Alessia Amodio1, Abimbola Feyisara Adedeji2,3, Matteo Castronovo2,3,4, Elisa Franco5, Francesco Ricci1. 1. Department of Chemistry, University of Rome , Tor Vergata, Via della Ricerca Scientifica, 00133 Rome, Italy. 2. PhD School of Nanotechnology, Department of Physics, University of Trieste , Via Valerio 2, 34127 Trieste, Italy. 3. Department of Medical and Biological Sciences, University of Udine , Piazzale Kolbe 4, 33100 Udine, Italy. 4. School of Food Science and Nutrition, University of Leeds , Leeds LS2 9JT, U.K. 5. Department of Mechanical Engineering, University of California , Riverside, California 92521, United States.
Abstract
We demonstrate a strategy to trigger and finely control the assembly of supramolecular DNA nanostructures with pH. Control is achieved via a rationally designed strand displacement circuit that responds to pH and activates a downstream DNA tile self-assembly process. We observe that the DNA structures form under neutral/basic conditions, while the self-assembly process is suppressed under acidic conditions. The strategy presented here demonstrates a modular approach toward building systems capable of processing biochemical inputs and finely controlling the assembly of DNA-based nanostructures under isothermal conditions. In particular, the presented architecture is relevant for the development of complex DNA devices able to sense and respond to molecular markers associated with abnormal metabolism.
We demonstrate a strategy to trigger and finely control the assembly of supramolecular DNA nanostructures with pH. Control is achieved via a rationally designed strand displacement circuit that responds to pH and activates a downstream DNA tile self-assembly process. We observe that the DNA structures form under neutral/basic conditions, while the self-assembly process is suppressed under acidic conditions. The strategy presented here demonstrates a modular approach toward building systems capable of processing biochemical inputs and finely controlling the assembly of DNA-based nanostructures under isothermal conditions. In particular, the presented architecture is relevant for the development of complex DNA devices able to sense and respond to molecular markers associated with abnormal metabolism.
In Nature,
several vital cellular
tasks, such as the formation of the cell membrane or of stable host–guest
complexes, rely on thermodynamically driven molecular assembly processes
based on relatively weak interactions.[1] The assembly of such complexes is usually finely controlled by a
series of biological inputs and molecular cues.[2] Inspired by this observation, researchers in the field
of supramolecular chemistry have exploited non-covalent interactions
to achieve controlled self-assembly of synthetic moieties and to build
complex nanostructures of defined geometries.[1,3] Because
of its predictable base-pairing interactions and its low synthesis
cost, DNA represents one of the best biomaterials to design and assemble
complex structures with nanoscale features. Such structures have reached
a level of complexity that would have been impossible to imagine 20
years ago: using synthetic DNA oligonucleotides, we can now build
2D and 3D nanoscale objects with virtually arbitrary shape.[4,5] Input-responsive DNA assemblies, engineered to exhibit functional
dynamic behaviors such as opening and closing or moving in response
to biochemical inputs, have been also built.[6]One of the current limitations of responsive DNA nanostructures
is that responses are generally encoded in the structure itself (for
instance, via input-responsive domains or aptamers) and can be modulated
exclusively as a function of the input concentration or intensity.
For example, DNA nanofabrication has been controlled directly using
small synthetic ligands or light irradiation.[7,8] Finer
control of assembly is desirable in many applications, such as sensing,
metabolic engineering,[9] or nanomanufacturing.
This limitation can be mitigated by using input-triggerable DNA strand
displacement circuits to control assembly.[10] Here, we demonstrate the viability of this approach with a pH-controlled
DNA catalytic circuit to control the assembly of DNA-based nanostructures.We focus on DNA structures self-assembling from DNA tiles, one
of the best-characterized approaches to build scalable DNA architectures.[11,12] In this strategy, DNA strands are designed to form rigid building
blocks, called tiles (Supporting Information (SI), Figure SI1), that can self-assemble into lattices, ribbons,
or tubular structures through single-stranded overhangs. DNA tile
assembly can be triggered by an upstream DNA strand displacement circuit:[10] inactive (protected) DNA tiles can be activated
(deprotected) by the output of a DNA catalytic circuit,[13] which is in turn triggered by a DNA catalyst
molecule. This approach allows the isothermal assembly of DNA nanostructures,
achieving control of the composition and timing of the process.[14,15]To achieve pH-controlled, circuit-tunable assembly of DNA
nanostructures,
we re-engineered a DNA strand displacement catalytic circuit (Figure ) to be responsive
to pH, and we used it to direct a well-known DNA tile self-assembly
process based on double-crossover tiles (Figure SI1). pH control is achieved by taking advantage of the well-characterized
pH sensitivity of triplex DNA, which requires the protonation of the
N3 of cytosine in the third strand to form (average pKa of cytosines in triplex structure is ∼6.5).[16] Specifically, we designed a pH-dependent substrate
(Figure , purple strand)
that prevents the strand displacement reaction with the catalyst strand
(C) at acidic pH, due to the formation of Hoogsteen interactions in
addition to the Watson–Crick base-pairings. Only at basic pHs
(when Hoogsteen interactions are destabilized) is the accessibility
of the DNA substrate, needed for enabling such strand displacement
circuit, restored. In turn, tile assembly can occur efficiently upon
catalyst addition (Figure , right) under these pH conditions.
Figure 1
pH-controlled self-assembly
of DNA tiles. We have achieved pH-controlled
DNA tile assembly by coupling an upstream re-engineered pH-controlled
circuit with a downstream DNA tile self-assembly process. (1) In the
pH-dependent upstream circuit, a catalyst (C) binds to a pH-dependent
substrate, leading to the release of a deprotector strand (D). (2)
The D strand, in turn, activates a downstream self-assembly reaction
by irreversibly associating with a protected tile (PT). This leads
to reactive double-crossover tiles (RT) self-assembling into lattices
and nanotubes (right). The pH-dependent substrate is implemented with
a clamp-like triplex-forming DNA strand (T) that, under acidic pHs,
can form a triplex complex, inhibiting the strand displacement reaction
with the catalyst.
pH-controlled self-assembly
of DNA tiles. We have achieved pH-controlled
DNA tile assembly by coupling an upstream re-engineered pH-controlled
circuit with a downstream DNA tile self-assembly process. (1) In the
pH-dependent upstream circuit, a catalyst (C) binds to a pH-dependent
substrate, leading to the release of a deprotector strand (D). (2)
The D strand, in turn, activates a downstream self-assembly reaction
by irreversibly associating with a protected tile (PT). This leads
to reactive double-crossover tiles (RT) self-assembling into lattices
and nanotubes (right). The pH-dependent substrate is implemented with
a clamp-like triplex-forming DNA strand (T) that, under acidic pHs,
can form a triplex complex, inhibiting the strand displacement reaction
with the catalyst.The designed upstream
pH-dependent circuit can be finely controlled
with pH. To demonstrate this, we have characterized in isolation the
pH-dependent strand displacement circuit by using an external, optically
labeled reporter (R) that stoichiometrically reacts with the liberated
deprotector strand (D) (Figure a). We first characterized the pH dependency of the substrate
complex by employing a triplex-forming strand (T) (responsible for
the substrate formation) labeled with a fluorophore and a quencher
(Figure b, left).
This allowed us to monitor the folding and unfolding of the triplex
structure at different pHs (Figure b, right). As expected, under acidic pHs (favoring
triplex formation) a low fluorescence signal is observed, suggesting
folding of the triplex complex. Upon increasing the solution’s
pH, the fluorescence signal increases, consistent with the destabilization
of Hoogsteen interactions (Figure b, right). The pH of semiprotonation (the average pKa due to several interacting protonation sites)
for this triplex complex is 7.5, which is in agreement with previous
observations of similar triplex-forming sequences.[16,17]
Figure 2
(a)
Upstream pH-dependent DNA circuit. (b) Triplex formation in
the pH-dependent substrate complex, studied by incorporating a pH-insensitive
FRET pair at the ends of the clamp-like triplex-forming strand (left)
and measuring the fluorescence signal at different pHs (right). Stable
triplex formation is observed only at pHs below 7.0. (c) The pH-dependent
triplex complex in the substrate inhibits strand displacement reaction
upon C addition (pH 5.0, left). At basic pHs the destabilization of
Hoogsteen interactions leads to substrate activation, which allows
strand displacement reaction in the presence of catalyst strand (C)
(pH 8.0, right). (d) The pH dependence of the catalyst/substrate reaction
can be finely controlled at different pHs. Here, strand displacement
reaction is followed by fluorescence measurements in a solution containing
the pH-dependent substrate (10 nM), the fuel strand (F) (20 nM), and
an external, optically labeled reporter (30 nM) (see experimental
details in the SI) that stoichiometrically
reacts with the released D to give a fluorescence signal. The catalyst
was added at a high concentration (30 nM) to better highlight the
pH dependence of the circuit. All experiments were performed in a
TAE 1x buffer + 15 mM MgCl2 at 25 °C with the pH adjusted
using small aliquots of HCl (1 M) and NaOH (1 M). Error bars here
and in the following figures represent the average and standard deviations
(average RSD = 6%) of three independent measurements.
(a)
Upstream pH-dependent DNA circuit. (b) Triplex formation in
the pH-dependent substrate complex, studied by incorporating a pH-insensitive
FRET pair at the ends of the clamp-like triplex-forming strand (left)
and measuring the fluorescence signal at different pHs (right). Stable
triplex formation is observed only at pHs below 7.0. (c) The pH-dependent
triplex complex in the substrate inhibits strand displacement reaction
upon C addition (pH 5.0, left). At basic pHs the destabilization of
Hoogsteen interactions leads to substrate activation, which allows
strand displacement reaction in the presence of catalyst strand (C)
(pH 8.0, right). (d) The pH dependence of the catalyst/substrate reaction
can be finely controlled at different pHs. Here, strand displacement
reaction is followed by fluorescence measurements in a solution containing
the pH-dependent substrate (10 nM), the fuel strand (F) (20 nM), and
an external, optically labeled reporter (30 nM) (see experimental
details in the SI) that stoichiometrically
reacts with the released D to give a fluorescence signal. The catalyst
was added at a high concentration (30 nM) to better highlight the
pH dependence of the circuit. All experiments were performed in a
TAE 1x buffer + 15 mM MgCl2 at 25 °C with the pH adjusted
using small aliquots of HCl (1 M) and NaOH (1 M). Error bars here
and in the following figures represent the average and standard deviations
(average RSD = 6%) of three independent measurements.pH-dependent triplex formation in the substrate
of the downstream
catalytic network allows rational control of the output concentration
by simply changing the solution’s pH. At pH 5.0, which is acidic
enough for clamp-like strand to form an inactive triplex complex,
the addition of the catalyst strand (C) results in no significant
fluorescence change (Figure c, left). This suggests that the circuit is fully suppressed.
At pH 8.0, which inhibits triplex formation, strand displacement successfully
proceeds with fast kinetics upon C addition (Figure c, right). The activation level of the circuit
can be modulated by changing the pH of the solution (Figures d and SI2) or the C concentration (Figure SI3). However, probably due to the presence of the triplex-forming sequence,
the circuit catalytic efficiency is poorer than previously reported
(Figure SI4).[10] At high C concentration, the complete circuit converts the gradual
pH dependency shown in Figure b into a digital-like response; in contrast, at low C concentration,
the circuit response remains gradual. A control experiment involving
a pH-independent substrate where the triplex-forming portion has been
substituted with a random sequence unable to form a triplex structure
shows no effect of pH over the entire pH range explored, and over
a wide range of C concentrations (Figure d, right, gray dots; Figures SI5, SI6, and SI7).The pH-controlled DNA catalytic
circuit can be used to direct the
assembly of DNA nanostructures using pH. To do this we have interconnected
the above-characterized pH-dependent circuit with a DNA tile self-assembly
process.[10,11a,11b,12] Fluorescence microscopy images (Figure , top) and AFM images (Figure , center) confirm
that tiles assemble only at neutral/basic pHs, while no assemblies
are observed over the same reaction time at acidic pHs (pH 5.0 and
6.0). Tile assembly largely yields tubular structures according to
fluorescence microscopy and AFM images. As a control experiment we
used a pH-independent substrate and observed assembly of DNA tiles
in the entire pH range investigated (Figure , bottom). Moreover, statistical analysis
shows that the length and yield of nanotubes formed with the pH-dependent
substrate under basic conditions (average length = 0.91 μm and
yield = 23 ± 10%, at pH 8.0) is comparable to those of the control
pH-independent substrate at both pH 8.0 (length = 0.75 μm and
yield = 12 ± 6%) and 5.0 (length = 0.79 μm and yield =
19 ± 12%) (see SI for experimental
details and Figure SI8). As a further demonstration
that pH does not affect the downstream tile assembly reaction, we
have exogenously added D to a solution containing protected tiles
and observed pH-independent tile assembly (Figure SI9). Conversely, the absence of C leads to no formation of
nanotubes (Figure SI10).
Figure 3
pH-dependent self-assembly
of DNA tiles. (Top) The upstream, pH-dependent
DNA circuit coupled with a downstream tile self-assembly process (Figure ) allows to control
DNA tile self-assembly with pH. At acidic pHs (pH 5.0 and 6.0) no
formation of assemblies is observed with optical fluorescence microscopy.
By increasing the pH of the solution (pH 7.0 and 8.0) we achieve evident
formation of DNA lattices. (Center) pH-dependent lattices were also
imaged with atomic force microscopy (AFM). (Bottom) A control experiment
using a pH-independent substrate (unable to form a pH-dependent triplex
structure (Figure SI5)) leads to pH-independent
assembly of DNA tiles. All the experiments shown here and in Figure 4 were performed using the following concentrations
of reagents: protected tile (PT), 200 nM; fuel (F), 440 nM; pH-dependent
substrate or control substrate, 220 nM; and catalyst (C), 20 nM. The
assembly was achieved in TAE 1x buffer + 15 mM MgCl2, at
25 °C with the pH adjusted using small aliquots of HCl (1 M)
and NaOH (1 M). For all the fluorescence microscopy experiments, a
cy3-labeled tile central strand (t4, see SI) was used to detect nanotubes formation. AFM images of the pre-adsorbed
nanostructures on freshly cleaved mica (see SI) were obtained with AC mode in TAE 1x buffer + 15 mM MgCl2 buffer, with 1 Hz scan rate, 256 pixel × 256 pixel image definition
and processed with second-rder flattening.
pH-dependent self-assembly
of DNA tiles. (Top) The upstream, pH-dependent
DNA circuit coupled with a downstream tile self-assembly process (Figure ) allows to control
DNA tile self-assembly with pH. At acidic pHs (pH 5.0 and 6.0) no
formation of assemblies is observed with optical fluorescence microscopy.
By increasing the pH of the solution (pH 7.0 and 8.0) we achieve evident
formation of DNA lattices. (Center) pH-dependent lattices were also
imaged with atomic force microscopy (AFM). (Bottom) A control experiment
using a pH-independent substrate (unable to form a pH-dependent triplex
structure (Figure SI5)) leads to pH-independent
assembly of DNA tiles. All the experiments shown here and in Figure 4 were performed using the following concentrations
of reagents: protected tile (PT), 200 nM; fuel (F), 440 nM; pH-dependent
substrate or control substrate, 220 nM; and catalyst (C), 20 nM. The
assembly was achieved in TAE 1x buffer + 15 mM MgCl2, at
25 °C with the pH adjusted using small aliquots of HCl (1 M)
and NaOH (1 M). For all the fluorescence microscopy experiments, a
cy3-labeled tile central strand (t4, see SI) was used to detect nanotubes formation. AFM images of the pre-adsorbed
nanostructures on freshly cleaved mica (see SI) were obtained with AC mode in TAE 1x buffer + 15 mM MgCl2 buffer, with 1 Hz scan rate, 256 pixel × 256 pixel image definition
and processed with second-rder flattening.
Figure 4
Kinetics
of pH-dependent self-assembly of DNA tiles. The self-assembly
of DNA tiles was followed by AFM images at different time intervals.
No tile assembly is observed within the time frame of the experiment
at pH 5.0. In contrast, at basic pH (pH 8.0), DNA lattices can be
clearly observed just 15 min after catalyst addition. See Figure caption for experimental
details.
The kinetics of DNA tile assembly was studied with AFM. Images
derived from the reaction samples (upstream pH-dependent circuit +
protected tiles) at different intervals after the addition of the
catalyst strand were obtained. No tiles assembly at pH 5.0 (Figure , top) and pH 6.0 (Figure SI11)
was observed during the entire time frame investigated. At pH 8.0
a substantial amount of assembled tiles can be observed within 30
min after catalyst addition (Figure , bottom). We note that assembly of small lattices
at pH 5.0 was observed under AFM after 4 days since the start of the
reaction, presumably due to leak of the deprotector from the substrate
(Figure SI12).[10]Kinetics
of pH-dependent self-assembly of DNA tiles. The self-assembly
of DNA tiles was followed by AFM images at different time intervals.
No tile assembly is observed within the time frame of the experiment
at pH 5.0. In contrast, at basic pH (pH 8.0), DNA lattices can be
clearly observed just 15 min after catalyst addition. See Figure caption for experimental
details.In this work we have demonstrated
a modular architecture to regulate
the self-assembly of DNA nanostructures with the sole change of pH.
We did so by integrating an upstream pH-dependent strand displacement
circuit into an already-characterized, downstream DNA tile self-assembly
process. Our architecture is potentially relevant in biomedical applications
of DNA nanotechnology. For example, pH disregulation is a hallmark
of several diseases,[18] including cancer.
The availability of pH-triggerable DNA nanostructures will have intriguing
potential applications in drug delivery research.[19] Moreover, because we have recently demonstrated that the
pH dependence of triplex DNA could be finely regulated by simply changing
the relative content of TAT vs CGC triplets in the triplex-forming
sequence,[16b] we anticipate the possibility
of programming the assembly of different DNA nanostructures at different
pH thresholds. Finally, many enzymes are known that catalyze either
proton-producing or proton-consuming reactions.[20] Therefore, different enzymes and enzymatic substrates could
be used as molecular, functional inputs to control the isothermal
assembly of DNA nanostructures.The approach described here
could also be expanded to consider
a wider range of molecular inputs controlling the self-assembly of
supramolecular structures. In fact, apart from pH, it is in principle
possible to engineer upstream DNA strand displacement circuits activated
by the presence of proteins, antibodies, or other relevant biomolecular
inputs so that the downstream self-assembly process is input-specific.
In principle, logic or dynamic circuits could replace the catalytic
network we considered, providing the system with expandable signal-processing
capacity. Finally, because strand displacement circuits can be designed
to be highly specific and to respond orthogonally to a specific input,
it would be possible to control the simultaneous assembly of different
structures using multiple inputs in a highly programmable fashion,
thus leading to a better temporal and spatial regulation of the assembly
processes.
Authors: Haorong Chen; Te-Wei Weng; Molly M Riccitelli; Yi Cui; Joseph Irudayaraj; Jong Hyun Choi Journal: J Am Chem Soc Date: 2014-05-02 Impact factor: 15.419
Authors: Sadao Takabayashi; Shohei Kotani; Juan Flores-Estrada; Elijah Spears; Jennifer E Padilla; Lizandra C Godwin; Elton Graugnard; Wan Kuang; Scott Sills; William L Hughes Journal: Int J Mol Sci Date: 2018-08-24 Impact factor: 5.923