Abstract
Complex structures and devices, both natural and manmade, are often constructed sequentially. From crystallization to embryogenesis, a nucleus or seed is formed and built upon. Sequential assembly allows for initiation, signaling, and logical programming, which are necessary for making enclosed, hierarchical structures. Although biology relies on such schemes, they have not been available in materials science. Here, we demonstrate programmed sequential self-assembly of DNA functionalized emulsions. The droplets are initially inert because the grafted DNA strands are pre-hybridized in pairs. Active strands on initiator droplets then displace one of the paired strands and thus release its complement, which in turn activates the next droplet in the sequence, akin to living polymerization. Our strategy provides time and logic control during the self-assembly process, and offers a new perspective on the synthesis of materials.
Natural complex systems are often constructed by sequential assembly but this is not readily available for synthetic systems. Here, the authors program the sequential self-assembly of DNA functionalized emulsions by altering the DNA grafted strands.
Introduction
Over the past decade, there has been growing interest in using colloids for the self-assembly of arbitrarily designed structures1–4, rather than the more conventional colloidal crystals fabricated over the past century5–8. Colloidal particles with specific interparticle recognition facilitated by their functionalization with DNA sticky ends9–11, lock and key interactions12, as well as particles of different shapes and symmetrically arranged patches13, 14, have led to theoretical proposals for the creation of demonstrative target structures, e.g., a colloidal version of the Empire State building4. Such proposals rely on self-assembly through tunable enthalpic and entropic interactions guiding the system toward thermodynamic equilibrium. In addition, introducing mobile linkers to colloids15, liposomes16, 17, and droplets18–20 avoids kinetic traps along the self-assembly pathways. However, the design principle that invokes sequential self or directed assembly has not yet been addressed due to the absence of an underlying technology. Sequential assembly is used industrially to make everything from integrated circuits to skyscrapers and is required in the growth of all living organisms. In many cases, it is a convenient organizational tool, in others, such as the three-dimensional enclosed structures of the Russian dolls, it is necessary to assemble the inside before the outside.
In this article, we demonstrate a technique for programmed self-assembly on the colloidal scale using the specific hybridization and easy design properties of DNA sequences21. Related schemes have been shown on molecular scales using DNA duplexes or DX motifs22–24. In our system, a family of diversely functionalized emulsion droplets… B, C, D,… are self-assembled such that C only binds to D after B binds to C. This process is controlled by using protected pairs of DNA strands on the droplets and a well-developed technology, toehold strand displacement25–27, as the enabling mechanism. With A as an initiator and E as a termination droplet, we spell out a droplet sequence ABCDE.
Results
Experimental design
In our design, we graft mobile DNA linkers to micro-scaled emulsion droplets, as depicted in Fig. 1a. In step 1, a set of droplets B and C have been prepared with pairs of DNA strands that are protected by their partial hybridization. In practice, each droplet has tens of thousands of such pairs. The protection renders the droplets inert—no bonds are formed between protected droplets. The complementary orange DNA sequences on B are hybridized and protected from the unpaired orange sequence on C. Similarly, the paired yellow sequences on C are protected from the unpaired yellow DNA strand on B. In step 2, an initiator droplet, A, is introduced. The DNA sequence on A has a section that is complementary to the unpaired red sequence and half of the paired orange sequence on B. Following the scheme of the toehold strand displacement mechanism (Fig. 1b), the complementary red sequences and half of the orange sequence bind by the DNA strand-branch migration. With proper sequence design, the remaining half of the originally hybridized yellow sequence is above its melting temperature and unbinds. Droplet A and B are then bound and the orange yellow DNA single strand is left unbound. If it were attached to a solid colloidal particle, it would be localized to the region near the A–B binding site. However, on an emulsion droplet, it is free to diffuse over the entire droplet surface, as shown in step 3 of Fig. 1a. Droplet B is then activated and can serve as an initiator for binding and activation of droplet C.
DNA functionalized droplets are different from similarly functionalized colloids in several ways related both to the mobility of the DNA ligands and the deformability of the droplets28–31. When droplets approach, a few DNA strands on one droplet can hybridize with complementary strands on the other droplet making an initial bond. However, surface diffusion allows additional DNA strands to migrate to the contact region to form additional hybridized bonds and a growing patch. The patch flattens the interface between the droplets at the cost of elastic energy (surface tension). The balance between the hybridization energy and the elastic energy gives rise to an equilibrium patch size with a given number of strands, N s. If the number of DNA strands on a droplet is less than or equal to the equilibrium N s, then the droplet should be monovalent and binds to only one other droplet. In the present case, we use a low concentration of initiator strands and a low volume fraction of droplets to ensure that we are in the monovalent regime for each binding event. The number of released strands must be less than or equal to the number bound in each previous step in the sequence.
As a demonstration of sequential assembly, we choose a simple design—a set of droplets each labeled with a unique color. The designed sequence of events is shown in Fig. 2a. Droplet A is the initiator, while droplets B, C, D have protected pairs of DNA strands, and droplet E is a terminator with single DNA strand protected in a hairpin configuration. The sequences for the active regions of A–E droplets are shown in Fig. 2b. Droplets B, C, D, and E are prepared separately and then added to the same bath, since they are inert. When the initiator droplets A are added, we begin to see the sequential assembly of droplets binding, illustrated in Fig. 2a, and the corresponding strand displacement reactions in Fig. 2b. The system forms dimers, trimers, tetramers, and pentamers in the correct color order (and nothing longer).
Gel electrophoresis
Our sequential assembly scheme relies on the stability of the protected strand pairs and the effectiveness of strand displacement. These properties were tested by a series of experiments on the individual strands before attachment to the emulsion droplets. (Note that each single strand illustrated in Fig. 2b is attached to a 36 nucleotide spacer strand, which can be hybridized to a complementary strand to make a duplex spacer with a biotinylated end allowing both attachment to a fluorescent streptavidin and separation of the active region from the droplet surface.) In Fig. 2c, we show a non-denaturing gel study verifying the protections and reactions between sequences depicted in Fig. 2b. Lane S0 indicates the band for strand S0 and serves as a reference for the single strands S2, S4, and S6 with similar molecular weight. Similarly D1 is a reference for bands D2 and D3 (completely hybridized duplex strands), L1 is a reference for L2 and L3 (partially hybridized strands), while S7 and D4 mark the terminator hairpin strand and its partially hybridized duplex strands. Lanes S0 + L1 → D1 + S2, S2 + L2 → D2 + S4, S4 + L3 → D3 + S6, and S6 + S7 → D4 show that the reactions depicted in Fig. 2b produce the desired results and leave none of the initial reactants. Lane L1 + L2 + L3 + S7 shows that the partially hybridized protected strand pairs do not react in the absence of the initiator. On the other hand, the final lane shows that when the initiator strand is added to the previously inert protected strands, the complete set of reactions goes to completion with only complete duplex strands and the partially hybridized termination duplex strands as the result.
DNA functionalization
Having confirmed the success of the molecular scheme, we next functionalize the droplets to drive their polymerization. The experiments are performed with micron-sized, lipids stabilized silicone oil in water emulsion droplets (see methods). DNA loops (L1, L2, and L3) are pre-annealed and purified from native gels to ensure the correct stoichiometry. A ‘biotinylated phospholipid—fluorescent streptavidin—biotinylated oligonucleotide’ linking strategy is applied to functionalize the oil droplets with the corresponding DNA structures (S0, L1, L2, L3, and S7). In the experiment, each combination of streptavidin with different fluorescent labels is specifically associated with one type of DNA strand/loop structure to distinguish them using fluorescence confocal microscopy. From fluorescence spectroscopy measurements, we estimate that the surface coverage of streptavidin on droplets is ~ 1000 μm−2 (Supplementary Methods and Supplementary Fig. 3).
Confocal imaging and data analysis
After DNA functionalization, the droplets are mixed together at a number ratio of A:B:C:D:E = 1:2:2:2:2, and loaded into a homemade sample chamber (Supplementary Methods). The droplets cream to the top surface forming a monolayer, and diffuse thermally. The chamber was placed on a leveled surface in an incubator at 12 °C. The sample is imaged using fluorescence confocal microscopy (Leica TCS SP5 II) at different time points. Confocal images demonstrate the growth of sequential clusters with initiators (Fig. 3a–d and Supplementary Figs. 3–7) and a control without initiator (Fig. 3e). The control shows little aggregation after 101 h with ~ 87% of the droplets staying unbound. The experiments with initiators show the droplets first self-assemble into dimers, then trimers, tetramers, and finally pentamers (Fig. 3f–i). Figure 4 quantifies these results showing that, in the presence of the initiators, by 101 h the dominant population (35% of the initiators) is the programmed pentamer in the correct sequence, and 94% of the initiators have been used up. Another analysis (Fig. 4 inset) indicates that initiated sequential bindings formed in the system are six times more than the number of mistakes (uninitiated bindings or bindings in the wrong sequence). Among the initiated sequential bindings, 73% are in linear regime (only one predecessor and one successor) and 27% in branched regime (multiple predecessors or successors). At present, the control of monovalent binding is less than perfect. Reducing the DNA surface density on droplets will further optimize our system, leading to a higher yield of linear chains.
Kinetics model for the sequential self-assembly
The time scale for these reactions is governed by the aggregation kinetics of monolayer DNA-coated droplets on a surface as studied in ref. 32. The aggregation time τ can be obtained from:
1 |
where
2 |
τ R is the reaction time of a pair of droplets with complementary sticky-end DNA on their surfaces staying within the reaction region (thickness L ~ 10 nm). C 0 is the number density of droplets of one particular type, ~ 3 × 102 mm−2 for droplet A and ~ 6 × 102 mm−2 for droplets B, C, D, and E. R d is the average radius of the emulsion droplets, ~ 2.35 μm; D 0 is the measured two dimensional diffusion coefficient of droplets, ~ 0.037 μm2 s−1. Our system is reaction limited with τ DLA ~ 0.5 h and the rate of DNA-coated droplet binding (the second term in the right hand side of Equation 1) ~ 0.2–2 h for the initiator reaction and ~ 2–20 h for the subsequent reactions (Supplementary Note 1). For hybridization to occur, the accumulated contact time for a pair of strands to be hybridized is ~1 s. Strands diffuse on the droplet surface quickly and make contact many times before binding from one droplet to another. Thus, τ R depends on the diffusion coefficient and density of active DNA on the droplet surface. For the initiator, the number of active strands is measured by fluorescence to be ~ 12,000, corresponding to a strand density ~ 200 per μm2. The kinetic model allows us to estimate the number of released strands from the adhesion patch to be ~ 1200 or 20 μm−2 in order to match the observed assembly time scales demonstrated in Fig. 4. To test the robustness of our system, the experiment is carried out using another batch of smaller droplets (3.4 μm) with higher diffusion coefficient (0.08 μm2 s−1). The results present a similar yield (Supplementary Tables 3 and 4) and assembly kinetics (Supplementary Fig. 8), which have also been confirmed by theoretical calculation (Supplementary Note 1).
Discussion
We have demonstrated a technique and developed a simple system to allow for the sequential assembly of micron-scale objects. The experimental parameters, such as temperature, DNA sequences, droplet density, size, and grafting chemistry can be optimized for faster growth, error reduction or increasing/decreasing branching. For instance, we can use a longer duplex in the loop structures for added stabilization, which should minimize uninitiated binding. We could also improve our yield through magnetic or surface tethered initiators, allowing us to remove the unreacted monomers and non-specific clusters. This method can be further extended in many directions. Programmed sequential self-assembly can produce stable non-equilibrium structures similar to the directed sequential growth achieved by molecular beam epitaxy33. A cyclic system, IABCABCABC… where the released strand on C is the same as the initiator strand would allow for an extended structure and a true emulsion analog to living polymerization. The linear chains can be folded into two or three-dimensional structures by coating surfaces with several different species of DNA, which can later be turned on chemically or by cooling. An initiator or subsequently freed strand can bind to release more than one type of strand in the next sequence step (by using the same protection strand on two partially different sequences or protecting two strands with one). This would allow control of branching and/or the direct construction of three-dimensional objects. Conversely, two or more initiator strands could be required to bind to and activate a droplet. Lipid coatings on colloidal particles enable mobility on their surfaces15, and thus serve as an extension of our technique to solid particles. Logic and sequence control should greatly expand the range of structures and devices accessible to colloidal/emulsion self-assembly.
Methods
Droplet fabrication
In the experiment two batches of droplets with different sizes were used. They were made via different methods. The 4.7 μm droplets: 5 ml of silicone oil (viscosity = 50 cst, from Sigma Aldrich) was extruded through a membrane with a mean pore size of 1 μm using a membrane emulsification device (internal pressure type micro kit, SPG Technology Co., Ltd). The droplets were stored in a 10 mM sodium dodecyl sulfate (SDS) buffer at 4 °C after two cycles of washes. The average diameter was 4.7 μm. The 3.4 μm droplets34: 5 ml of DMDES was vortexed with 500 μl of deionized water for 5 min, then left on a rotator for 30 min until the mixture was homogeneous. We then mixed a solution of 6% v/v prehydrolyzed DMDES and 20% v/v ammonia (total volume was 35 ml), and vortexed for 5 min. The droplets were left to grow undisturbed for 24 h, until the droplets were monodisperse and ~1.75 μm in diameter. After growth, we dialyzed the droplet solution against a 1 mM SDS solution until all traces of ammonia were removed. We then restarted the reaction by adding 1.5 ml of prehydrolyzed DMDES and 1% v/v ammonia. The PDMS droplet seeds were left to grow undisturbed until their growth had saturated. More prehydrolyzed DMDES was added until the droplets had reached the desired diameter. These droplets were again dialyzed against a 1 mM SDS solution until all unreacted monomer and ammonia were removed, and then stored in a 10 mM SDS buffer at 4 °C until the droplets were ready to be labeled with lipids.
Phospholipids labeling
We used different methods to functionalize the two batches of droplets with phospholipids. For the 4.7 μm droplets: egg l-α-phosphatidylcholine lipids and DSPE-PEG (2000) biotin (both from Avanti Polar Lipids) were mixed at a molar ratio of 95:5, and evaporated under filtered nitrogen. The dried phospholipids were then dissolved in dimethyl sulfoxide (Sigma Aldrich) to 100 g l−1, and further diluted in a 10 mM Tris-HCl, pH 8, 1 mM SDS, 0.1 mM NaN3 buffer to 1 g l−1. The lipids buffer was then added to the creamed emulsion droplets at a volume ratio of 1000 μl:100 μl. Then the mixture was diluted to 10 ml using the same buffer, and tumbled gently at room temperature overnight. The emulsion was washed three times using the TMS buffer (10 mM Tris-HCl, pH 8, 3 mM MgCl2, 1 mM SDS, 0.1 mM NaN3) and then stored at 4 °C for further use. These emulsions are stable for several months. For the 3.4 μm droplets: DSPE-PEG (2000) (1,2-distearoyl-sn-glycero-3-phosphoethanolamine-N-[amino(polyethylene glycol)-2000]) and DSPE-PEG (2000) biotin (both dissolved in chloroform) were mixed at a 20:1 molar ratio. Approximately 10 μl of this lipid mixture (10 g l−1 in chloroform) was added to a clean glass vial. We then evaporated off all chloroform with nitrogen, and resuspended the lipid cake in 70 μl of dimethyl sulfoxide (Sigma Aldrich). To this mixture, we added 1 ml of 10 mM sodium acetate buffer (pH 5), 1 mM SDS, 1 mM EDTA. Then, 50 μl of creamed emulsion droplets were added in this solution, and left to incubate on a rotator for 24 h. The droplets were then washed three times in a 10 mM Tris-HCl pH 8, 1 mM Tergitol TMN-6, 1 mM EDTA buffer to remove any unattached lipids. Lipid-functionalized droplets were stored at 4 °C until ready to be complexed with streptavidin and DNA.
DNA sequence
All the sequences were generated using the program Uniquimer and were purchased from Integrated DNA Technology, Inc (www.idtdna.com). The biotinylated CS strands (Btn-CS) were HPLC purified. The strands S0–S7 and PolyT were purified by denaturing PAGE. Below are the sequences:
Btn-CS: CATCGAACAATCCGGTCGAGTGCCATGATTTGTGAG/3BioTEG/
PolyT: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGTTTTTTTTTTT
S0: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGCGTGACGTAAGTGGT
S1: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGACCACTTACGTCACGAAGAG
S2: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGCGTAGCTCTTCGTGA
S3: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGTCACGAAGAGCTACGATGCT
S4: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGGGTTCAGCATCGTAG
S5: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGCTACGATGCTGAACCTTCCT
S6: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGTTTTTAGGAAGGTTC
S7: CTCACAAATCATGGCACTCGACCGGATTGTTCGATGGAACCTTCCTAAAAAGCAAATTTTTTTTTGCTTTTTAG
Native polyacrylamide gel electrophoresis
The gel demonstrating results of the toehold strand displacement reactions was a 10% native gel. It was prepared in 1 × TAE/Mg++ buffer (20 mM Tris-HCl, pH 7.5, 2 mM EDTA, 6.25 mM Mg++, pH = 7.6). The DNA structures were annealed following a standard protocol: heating at 95 °C for 5 min followed by cooling to room temperature over ~2.5 h. The gel was run on a Hoefer SE-600 gel electrophoresis unit at 7 V cm−1 for 5 h at 12 °C, post-stained with 0.5 μg ml−1 ethidium bromide, and visualized by UV transillumination.
DNA functionalization
Overall, 50 pmol DNA loop structures L1, L2, and L3 (native gel-purified), 100 pmol initiator strand S0 and 100 pmol hairpin strand S7 were separately annealed with an equimolar amount of biotinylated complementary strands in the magnesium buffer (TMS buffer for the strands functionalized on 4.7 μm droplets; TMT buffer: 10 mM Tris-HCl pH 8, 4 mM MgCl2, 1 mM Tergitol TMN-6, 0.1 mM NaN3 for the strands functionalized on 3.2 μm droplets, same in the following steps). Then different combinations of fluorescent streptavidin were added to the DNA solutions at a ratio of 1 streptavidin molecule: 1 biotin group. For the streptavidin added to S0: 100% were labeled with Alexa® Fluor 647; L1: 67% Alexa® Fluor 647 and 33% Alexa® Fluor 488; L2: 33% Alexa® Fluor 647 and 67% Alexa® Fluor 488; L3: 100% Alexa® Fluor 488; S7: 100% Alexa® Fluor 546. Meanwhile, 35 μl (25 μl) of the creamed 4.7 μm (3.4 μm) emulsion droplets were diluted in a 500 μl magnesium buffer, and then split evenly into five parts. After a 30-min incubation, each DNA/streptavidin solution was mixed with one part of the emulsions. The mixtures were incubated for 1 h allowing for the binding of streptavidin to biotin groups on the emulsion droplet’s surface. Then they were washed four times to remove the remaining unbound DNA and excess streptavidin. Each type of droplets were diluted using the same magnesium buffer to a final concentration ~ 3 × 103 μl−1.
Confocal fluorescent microscopy
Leica DM6000 CS confocal microscope (TCS SP5 II) was used to take fluorescent images of our samples. Excitations with 488 nm, 543 nm, and 633 nm were used for imaging the samples. A ×63 oil immersion objective (Leica) was used for all fluorescent imaging.
Data Availability
The data that support the findings of this study are available from the corresponding author on request.
Electronic supplementary material
Acknowledgements
This research has been primarily supported by DOE DE-SC0007991 to P.M.C., N.C.S., R.S., and X.H. for initiation, design, analysis, and imaging. We acknowledge partial support from the Gordon and Betty Moore Foundation to P.M.C., N.C.S., R.S., and X.H. for DNA sequence design, preparation, and characterization; grants EFRI-1332411 and CCF-1526650 from the NSF, MURI W911NF-11-1-0024 from ARO and N000141110729 from ONR to N.C.S. and R.S. for data analysis. Y.Z. acknowledges support from DOE CBES for sample preparation, confocal microscopy, and data analysis. A.M., L.-L.P., X.H., and J.B. acknowledge partial support from the MRSEC program of the National Science Foundation under Award Number DMR-1420073 for synthesis and characterization of the emulsion droplets. We are grateful for shared facilities provided through the MRSEC program of the National Science Foundation under Award Number DMR-1420073. We thank Wenhai Zheng for the measurement of the droplets diffusion coefficient.
Author contributions
Y.Z. and P.M.C. designed research; Y.Z., A.M., L.-L. P., X.H., and R.S. performed research; Y.Z. analyzed data; Y.Z., N.C.S., J.B., and P.M.C. wrote the paper.
Competing interests
The authors declare no competing financial interests.
Footnotes
Electronic supplementary material
Supplementary Information accompanies this paper at doi:10.1038/s41467-017-00070-0.
Publisher's note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Contributor Information
Nadrian C. Seeman, Email: ned.seeman@nyu.edu
Jasna Brujic, Email: jasna.brujic@nyu.edu.
Paul M. Chaikin, Email: chaikin@nyu.edu
References
- 1.Whitesides GM, Grzybowski B. Self-assembly at all scales. Science. 2002;295:2418–2421. doi: 10.1126/science.1070821. [DOI] [PubMed] [Google Scholar]
- 2.Whitesides GM, Boncheva M. Beyond molecules: self-assembly of mesoscopic and macroscopic components. Proc. Natl Acad. Sci. USA. 2002;99:4769–4774. doi: 10.1073/pnas.082065899. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 3.Szwarc M. ‘Living’ polymers. Nature. 1956;178:1168–1169. doi: 10.1038/1781168a0. [DOI] [Google Scholar]
- 4.Halverson JD, Tkachenko AV. DNA-programmed mesoscopic architecture. Phys. Rev. E. 2013;87:062310. doi: 10.1103/PhysRevE.87.062310. [DOI] [PubMed] [Google Scholar]
- 5.Pieranski P. Colloidal crystals. Contemp. Phys. 1983;24:25–73. doi: 10.1080/00107518308227471. [DOI] [Google Scholar]
- 6.Leunissen ME, et al. Ionic colloidal crystals of oppositely charged particles. Nature. 2005;437:235–240. doi: 10.1038/nature03946. [DOI] [PubMed] [Google Scholar]
- 7.Kim AJ, Biancaniello PL, Crocker JC. Engineering DNA-mediated colloidal crystallization. Langmuir. 2006;22:1991–2001. doi: 10.1021/la0528955. [DOI] [PubMed] [Google Scholar]
- 8.Wang Y, et al. Crystallization of DNA-coated colloids. Nat. Commun. 2015;6:7253. doi: 10.1038/ncomms8253. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 9.Mirkin CA, Letsinger RL, Mucic RC, Storhoff JJ. A DNA-based method for rationally assembling nanoparticles into macroscopic materials. Nature. 1996;382:607–609. doi: 10.1038/382607a0. [DOI] [PubMed] [Google Scholar]
- 10.Valignat MP, Theodoly O, Crocker JC, Russel WB, Chaikin PM. Reversible self-assembly and directed assembly of DNA-linked micrometer-sized colloids. Proc. Natl Acad. Sci. USA. 2005;102:4225–4229. doi: 10.1073/pnas.0500507102. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 11.Rogers WB, Manoharan VN. Programming colloidal phase transitions with DNA strand displacement. Science. 2015;347:639–642. doi: 10.1126/science.1259762. [DOI] [PubMed] [Google Scholar]
- 12.Sacanna S, Irvine WTM, Chaikin PM, Pine DJ. Lock and key colloids. Nature. 2010;464:575–578. doi: 10.1038/nature08906. [DOI] [PubMed] [Google Scholar]
- 13.Wang Y, et al. Colloids with valence and specific directional bonding. Nature. 2012;491:51–55. doi: 10.1038/nature11564. [DOI] [PubMed] [Google Scholar]
- 14.Chen Q, Bae SC, Granick S. Directed self-assembly of a colloidal kagome lattice. Nature. 2011;469:381–384. doi: 10.1038/nature09713. [DOI] [PubMed] [Google Scholar]
- 15.van der Meulen SAJ, Leunissen ME. Solid colloids with surface-mobile DNA linkers. J. Am. Chem. Soc. 2013;135:15129–15134. doi: 10.1021/ja406226b. [DOI] [PubMed] [Google Scholar]
- 16.Hadorn M, Hotz PE. DNA-mediated self-assembly of artificial vesicles. PLoS ONE. 2010;5:E9886. doi: 10.1371/journal.pone.0009886. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 17.Parolini L, Kotar J, Di Michele L, Mognetti BM. Controlling self-assembly kinetics of DNA-functionalized liposomes using Toehold exchange mechanism. ACS Nano. 2016;10:2392–2398. doi: 10.1021/acsnano.5b07201. [DOI] [PubMed] [Google Scholar]
- 18.Hadorn M, et al. Specific and reversible DNA-directed self-assembly of oil-in-water emulsion droplets. Proc. Natl Acad. Sci. USA. 2012;109:20320–20325. doi: 10.1073/pnas.1214386109. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 19.Feng L, Pontani L-L, Dreyfus R, Chaikin PM, Brujic J. Specificity, flexibility and valence of DNA bonds guide emulsion architecture. Soft Matter. 2013;9:9816–9823. doi: 10.1039/c3sm51586a. [DOI] [Google Scholar]
- 20.Joshi D, et al. Kinetic control of the coverage of oil droplets by DNA-functionalized colloids. Sci. Adv. 2016;2:E1600881. doi: 10.1126/sciadv.1600881. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 21.Seeman NC. DNA in a material world. Nature. 2003;421:427–431. doi: 10.1038/nature01406. [DOI] [PubMed] [Google Scholar]
- 22.Dirks RM, Pierce NA. Triggered amplification by hybridization chain reaction. Proc. Natl Acad. Sci. USA. 2008;101:15275–15278. doi: 10.1073/pnas.0407024101. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 23.Yin P, Choi HM, Calvert CR, Pierce NA. Programming biomolecular self-assembly pathways. Nature. 2008;451:318–322. doi: 10.1038/nature06451. [DOI] [PubMed] [Google Scholar]
- 24.Padilla JE, et al. A signal-passing DNA-strand-exchange mechanism for active self-assembly of DNA nanostructures. Angew. Chem. Int. Ed. 2015;54:5939–5942. doi: 10.1002/anie.201500252. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 25.Yurke B, Turberfield AJ, Mills AP, Simmel FC, Neumann JL. A DNA-fuelled molecular machine made of DNA. Nature. 2000;406:605–608. doi: 10.1038/35020524. [DOI] [PubMed] [Google Scholar]
- 26.Zhang DY, Winfree E. Control of DNA strand displacement Kinetics using toehold exchange. J. Am. Chem. Soc. 2009;131:17303–17314. doi: 10.1021/ja906987s. [DOI] [PubMed] [Google Scholar]
- 27.Srinivas N, et al. On the biophysics and kinetics of toehold-mediated DNA strand displacement. Nucleic Acids Res. 2013;41:10641–10658. doi: 10.1093/nar/gkt801. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 28.Pontani LL, Jorjadze I, Viasnoff V, Brujic J. Biomimetic emulsions reveal the effect of mechanical forces on cell–cell adhesion. Proc. Natl Acad. Sci. USA. 2012;109:9839–9844. doi: 10.1073/pnas.1201499109. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 29.Thiam AR, Farese RV, Jr, Walther TC. The biophysics and cell biology of lipid droplets. Nat. Rev. Mol. Cell Biol. 2013;14:775–786. doi: 10.1038/nrm3699. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 30.Campàs O, et al. Quantifying cell-generated mechanical forces within living embryonic tissues. Nat. Methods. 2014;11:183–189. doi: 10.1038/nmeth.2761. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 31.Pontani LL, Haase MF, Raczkowska I, Brujic J. Immiscible lipids control the morphology of patchy emulsions. Soft Matter. 2013;9:7150–7157. doi: 10.1039/c3sm51137e. [DOI] [Google Scholar]
- 32.Wu K-T, et al. Kinetics of DNA-coated sticky particles. Phys. Rev. E. 2013;88:022304–022308. doi: 10.1103/PhysRevE.88.022304. [DOI] [PubMed] [Google Scholar]
- 33.Arthur JR. Molecular beam epitaxy. Surf. Sci. 2002;500:189–217. doi: 10.1016/S0039-6028(01)01525-4. [DOI] [Google Scholar]
- 34.Elbers NA, Jose J, Imhof A, van Blaaderen A. Bulk scale synthesis of monodisperse PDMS droplets above 3 μm and their encapsulation by elastic shells. Chem. Mater. 2015;27:1709–1719. doi: 10.1021/cm504504t. [DOI] [Google Scholar]
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Supplementary Materials
Data Availability Statement
The data that support the findings of this study are available from the corresponding author on request.