---|---|---|
1–6 | 0.3989 | 61.4 |
7–12 | 0.3991 | 61.4 |
13–15 | 1.9515 | 60.1 |
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Fig. 1 Graphical depiction for the formation of the dsDNA–gold nanoparticle tail-to-tail and head-to-head dimers. |
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Fig. 2 Stacked FT-IR spectra of the mono-functionalized AuNP, mono-maleimido functionalized AuNP, head-to-head dsDNA–AuNP dimer and the tail-to-tail dsDNA–AuNP dimer. |
Nanostructures | IR absorption frequency (cm−1) | Assignment |
---|---|---|
mono-maleimido functionalized AuNP | 2936 | alkane C–H stretching |
1744 | ester C=O stretching | |
1707 | unsymmetric maleimide C=O stretching | |
1651 | amide C=O stretching | |
837 | para-substituted aromatics C–H | |
dsDNA–AuNP head-to-head dimer | 2924 | alkane C–H stretching |
1722 | ester C=O stretching | |
1631 | amide C=O stretching | |
1094 (broad) | symmetric PO2− stretching | |
828 | para-substituted aromatics C–H | |
dsDNA–AuNP tail-to-tail dimer | 2924 | alkane C–H stretching |
1722 | ester C=O stretching | |
1633 | amide C=O stretching | |
1097 (broad) | symmetric PO2− stretching | |
830 | para-substituted aromatics C–H |
Upon addition of the target ssDNA A′B′ to the mono-ssPrimer functionalized AuNPs, the absorbance of AuNP at 521 nm disappeared, indicating that new dsDNA–AuNP nanostructures were formed. Upon melting temperature analysis, the increased temperature of the dsDNA–AuNP would increase the relative absorbance at 521 nm, indicating that the AuNPs were dissociated into a monomeric state. Melting curves were plotted wherein the melting temperatures were determined according to the first derivatives of the curves (Table 6). The dsDNA–AuNP complexes possess two structural alignments: tail-to-tail (Table 1) and head-to-head (Tables 1 and 2). For tail-to-tail alignment, two AuNPs were expected to align with each end connected with the target dsDNA strand. For head-to-head alignment, two AuNPs were expected to align closely at the middle of the target dsDNA strand (Fig. 1). However, red shifts of the characteristic absorption wavelength from 520 nm to 650 nm were not observed in both cases. It may be attributed that the formation of AuNP dimers have only a small degree of agglomeration and the inter-particle distance between two AuNPs is larger than the average size of an individual AuNP, and such shifts are too weak to be detected.33,34 The assembling yield, which was measured by the percentage of dimer formation, and the interparticle distance of the AuNPs were measured using the transmission electron microscopy (TEM) images, which showed that they are longer than the average size of an individual AuNPs and have a satisfactory assembling yield (Table 5). That such a long interparticle distance was obtained even for head-to-head alignment may be due to the flexibility of the ligand linker, together with the flexibility of DNA which places the AuNPs opposite to each other (Fig. 1). Therefore, the SPR band was not shifted from 521 nm to > 600 nm upon formation of dimer. Rather, the increase in the SPR band at 521 nm during melting was used to measure the monomeric state of the AuNPs and such observation agrees well with the literature.35
Entry | Interparticle distance (TEM)b | Assembly yield (% dimer formed)b | Alignment |
---|---|---|---|
a Randomly functionalized AuNPs are used. b Measured by counting 60 particles. | |||
3 | 3.5–5.0 nm | 79% | Tail-to-tail |
6 | 3.1–5.0 nm | 72% | Tail-to-tail |
9 | 2.7–4.5 nm | 70% | Head-to-head |
12 | 3.0–4.5 nm | 73% | Head-to-head |
15a | 2.0–3.6 nm | Nil. | Head-to-head |
Entry | Melting Temperature °C | Solvent ratio (DMF/CHCl3/H2O) | [NaCl] (μM) | dsDNA–AuNP alignment |
---|---|---|---|---|
a Randomly functionalized AuNPs are used. | ||||
1 | 24.1 | 1![]() ![]() ![]() ![]() |
1 | Tail-to-tail |
2 | 26.6 | 1![]() ![]() ![]() ![]() |
5 | Tail-to-tail |
3 | 29.3 | 1![]() ![]() ![]() ![]() |
10 | Tail-to-tail |
4 | 24.9 | 1![]() ![]() ![]() ![]() |
1 | Tail-to-tail |
5 | 27.8 | 1![]() ![]() ![]() ![]() |
5 | Tail-to-tail |
6 | 30.0 | 1![]() ![]() ![]() ![]() |
10 | Tail-to-tail |
7 | 23.8 | 1![]() ![]() ![]() ![]() |
1 | Head-to-head |
8 | 26.5 | 1![]() ![]() ![]() ![]() |
5 | Head-to-head |
9 | 29.0 | 1![]() ![]() ![]() ![]() |
10 | Head-to-head |
10 | 25.2 | 1![]() ![]() ![]() ![]() |
1 | Head-to-head |
11 | 27.0 | 1![]() ![]() ![]() ![]() |
5 | Head-to-head |
12 | 30.3 | 1![]() ![]() ![]() ![]() |
10 | Head-to-head |
13a | 27.1 | 1![]() ![]() ![]() ![]() |
1 | Head-to-head |
14a | 28.6 | 1![]() ![]() ![]() ![]() |
5 | Head-to-head |
15a | 31.7 | 1![]() ![]() ![]() ![]() |
10 | Head-to-head |
It is also not surprising to find out that the interparticle distance of the randomly functionalized AuNPs determined by TEM was generally shorter than that of the mono-functionalized AuNPs (Table 5). The randomly functionalized AuNPs may form three-dimensional network aggregations (Fig. 3) and the AuNPs can aggregate through three-dimensional spaces. As observed from the TEM images, which cannot resolve the three-dimensional domains, the interparticle distance of the randomly functionalized AuNPs should be smaller. Such three-dimensional network aggregations may also form even when there exists a few components on the AuNPs which have not been self-assembled with its recognizing targets, indicating that detection using randomly functionalized AuNPs is somewhat less sensitive. This is an important issue for developing a more quantitative detection method for single molecules in the future.
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Fig. 3 Graphical depiction for the formation of dsDNA–AuNP head-to-head oligomers, using randomly functionalized AuNPs. |
By comparing the melting temperature results (Table 6 and Fig. 4), the head-to-head alignments possess similar melting temperatures to those of the tail-to-tail alignments under the same conditions, which is highly unusual when randomly functionalized AuNPs are used. It is believed that they possess enhanced steric and electrostatic repulsion between the DNA in the randomly functionalized AuNPs when in close proximity. This effect can be minimized by using mono-functionalized AuNP.
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Fig. 4 First derivative of melting curves of selected entries (3, 6, 9, 12, and 15). The melting temperatures of entries 3 and 9 are similar at ca. 29 °C; whilst the melting temperatures of entries 6 and 12 are similar at ca. 30 °C. It indicates that the alignment of the DNA-AuNPs does not affect the melting temperature to any great extent; rather the solvent effect will cause a greater change in melting temperature (comparison between 3, 6 and 9, 12 respectively). The randomly functionalized AuNPs possess a higher melting temperature than the mono-functionalized AuNPs, compare entry 9 with entry 15, which is under the same conditions (y-axis not to scale). |
Salts are essential for DNA assembly for charge balance in the dsDNA structures, especially in the presence of organic solvents. The salt effect in the formation of dsDNA–AuNP nanostructures was studied (Fig. 5). Three different concentrations of sodium chloride solution (1, 5, and 10 μM) were added to the mixtures. It was found that the melting temperature (Table 6) of the dsDNA–AuNP complexes increases with increasing salt concentrations for both tail-to-tail and head-to-head alignments.
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Fig. 5 Relationship between the salt concentration and melting temperature of dsDNA–AuNP nanostructures. |
The solvent effect on the formation of the dsDNA–AuNP complexes is also studied by increasing the ratio of CHCl3 to DMF. Since the target DNA consists of only 10 base pairs, such short DNA increases the hydrophobicity and hence reduces the free energy in the annealing process. Moreover, the mono-ssPrimer functionalized AuNPs are more soluble in CHCl3 than in DMF.
Therefore, addition of CHCl3 should also increase the stability of the dsDNA–AuNP nanostructures. As a result, the melting temperatures of the dsDNA–AuNP nanostructures increase with the increasing CHCl3 ratio. The melting temperature difference of dsDNA between the mono-functionalized AuNPs (entries 7–9) and the randomly functionalized AuNPs (entries 13–15) is compared. The melting temperatures using the randomly functionalized AuNPs for dsDNA assembly are higher than that of the mono-functionalized AuNPs by 1.9–3.3 °C for the same conditions. That is, the melting temperature increases with increasing probe density. Therefore, the probe density was tunable not only by diluent stranded place exchange reaction, but also by controlling the functional ligand density of the particle’s surface.
The dsDNA–AuNP solutions were analyzed by TEM with nearly the same AuNP concentrations (Table 3). The TEM images of solutions of entries 3 and 6, which contain the tail-to-tail dimeric species, reveal significant amounts of AuNP dimer pairs (Fig. 6, pairing of dark dots). Similarly, significant amounts of AuNP dimer pairs are also observed in their TEM images for the solutions of entries 9 and 12 from which they contain head-to-head dimeric species. In contrast, the TEM image of the solution of entry 15 reveals agglomerated AuNP nanostructures. This observation demonstrates that the randomly functionalized AuNPs involve the formation of a network of AuNPs while the mono-functionalized AuNPs form discrete nanostructures.
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Fig. 6 Transmission electron microscopic images of entries 3 and 6 (dsDNA–AuNP, tail-to-tail alignment); entries 9 and 12 (dsDNA–AuNP, head-to-head alignment); and entry 15 (dsDNA–randomly functionalized AuNP, head-to-head alignment). The scale bar (white) represents 20 nm. |
The formation of randomly agglomerated nanostructures may presumably result in the cross binding of non-hybridized primer-DNA and AuNPs trapped within a sterically crowded network, leading to inaccurate shifts of UV/visible absorption signals. While our mono-functionalized AuNPs which provide one to one DNA annealing to AuNP, the spectroscopic signals are revealed by the formation of discrete dsDNA–AuNP dimeric complexes. This approach based on the formation of discrete nanoparticles and the less sterically hindered head-to-head alignment provides a more quantitative sensing property, and great potential for future applications in nanomedicine and aptamer sensor development.
This journal is © The Royal Society of Chemistry 2011 |