gold nanoparticle 3d-dna building blocks: high purity preparation and use for modular access to...
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Gold Nanoparticle 3D-DNA Building Blocks: High Purity Preparation and Use for Modular Access to Nanoparticle Assemblies
Kai Lin Lau , Graham D. Hamblin , and Hanadi F. Sleiman *
Gold nanoparticle (AuNP) assemblies have garnered much
interest with regard to applications in nanophotonics and
nanoelectronics. [ 1 ] A key aspect to their possible implementa-
tion is the ability to organize such assemblies with ease and
control. In this context, the use of DNA to guide the organi-
zation of AuNPs has been extensively investigated, given its
highly predictable self-assembly properties. These properties
combined with knowledge of DNA structural parameters
have led to the development of a wide variety of nanoarchi-
tectures – from basic, fl exible single-stranded DNA, to rigid
tile-motifs, DNA origami, and DNA nanotubes. Furthermore,
current commercial availability and automated synthesis
allows for facile preparation of DNA featuring any number
of functional groups, over a wide range of desired length and
sequence. The result is a substantial library of DNA struc-
tures which may be used in the organization of materials,
including AuNPs. [ 2 ]
Numerous approaches for the preparation of one-dimen-
sional AuNP assemblies via DNA have been detailed. [ 3 ]
These include methods which utilize DNA sequence-specifi c
hybridization, as well as electrostatic, intercalative interac-
tions, and covalent conjugation chemistry. One early class of
structures which utilizes a sequence-specifi c approach is DNA
tile-motifs. Rigid DNA tiles composed of oriented duplexes
with addressable sticky ends may be used to organize AuNPs
into extended one-dimensional arrays upon self-assembly
of the tiles into higher order structures, with the possibility
for patterning and alignment. [ 3f-j ] Despite the sophistication
of tile-motifs for the preparation of extended AuNP archi-
tectures, their assembly is reliant on a step-growth poly-
merization mechanism where monomers fi rst react to form
dimers, then trimers and eventually long polymers. Hence, as
with synthetic polymers, analogous limitations are imposed
regarding poor size control of long, extended assemblies.
More recently, DNA origami featuring remarkable struc-
tural complexity has emerged as a powerful tool for the
assembly of AuNPs. [ 2e , 3k-m , 4 ] Using a multitude of unique
staple strands, a single genomic template strand may be
folded into a phenomenal variety of structures featuring full
addressability. The power of DNA origami as an organiza-
tional scaffold stems from this inherent addressability, as
the modifi cation of select staple strands for functionaliza-
tion with AuNPs allows precise positioning of AuNPs in
desired locations for well-defi ned linear assemblies. None-
theless, the preparation of DNA origami scaffolds is not
trivial. It requires hundreds of unique staple strands and long
annealing times for each structure, compounded by the cost
of starting materials and error rate of self-assembly. [ 5 ] Fur-
thermore, DNA origami has yet to enable organization of
extended AuNP assemblies due to inherent size limitations
regarding the single long scaffold strand.
The use of long enzymatically produced template strands
presents an interesting alternative approach for the prepara-
tion of AuNP assemblies. Through rolling circle amplifi cation
(RCA), a DNA backbone strand featuring a repeat sequence
motif may be easily prepared. The placement of AuNPs
on this backbone strand can then be achieved through a
variety of means, from the use of protein interactions, to
direct hybridization with DNA-AuNP mono-conjugates. [ 3n-p ]
In particular, the latter option is especially attractive given
the aforementioned advantages of DNA directed assembly.
Overall, such an approach strikes a practical balance between
tile-based assembly and DNA origami scaffolds with regard
to control, complexity, and size. It has signifi cant simplicity in
comparison to DNA origami, without the need for numerous
constituent stands. At the same time, it enables the templated
assembly of extended AuNPs architectures on the scale of
several hundreds of nanometers and larger, without the
poor size control associated with step-growth polymerization
mechanisms.
Despite this, there are few reports in the literature uti-
lizing RCA produced DNA backbone strands for the templa-
tion of one-dimensional AuNP assemblies, and even fewer
where direct hybridization with DNA-AuNP mono-conju-
gates is used to organize the AuNPs. [ 3n-p ] Furthermore, of
those which feature direct hybridization for AuNP placement,
simple double-stranded DNA was the organizational scaf-
fold, with resultant AuNP structures exhibiting low rigidity.
Here, we report a new strategy in using RCA templated
assembly for the preparation of one-dimensional AuNP DOI: 10.1002/smll.201301562
Self-Assembly
K. L. Lau, G. D. Hamblin, Prof. H. F. SleimanDepartment of ChemistryMcGill University Montreal QC , H3A 2K6 , Canada E-mail: [email protected]
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assemblies. Recent work in our group has demonstrated the
simple and rapid formation of well-defi ned DNA nanotubes,
featuring minimal complexity. [ 6 ] The basic design consisted of
a triangular rung unit composed of fi ve unmodifi ed compo-
nent strands and a single-stranded binding region of 42 bp,
giving the rung an approximate length of 14.3 nm. Upon
addition of a templating RCA backbone strand featuring
repeating binding sites for the rung, DNA nanotubes of 0.64 ± 0.24 μ m were thus formed. Herein, we utilize this DNA nano-
tube structure as a platform upon which AuNPs are site-
specifi cally organized into well-defi ned linear arrays. This is
achieved through the construction of DNA-AuNP mono-
conjugates, in which a gold nanoparticle is stably attached to
a three-dimensional DNA rung structure, followed by their
hybridization to linear DNA strands with repeat binding sites.
In order to utilize this DNA nanotube structure as a plat-
form, we planned to conjugate AuNPs with the triangular
rung unit, whereupon hybridization with the RCA backbone
strand ( RCA ) would yield a one-dimensional assembly of
AuNPs ( Scheme 1 ). Shown in Scheme 1 a, one side of the
rung has a single-stranded binding region, whilst the other
two have very short single-stranded and self-complementary
sticky ends of three bases (labelled x , y , x ’ and y ’). These fea-
tures were designed to facilitate nanotube formation when
hybridized with the RCA backbone strand. [ 6 ] To enable
conjugation to AuNPs however, additional features were
incorporated into the basic triangular rung unit to give the
modifi ed rung unit, labeled RNG . One component strand was
elongated and another component strand added to create
a 15 bp double-stranded overhang featuring two terminal
cyclic dithiols which could conjugate to AuNPs. The use of
multiple thiol anchor points has been shown to yield better
conjugation to AuNPs. [ 7 ] Quantitative formation of this mod-
ifi ed rung was confi rmed by gel electrophoresis (Supporting
Information, Figure S2).
To our knowledge, this conjugation approach is unique.
The majority of assembly strategies for DNA-AuNP mono-
conjugates feature AuNPs modifi ed with simple single-
stranded or double-stranded DNA. [ 3j , 7a,c , 8 ] In contrast, our
strategy is reliant on mono-conjugation of AuNPs with a pre-
formed three-dimensional DNA nanostructure. This presents
several distinct advantages. Firstly, the use of the triangular
rung presents a facile means of adding further functionality,
as its multiple component strands may be easily modifi ed
to feature functional groups or overhangs for the attach-
ment of other cargo. [ 6 ] In essence, a DNA-AuNP three-
dimensional ‘building-block’ is created. In fact, although the
AuNP is technically mono-conjugated, it may be considered
as functionally divalent (or multivalent) due to the multiple,
modifi able components strands and directionality present
in the triangular rung unit. The result is a facile method by
which functional multivalency of AuNPs may be accessed,
the preparation of which has sparked interest with regard
to their potential use for AuNP assemblies. [ 3q,r , 9 ] Finally, it
is well known that DNA-AuNP mono-conjugation is lim-
ited with regard to AuNP size and DNA length, as the use of
AuNPs of >15 nm and/or DNA of <80 bp makes it diffi cult to
fully resolve between non-conjugated and mono-conjugated
product. Although our group has introduced a non-covalent
extension strategy to help overcome this limitation, its use
presents several more work up steps in order to obtain the
fi nal mono-conjugate product. [ 7c ] By conjugating to a com-
paratively large three-dimensional DNA structure, these
steps can be avoided. Given these advantages, we predict
that our novel conjugation approach will have a signifi cant
impact on available DNA-directed AuNP assembly strategies
beyond the preparation of one-dimensional arrays as pre-
sented herein.
Scheme 1. General strategy for the assembly of one-dimensional AuNP assemblies through using our DNA nanotube as an organizational platform. a) The basic rung unit of our nanotube was modifi ed to feature a double stranded overhang with two terminal cyclic dithiols. These rungs were labeled RNG . b) Through this two dithiol moieties, incubation of RNG with AuNPs could thus give RNG -AuNP conjugates. Addition of RCA would therefore yield the alignment of RNG -AuNP conjugates into a one-dimensional assembly.
RCA
b.
RT, overnight
RNG
RT, overnight
Constant Core
x
y
x’
y’RNG
Bin
ding
Reg
ion Over-
hang
a. 2 x
SS
OP
O
O
OH
O
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In order to show the feasibility of such a conjugation
strategy, RNG was fi rst conjugated to 13 nm diameter AuNPs
by combining in equimolar amounts and incubating over-
night. 13 nm AuNPs were chosen to agree with the rung length
of 42 bp (ca. 14.3 nm). These conjugates were then modifi ed
with a low molecular weight thiolated polyethylene glycol
ligand in order to stabilize the AuNPs in the buffer condi-
tions necessary for nanotube formation. [ 10 ] Figure 1 a depicts
agarose gel electrophoresis (AGE) of the resultant products.
Lane 1 corresponds to a 13 nm AuNP control, and lane 2 to
the sample mixture. The appearance of lower-mobility bands
in lane 2 suggested the formation of RNG -AuNP mono-
conjugate and di-conjugate, with the mono-conjugate band
as indicated in Figure 1 a. Subsequently, the desired RNG -
AuNP mono-conjugate was purifi ed via band excision and
electroelution. Figure 1 b depicts AGE characterization of
this process, where lane 1 corresponds to a 13 nm AuNP con-
trol, and lane 2 to the purifi ed RNG -AuNP conjugate. The
single band of lane 2 indicates that the rung DNA structure is
robust enough to remain intact through the purifi cation pro-
cess. Furthermore, the clean and well-resolved nature of the
bands highlight the advantage of mono-conjugation with a
preformed DNA structure. In previous work featuring single-
stranded DNA conjugated to 13 nm AuNPs, mono-conju-
gated structures could not be resolved directly, and required
the use of a long single-stranded DNA extension strand (the
non-covalent extension strategy). [ 7c ] Here, RNG -AuNP con-
jugates may be directly resolved and purifi ed.
As a preliminary investigation into future use and the
versatility of such conjugates, further functionalization and
potential multivalency was examined. 13 nm AuNPs were
conjugated to a modifi ed version of RNG featuring two
single-stranded binding regions on two different sides of
the rung. With two single-stranded binding regions, the con-
jugates may be multivalently functionalized with species
featuring the appropriate complementary strands. To demon-
strate this, 6 nm AuNPs featuring complementary sequences
to the single-stranded binding regions were added to the
purifi ed conjugates. Figure 1 c depicts AGE characterization
of the resultant product. Lane 1 corresponds to the initial
purifi ed conjugate, and lane 2 to the purifi ed divalently func-
tionalized product. The lower mobility of the band in lane 2
suggests the formation of desired higher order structures. The
trivalently functionalized structures were further confi rmed
by transmission electron microscopy (TEM), as presented
under Figure 1 d.
With the formation of RNG -AuNP mono-conjugates,
their ability to hybridize to a templating strand was inves-
tigated via the controlled preparation of dimers, trimers
and tetramers upon addition of backbone strands featuring
the corresponding number of repeat binding regions ( BB2 ,
BB3 and BB4 in Scheme 2 ). This experiment was also per-
formed in order to demonstrate adaptability of our DNA
directed assembly strategy for the preparation of discrete
one-dimensional AuNP architectures. Figure 2 presents the
AGE and TEM characterization of the resulting products
Figure 1. a) 3% AGE characterization of incubated sample containing equimolar amounts of RNG and 13 nm AuNP. Lane 1 corresponds a 13 nm AuNP control, and lane 2 corresponds to the sample mixture. The indicated band of lower mobility is assumed to be of RNG -AuNP mono-conjugate. b) 3% AGE characterization of purifi ed RNG -AuNP conjugate. Lane 1 corresponds to a 13 nm AuNP control, and lane 2 to the RNG -AuNP conjugate purifi ed via excision and electroelution. c) 3% AGE characterization of modifi ed RNG -AuNP conjugates divalently functionalized with 6 nm AuNPs. Lane 1 corresponds to the purifi ed conjugates, with the orange arrows indicating binding regions. Lane 2 corresponds to the purifi ed divalently functionalized product. d) TEM images of the divalently functionalized samples. Scale bar is 50 nm.
a. 1. 2.
crud
e
b. 1. 2.
pure
c. 1. 2.
Scheme 2. Preparation of dimers, trimers, and tetramers from rung-DNA mono-conjugates via addition of backbone strands featuring the appropriate number of repeat binding regions. Here, BB2 refers to the dimerizing backbone strand, BB3 to the trimerizing backbone strand, and BB4 to the tetramerizing backbone strand.
BB2
2 x
3 x
4 x
BB3
BB4
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after purifi cation via agarose gel excision and subsequent
electroelution. Lanes 1 to 3 of AGE under Figure 2 a corre-
spond to purifi ed dimer, trimer and tetramer product, respec-
tively, and lane 4 to the RNG -AuNP mono-conjugate control.
Decreasing band mobility suggests the progressive formation
of these products, with the presence of well-defi ned single
bands demonstrating the robust nature of these conjugates
during the purifi cation process. TEM images of these sam-
ples as per Figure 2 b indicate the defi nitive formation of the
AuNP dimers, trimers and tetramers. Counting over 700 par-
ticles per sample through visual inspection, statistical analysis
showed that 60–65% of the AuNPs participated in their pre-
dicted higher order groupings. The presence of non-partici-
pating nanoparticles may be attributed to sample distortion
and denaturation upon sample preparation, especially given
the purity of the structures in observed in AGE characteri-
zation. [ 11 ] As such, the RNG -AuNP conjugates were shown
to successfully interact with complementary strands for tem-
plated assembly.
Interparticle distance histograms for the structures
observed via TEM showed that the majority of particles
within the structures were touching, with an interparticle
distance of ∼ 0 nm (Supporting Information, Figure S3). As
the diameter of the 13 nm AuNPs were chosen to corre-
spond to the DNA rung length of 14.3 nm, we anticipated
low interparticle distances of ca. 1.3 nm. The observance of
interparticle distances of ∼ 0 nm appears to correspond well
with this expected value, as distances of ca. 1.3 nm may not
be well resolved via TEM, and AuNPs have the propensity to
aggregate during the drying process of sample preparation.
However, despite the apparent correspondence of ∼ 0 nm
interparticle distances with that expected, we believe that
the nanoparticles in solution are in actuality characterized
by larger interparticle distances due to added structural
freedom incurred by the 15 bp overhang used for conjuga-
tion of the DNA rung to AuNPs. Though the diameter of
the AuNPs were chosen to correspond to the length of the
triangular rung, the presence of the double-stranded over-
hangs must also be taken into account (15 bp, ca. 5.1 nm).
Hence, the maximum possible interparticle distance can be
calculated as ca. 24.5 nm, corresponding to orientation of
the double-stranded overhangs along the length of the rungs
and away from one another (14.3 nm, and 2 × 5.1 nm). This
structural freedom is particularly evidenced by the non-linear
shape observed in the trimer and tetramer assemblies, as
many do not appear as one-dimensional structures. Similarly,
the observation of larger interparticle distances via TEM can
be attributed this additional structural fl exibility introduced
by the overhang. A signifi cant portion of low interparticle
distances likely results from the aforementioned propensity
for AuNPs to aggregate during the drying process of sample
preparation.
One possible method of reducing the degrees of freedom
in this system is through modifi cation of the rung DNA
component strands with dithiol groups inserted at internal
rather than terminal positions, as previously reported by
our group. [ 7c ] Nonetheless, the formation of discrete dimers,
trimers and tetramers by these fi rst-generation DNA-AuNP
conjugates demonstrates the potential of our DNA directed
assembly strategy for the preparation of discrete one-dimen-
sional AuNP architectures of high purity and stability.
Having demonstrated binding capability of RNG -AuNP,
nanotube formation for the assembly of extended one-
dimensional AuNP architectures was attempted via addition
of the RCA backbone strand. Figure 3 a shows AGE char-
acterization of resultant structures. Lane 1 corresponds to
RNG -AuNP conjugates as the control, whereas lane 2 cor-
responds to a mixture of RCA added to RNG -AuNP at a
1:1.1 ratio, and incubated overnight. A slight excess of RNG -
AuNP was used to ensure complete nanotube formation.
Figure 2. Formation of discrete AuNP assemblies via addition of BB2 , BB3 , and BB4 backbone strands to RNG -AuNP mono-conjugates. a) 3% AGE of the assembled structures. Lanes 1–3 correspond to the purifi ed dimer, trimer, and tetramer products, respectively, and lane 4 to RNG -AuNP mono-conjugate control. b) TEM images of the samples. From top to bottom, the rows correspond to dimer, trimer and tetramer samples. Scale bar is 50 nm.
a. 1. 2. 3. 4.
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Lane 2 features non-penetrating material indicating the
formation of AuNP assemblies larger than the agarose gel
pore size. Figure 3 b shows subsequent TEM characteriza-
tion of the sample mixture. One-dimensional assemblies of
AuNPs were clearly evident, with their alignment on the grid
into extended arrays attributed to fl uidic forces from sol-
vent droplet removal in the sample deposition proccess. [ 3n ]
These assemblies featured average end-to-end lengths of
0.65 ± 0.22 μ m, in excellent agreement to that measured in
previous work for the unmodifi ed nanotube (0.64 ± 0.24 μ m).
Furthermore, as TEM sample preparation methods are
known to distort and denature DNA-AuNP architectures, the
number of AuNPs found in the assemblies was also counted
as another means to establish a measurement of length for
the structures. This gave an average count of 44 ± 12 AuNPs
per assembly. Given that the rung is ca. 14.3 nm in length, this
equates to nanotube lengths of 0.63 ± 0.17 μ m. Again, this is
in excellent agreement with previously reported values, and
presents strong evidence for the successful formation of one-
dimensional AuNP assemblies via our planned strategy.
For further analysis, the difference between direct meas-
urement of assembly length and indirect measurement via
counting of AuNPs was evaluated for each assembly (Sup-
porting Information, Figure S4). Despite good correlation of
average values, it was found that the two
methods of measurement gave widely
varying values for individual assembly
lengths. This may be explained by the dif-
fering drawbacks behind the two methods
of measurement. For both methods, sample
distortion and denaturation during the
TEM sample preparation process may
affect the measured value. In directly
measuring the lengths of the assemblies
as imaged by TEM, fl uidic forces from sol-
vent droplet removal during sample depo-
sition may extend the nanotube structure,
whereas gold aggregation during sample
drying may contract the nanotube struc-
ture. On the other hand, in measuring the
lengths of the assemblies indirectly through
the number of AuNPs present per assembly,
sample denaturation may cause the loss of
AuNPs within an assembly, whereas gold
aggregation may cause the addition of
non-participating AuNPs to gather around
the one-dimensional assemblies. As the
two methods of measurement have draw-
backs which may occur differently upon
individual assemblies, variance in resultant
measured lengths is to be expected.
As with the assembled discrete struc-
tures, the creation of an interparticle dis-
tance histogram showed that the majority
of interparticle distances observed via
TEM were low, a probable result of AuNP
aggregation during the sample drying pro-
cess (Supporting Information, Figure S5).
The added structural fl exibility introduced
by the 15 bp overhang is particularly evident in the struc-
tural non-linearity between adjacent nanoparticles within
the extended one-dimensional assemblies: in many instances,
regions of particle groupings are observed, while other regions
do not have any particles. This structural effect may be further
compounded by aforementioned sample distortion/denatura-
tion, including the occurrence of AuNP aggregation.
UV-vis spectroscopy of the one-dimensional AuNP
assemblies was performed in order to assess plasmonic prop-
erties. The results are presented in Figure S6 under Sup-
porting Information. The spectrum for sample corresponding
to RCA added to RNG -AuNP conjugates at a 1:1.1 ratio
demonstrated slight broadening of the plasmon resonance
peak in comparison to the rung starting material, as predicted
for plasmonic coupling. [ 2d , 12 ] The absence of a signifi cant red-
shift was not unexpected due to the observed structural fl ex-
ibility of our assemblies. For signifi cant plasmonic coupling
to occur, particle spacings smaller than the particle diameter
are required as coupling strength decays exponentially with
increasing interparticle distance. [ 13 ] Although low interpar-
ticle distances were observed via TEM, a signifi cant portion
of this observation was attributed the propensity for AuNPs
to aggregate during the drying process of sample prepara-
tion, and the nanoparticles are likely characterized by larger
a. 1. 2.
Figure 3. Formation of one-dimensional AuNP assemblies via addition of RCA backbone strand to RNG -AuNP mono-conjugates. a) 2.5% AGE of the assembled structures. Lane 1 corresponds to RNG -AuNP conjugates as the control, and lane 2 to a mixture of RCA added RNG -AuNP at a 1:1.1 ratio allowed to incubate overnight. Non-penetrating material as indicated suggests the formation of large higher order assemblies. b) TEM images of the sample mixture. Scale bar is 500 nm.
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average interparticle distances in solution due to added
structural freedom incurred by the overhang. Furthermore,
this distance likely changes dynamically in solution, there-
fore obscuring discrete spectral changes. We expect that
minor adjustments, such as use of internal dithiol modifi ca-
tions within the rung DNA component strands, will result in a
more rigid structure with smaller interparticle distances and
signifi cant plasmonic coupling, an option we are currently
exploring.
Overall, we have described a new strategy for the facile
preparation of one-dimensional AuNP assemblies. The
strategy is based upon initial mono-conjugation of AuNPs to
relatively large, three-dimensional triangular rung DNA units.
The rung-AuNP conjugate has been shown to controllably
form both small, discrete assemblies of AuNPs, as well as
extended one-dimensional assemblies of AuNPs. The robust
and high purity mono-conjugation yields gold nanoparticle
3D-‘building-blocks’ with the potential to undergo modular
and high yield assembly in one-, two- or three-dimensions.
These structures feature multiple positions for functionaliza-
tion and patterning, and as such, they enable the creation of
a new toolbox of pure and stable gold nanoparticle assem-
blies with potential utility in the fi elds of nanophotonics and
nanoelectronics.
Experimental Section
Materials and Instrumentation : A full list of materials and instrumentation is available under Supporting Information. 1xTBE buffer is composed of 90 m M tris(hydroxymethyl)-aminomethane (Tris) and boric acid, 1.1 m M ethylenediaminetetraacetic acid (EDTA), with a pH of ∼ 8.3. 1xTA buffer is composed of 45 m M Tris, with pH adjusted to 8.0 using glacial acetic acid. 1xTAMg buffer is composed of 45 m M Tris, 7.6 m M MgCl 2 , with pH adjusted to 8.0 using glacial acetic acid. All AuNPs used were prepared via Turkevich-Frens synthesis, with subsequent passivation by bis(p-sulfonatophenyl)phenylphosphine as described in literature. [ 8a ]
RNG Preparation : The DNA triangular rung unit RNG was pre-pared as previously reported. [ 6 ] Briefl y, all component strands were combined in equimolar amounts, with a fi nal concentration of 435 n M in 1xTBE, 100 m M NaCl. This mixture was annealed from 95 °C to 20 °C over 3 to maximize clean product formation (refer to Figure S2 in the Supporting Information).
RNG -AuNP Mono-Conjugate Preparation : RNG was combined in equimolar amounts with 13 nm AuNPs, with a fi nal concentra-tion of 125 n M in 1xTBE, 100 m M NaCl. This mixture was allowed to incubate overnight at room temperature. After incubation, the crude sample mixture was incubated with 4, 7, 10, 13, 16, 19, 22, 25, 32, 35, 38, 41, 44, 47, 50, 53-Hexadecaoxa-28, 29-dithi-ahexapentacontanedioic acid (PEG 7 ) at 30 000x excess for 30 min for further passivation of the AuNPs. [ 10 ] Excess PEG 7 was removed via 3x wash cycles with 1xTAMg using Amicon Ultra 0.5 mL cen-trifugal fi lters (MWCO = 100 kDa, 5 min spin cycles at ∼ 5–6 kRPM).
The crude product was then run on 3% agarose gel in 1xTA at 10 V/cm to allow separation of non-, mono- and di-conjugated AuNP. The desired mono-conjugate product band was excised and electroeluted out, with the collected electroeluted fraction spiked with aqueous MgCl at 76 m M to bring buffer conditions to
1xTAMg. This was concentrated as necessary using Amicon Ultra 0.5 mL centrifugal fi lters (MWCO = 100 kDa). Quantifi cation of the obtained pure RNG -AuNP conjugates was performed via UV-Vis spectroscopy using an extinction coeffi cient ε 450 for 13 nm AuNPs found in literature. [ 14 ]
Experimental details regarding the preparation and further functionalization of modifi ed RNG -AuNP conjugates may be found under Supporting Information.
Assembly of One-Dimensional AuNP Structures : For the prepa-ration of extended assemblies, RCA was combined with RNG -AuNP conjugates at a 1:1.1 ratio and allowed to incubate overnight at room temperature. Prior to this, quantifi cation of RCA was per-formed via binding site titration characterized by gel electropho-resis. [ 6 ] For the preparation of discrete assemblies, RNG -AuNP conjugates were combined with the appropriate backbone strands in theoretical equimolar amounts, and allowed to incubate over-night. Yields were high, but diffi culty in quantifi cation of the RNG -AuNP conjugates and backbone strands due to AuNP polydis-persity and secondary interactions of the 80 bp backbone strands led to imperfect ratios and an impure fi nal product (refer to Figure S7 under Supporting Information). Hence, a purifi cation procedure similar to that described above for the RNG -AuNP conjugates was employed. This step could be omitted if desired by titrating the backbone strands with RNG -AuNP to fi nd a true 1:1 stoichiometry. Purifi cation of an impure fi nal product was found to be preferable with regard to total preparation time required and economy of the RNG -AuNP conjugates.
Supporting Information
Supporting Information is available from the Wiley Online Library or from the author.
Acknowledgements
The authors thank NSERC, CIFAR and FQRNT for funding. H. F. S. is a Cottrell Scholar of the Research Corporation.
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Gold Nanoparticle 3D-DNA Building Blocks
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Received: May 21, 2013Revised: July 12, 2013Published online:
small 2013, DOI: 10.1002/smll.201301562