One of the fundamental challenges in nanophotonics is to gain full control over nanoscale optical elements. The precise spatiotemporal arrangement determines their interactions and collective behavior. To this end, DNA nanotechnology is employed as an unprecedented tool to create nanophotonic devices with excellent spatial addressability and temporal programmability. However, most of the current DNA-assembled nanophotonic devices can only reconfigure among random or very few defined states. Here, we demonstrate a DNA-assembled rotary plasmonic nanoclock. In this system, a rotor gold nanorod can carry out directional and reversible 360° rotation with respect to a stator gold nanorod, transitioning among 16 well-defined configurations powered by DNA fuels. The full-turn rotation process is monitored by optical spectroscopy in real time. We further demonstrate autonomous rotation of the plasmonic nanoclock powered by DNAzyme-RNA interactions. Such assembly approaches pave a viable route towards advanced nanophotonic systems entirely from the bottom-up.
Precise and reversible control of metal nanoparticles in space and time is a prerequisite to build dynamic plasmonic nanosystems with tailored optical functionality. However, realization of spatiotemporal control in three-dimensions with nanoscale accuracy poses great challenges. If one looks into the dynamic systems in nature, especially those on the molecular level, for instance, biological machines1,2 in living cells, their functionality represents remarkable examples of high-fidelity spatiotemporal control in a complex setting. FoF1-adenosine triphosphate (ATP) synthase3 is a rotary machine, which is fascinating particularly due to its sophisticated structure and extraordinary performance. It consists of interacting rotor and stator components that couple ATP synthesis/hydrolysis with a transmembrane proton translocation. By consuming chemical energy, its subunits can carry out astonishing 360° rotary motion with precise control over biological activity in space and time.
Despite the vigorous progress in dynamic plasmonics, rotary plasmonic nanosystems have been restricted to perform simple switching functions between on and off states4,5,6,7,8. In this work, we demonstrate a DNA-assembled plasmonic nanoclock that can carry out 360° rotary motion, taking inspiration from ATP synthase. In particular, we optically monitor and compare stepwise rotation driven by strand displacement reactions and autonomous rotation driven by DNAzyme-RNA interactions, respectively. Our work will set basis for the realization of DNA-assembled nanophotonic systems with dynamic complexity and tailored optical functionality.
Design of the rotary plasmonic nanoclock
Figure 1a shows the schematic of the rotary device, which contains several functional units. The rotor is a gold nanorod (AuNR, 38 nm × 10 nm) assembled on a 10-helix DNA origami9,10,11 bundle of 52 nm in length. Two 12-nt single-stranded foot strands (black) are extended from the two ends of the origami bundle. The lateral distance between the two feet is ~34.6 nm. The stator is another AuNR (38 nm × 10 nm) assembled on the bottom surface of a DNA origami plate (54 nm × 52 nm). Both the rotor and stator AuNRs are positioned on the respective origami surfaces via 10 staple extensions as binding sites. On the top surface of the plate, a ring-shaped origami structure12 is immobilized through three pairs of adjacent scaffold crossovers with six unpaired bases (see Supplementary Figs. 1 and 2). Sixteen footholds are evenly arranged and extended from the ring-shaped origami, forming a circular track of ~33.2 nm in diameter. This dimension matches the lateral distance between the two feet on the rotor bundle (see Supplementary Fig. 2). Each foothold consists of a binding domain (9-nt, black) with an identical sequence and a toehold domain (8-nt, colored) for endowing specific site information. To ensure the structural flexibility for rotation, the origami bundle and the origami plate are linked through their centers using two adjacent scaffold crossovers with 30 unpaired bases (see Supplementary Figs. 1 and 2).
Figure 1b shows the arrangement of the 16 footholds (fhi, fhi′, i = 1–8) in eight pairs distributed around the ring track. They are evenly separated by a distance of ~6.5 nm or by an angle of π/8. The footholds are identical in each pair and illustrated using the same color. The angle formed between the rotor and stator AuNRs is defined as θ. Figure 1c depicts the working principle of the stepwise rotation powered by DNA fuels. The two AuNRs are omitted in this figure. The rotation is based on a “release and capture” mechanism upon addition of specifically designed blocking and removal strands13 (see Supplementary Table 1). The blocking and removal strands for fh1, fh1′–fh8, fh8′ are marked as B1–B8 and R1–R8, respectively. Each blocking strand consists of three domains: an 11 nt-top domain (colored), a 6 nt-middle domain (black), and an 8 nt-bottom domain (colored). The top domain serves as a toehold and the rest two domains function as a blocking segment, which is complementary to one specific pair of the footholds on the ring track. The corresponding removal and blocking strands are fully complementary to each other. As shown in Fig. 1c, initially the two feet are bound to fh1 and fh1′ (red). The rest of the footholds are deactivated by blocking strands (only fh2 and fh2′ are shown for simplicity). To impose a clockwise rotation step from position 1–1′ to position 2–2′, removal strands R2 and blocking strands B1 are added sequentially. Through toehold-mediated strand displacement reactions14 (see Supplementary Fig. 3), fh2 and fh2′ are first activated, and fh1 and fh1′ are subsequently blocked. The two feet released from position 1–1′ search next active binding sites and subsequently capture fh2 and fh2′. This gives rise to a π/8 clockwise rotation and the origami bundle is bound to position 2–2′. Upon addition of corresponding DNA fuels (Supplementary Tables 2–4), the origami bundle and therefore the rotor AuNR can reach any designated positions around the ring track, carrying out programmable clockwise or counterclockwise stepwise rotation with respect to the stator AuNR. Figure 1d presents the transmission electron microscopy (TEM) image of the DNA origami structures. The origami bundle and ring are clearly visible in the inset image. Figure 1e shows the TEM image of the plasmonic nanoclock devices (see also Supplementary Fig. 4).
Optical characterizations of the stepwise rotation process
The crossed AuNRs in the plasmonic nanoclock system form a chiral object8,15,16. At incidence of circularly polarized light, the interacting plasmons excited in the two AuNRs can give rise to circular dichroism (CD) responses8,16,17,18. As a result, the stepwise rotations of the rotor AuNR with respect to the stator AuNR can be transformed into dynamic CD spectral changes, establishing a correlated relation between nanoscale motion and optical information. Figure 2a presents the CD spectra of the plasmonic nanoclock recorded during a full-turn clockwise rotation process at intervals of π/8 in 16 distinct states using a Jasco-1500 CD spectrometer. Nominally, at θ = 0 the plasmonic nanoclock is in an achiral state. When θ increases from 0 to π, the system first enters a left-handed (LH) zone and then a right-handed (RH) zone by crossing an achiral state at θ = π/2 in between. When θ increases from π to 2π, the system subsequently reaches LH and RH zones again. The theoretical results of the CD intensity as a function of θ are presented in Supplementary Fig. 5. In Fig. 2b, the experimental CD intensities at 732 nm (see the black dots marked in Fig. 2a) at different θ are replotted. It is apparent that the CD intensity follows a sinusoidal-like profile as a function of θ. The experimental CD results show an overall LH preference mainly because the centers of the AuNRs, the origami bundle, and the ring track are not perfectly coaxial (see Supplementary Fig. 2) and the ring track is not a perfect circle. Nevertheless, such slight imperfections offer a unique opportunity to optically differentiate the rotation states in the two nominally identical LH (or RH) domains. It is noteworthy that the experimental CD intensity at θ = 2π returns to its initial value at θ = 0. This reveals that the plasmonic nanoclock structures have been successfully directed back after the full-turn rotation, demonstrating the high fidelity of the programmable process. The in situ time-course measurements to characterize the kinetics of the individual rotation steps can be found in Supplementary Fig. 6. To validate the rotation reversibility, the CD intensities recorded along two opposite rotation directions are compared. As shown in Fig. 2c, the system first carries out counterclockwise stepwise rotation (red) from 0 to 15π/8 and is then driven back, undergoing clockwise stepwise rotation (black). The CD intensities at the corresponding rotation angles along the two opposite routes nearly coincide with one another, proving excellent reversibility of the stepwise rotation process.
Next, we further develop the rotary plasmonic nanoclock to an autonomous system. This represents one of the first steps towards autonomous nanoplasmonics. The schematic of the autonomous system is shown in Fig. 3a. In this case, the feet are two 8–17 DNAzyme19 strands (green) extended from the two ends of the DNA origami bundle. Each DNAzyme strand contains a 4-nt flexible segment, 7-nt and 9-nt binding domains, as well as a 14-nt catalytic core. Around the ring track on the origami plate, identical RNA strands (purple) are assembled, serving as footholds. The DNAzyme can catalyze the cleavage of the phosphodiester bond (purple dot) in the individual RNA substrate in the presence of Mg2+, converting chemical energy into mechanical motion20,21,22. This gives rise to autonomous rotation of the rotor AuNR with respect to the stator AuNR processively. To specifically define the starting position of the autonomous process, two upper locking strands (black) are assembled on the origami bundle adjacent to the two DNAzyme feet, respectively, as shown in Fig. 3b and Supplementary Fig. 7. On the ring track, fh1 and fh1′ work as the corresponding lower locking strands (black-red) for hybridization with the upper ones to fix the origami bundle at position 1-1′ before rotation. Meanwhile, the two feet are initially deactivated using blocking strands b (brown, see Fig. 3b). The TEM image is shown in Supplementary Fig. 8.
The working principle of the autonomous rotation without external intervention is depicted in Fig. 3b. Only the substrates at fh2, fh2′, fh3, and fh3′ are shown for simplicity. The autonomous rotation is actuated in two steps. The first one is the activation of the two DNAzyme feet by addition of removal strands r (Supplementary Fig. 9 panels a–c). The feet then bind to the neighboring substrates at position 2–2′, forming bulged pseudo-duplexes and subsequently cut the substrates into shorter segments. At this state, the rotor bundle resides likely in between positions 1–1′ and 2–2′. The second step is the releasing of the rotor bundle from position 1–1′ by addition of blocking strands B1 (red-black-red) (Supplementary Fig. 9 panels d–f). Subsequently, the rotor AuNR hosted on the origami bundle starts autonomous movements powered by RNA hydrolysis (Supplementary Fig. 9 panels g–j), processively rotating clockwise along the ring track based on a burnt-bridge mechanism23.
Optical characterizations of the autonomous rotation process
To provide insights into the correlation between autonomous nanoscale motion and optical information as well as the fundamental differences between autonomous rotation without external intervention and stepwise rotation by sequential additions of DNA fuels, a set of in situ optical measurements have been carried out. Figure 4a shows the different time-course measurements for clockwise autonomous rotations, in which the number of the substrate footholds is successively varied. To facilitate clockwise rotations, position 8–8′ is free of substrates. The corresponding foothold positions of the six samples are presented in Supplementary Table 5. The CD intensities are monitored at a fixed wavelength of 732 nm. Upon addition of removal strands r, the CD intensities of the six samples exhibit similar signal increases. This indicates that the DNAzyme feet on the origami bundle are activated. The rotor AuNR starts to rotate and resides in between positions 1–1′ and 2–2′. Upon addition of blocking strands B1, the CD intensity changes of the six samples become substantially different. For the track arrangements 1–2, 1–2–3, and 1–2–3–4, the CD intensities increase. This is similar to the trend observed for the stepwise rotation in Fig. 2b, in which the CD signal reaches the maximum value at position 3–3′ (θ = π/4) in the first LH zone. For the track arrangements 1–2–3–4–5, 1–2–3–4–5–6, and 1–2–3–4–5–6–7, the CD intensities first show clear leaps and then immediate decreases. The observed leaps prove that a majority of the structures in the individual samples follow clockwise rotations. Otherwise, as shown in Fig. 2c a counterclockwise rotation would first lead to a valley feature instead of a leap. Interestingly, the CD decreasing magnitudes reveal a relation of 1–2–3–4–5–6–7 < 1–2–3–4–5–6 (see Fig. 4a). In other words, the minimum CD value occurs at position 6–6′ (θ = 5π/8). It is different from the stepwise rotation in Fig. 2b, in which the CD signal reaches the minimum value at position 7–7′ (θ = 3π/4). This counterintuitive observation outlines crucial differences of the plasmonic nanoclock system between carrying out autonomous rotation without external intervention and stepwise rotation powered by DNA fuels.
In order to understand the observed phenomena, two control experiments have been performed. We first examine whether the autonomous rotation can proceed, if two neighboring foothold sites along the ring track are free of substrates (Supplementary Table 6). As shown in Fig. 4b, for the track arrangement 1–2–x–x–5, i.e., the substrates are omitted at fh3 (fh3′) and fh4 (fh4′), its time-course result (light blue) is very similar to that of the track arrangement 1–2 (black). However, for the track arrangement 1–2–3–4–5 (light grey), the CD intensity decreases over time during rotation. Such experimental evidence indicates that the autonomous rotation cannot proceed, if two neighboring substrate footholds are missing. The rotor AuNR thus halts, before the first open site. Next, we examine whether the autonomous rotation can progress, if only one substrate foothold is omitted along the ring track. As shown in Fig. 4c, for the track arrangement 1–2–3–x–5, i.e., the substrate is omitted at fh4 (fh4′), its time-course result (dark blue) lies in between those of the track arrangements 1–2–3 (dark grey) and 1–2–3–4–5 (light grey). This reveals that it is possible for the rotor AuNR to hop over the open site and proceed with the autonomous rotation in this case.
Consequently, the observed phenomena in Fig. 4a can be understood and interpreted as follows. In the case of stepwise rotation powered by sequentially adding DNA fuels, each foothold on the ring track is site specific. The rotation direction is thus fully deterministic and unidirectional. In contrast, for autonomous rotation powered by RNA hydrolysis, each substrate foothold on the ring track is identical. Once the DNAzyme feet are activated from starting position 1–1′, in principle both clockwise and counterclockwise rotations are allowed. For the track arrangement 1–2–3–4–5–6, the clockwise autonomous rotation is highly preferable, because the neighboring substrates at fh7′ (fh7) and fh8′ (fh8) for facilitating the counterclockwise rotation are omitted. For the track arrangement 1–2–3–4–5–6–7, as only one substrate is missing at fh8 (fh8′), it is possible for the counterclockwise rotation to take place by hopping over one open site. Therefore, in this case the time-course result contains contributions from both clockwise and counterclockwise rotations. As demonstrated in Fig. 2b, c, clockwise and counterclockwise rotations starting from position 1–1′ give rise to CD values of opposite signs. Therefore, in Fig. 4a the CD decreasing magnitudes reveal a relation of 1–2–3–4–5–6–7 < 1–2–3–4–5–6. Taking a further step, different time-course measurements for counterclockwise autonomous rotations are performed. In this case, position 2–2′ is free of substrates to facilitate counterclockwise rotations. As shown in Fig. 4d (see also Supplementary Table 7), the experimental results agree with the predictions well, further validating our interpretations.
DNA nanotechnology opens a unique avenue to build programmable nanophotonic devices with coordinated motion from the bottom-up4,13,24,25,26,27. The precise spatiotemporal control of nanoscale optical elements endows photonic nanoarchitectures with unprecedented dynamic complexity, which is beyond the scope of other state of the art nanotechniques28,29. Importantly, by exploiting the assembly power of DNA origami together with the patterning capabilities of top-down nanotechniques, such as electron-beam lithography30,31, many new opportunities may arise, setting a solid foundation for futuristic research topics. For instance, fully addressable and programmable metasurfaces could be achieved by patterning DNA-assembled rotary AuNRs in two-dimensional lattices to create artificial nanostructured interfaces for manipulating light properties including phase, amplitude, and polarization32,33. Such a metasurface could shape light wavefronts via geometric phase, e.g. Pancharatnam-Berry phase32, by independently controlling the in-plane orientation of each rotary AuNR (see Supplementary Fig. 10). Furthermore, besides metal nanoparticles other nanoscale optical elements such as single emitters could also be integrated together. The combination of the DNA origami technique and on-chip nanolithography will particularly enable excellent control of light-matter interactions on the nanoscale in a fully programmable manner34. The relative distances and orientations between the AuNRs and single emitters could be dynamically tailored. This will substantially enhance and impedance match the outgoing radiation of the emitters to the far-field. In turn, light from the far-field can be confined in a subwavelength volume by the AuNRs, leading to strong modifications of the decay rate, emission direction, and quantum efficiency of the emitter35. Such hybrid platforms could, in the first instance, endow nanophotonics with full addressability and programmability on a single chip to create functional optical devices that utilize the respective strengths of both bottom-up and top-down nanotechniques.
Design and preparation of the DNA origami structures
Single-stranded scaffold DNA (p8064) was purchased from tilibit nanosystems. Staple, blocking, and removal strands were purchased from Sigma-Aldrich. Substrates were purchased from Integrated DNA Technologies, Inc. Agarose for electrophoresis and SYBR Gold nucleic acid stain were purchased from Life Technologies. Uranyl formate for negative TEM staining was purchased from Polysciences, Inc.
The DNA origami system was designed using caDNAno software36. It consisted of a 10-helix bundle, a 6-helix ring, and a single-layer plate arranged in a ‘honeycomb’ lattice, which were connected through scaffold crossovers (design and sequence details can be found in Supplementary Fig. 1 and Table 1). The DNA origami structures for stepwise plasmonic nanoclocks were assembled from 10 nM scaffold strands and 100 nM of each set of the staple strands (10-fold excess) in a 0.5 × TE buffer with 12 mM MgCl2 and 5 mM NaCl using a 20 h annealing program (85 °C 5 min, 70 °C–61 °C −1 °C/min, 60 °C–51 °C −1 °C/1 h, 50 °C–22 °C −1 °C/20 min, and 15 °C hold). The DNA origami structures were purified by 0.7% agarose gel electrophoresis in a 0.5 × TBE buffer with 11 mM MgCl2 for 3 h at 8 V/cm in a gel box immersed in an ice-water bath, and extracted by BioRad Freeze N Squeeze spin columns. The DNA origami structures for autonomous plasmonic nanoclocks were assembled and purified in a similar way. First, the mixture of the scaffold and staple strands without the foot strands were annealed to form the main structures in a 1 × TA buffer with 12.5 mM Mg(OAc)2, pH 7.6. Second, the blocked foot strands were added and the mixture was incubated at 30 °C for 24 h. Design and sequence details can be found in Supplementary Fig. 11, Tables 1 and 8. The autonomous DNA origami structures were purified by 0.7% agarose gel in a 1 × TA buffer with 15 mM Mg(OAc)2, pH 7.6 for 3 h at 8 V/cm in a gel box immersed in an ice-water bath (Supplementary Fig. 12).
DNA functionalization of the AuNRs and structure assembly
AuNRs (38 nm in length and 10 nm in diameter) were purchased from Sigma-Aldrich (Cat no 716812). Functionalization of the AuNRs with thiolated DNA (5′ HS-T12: HS-TTTTTTTTTTTT, purchased from Sigma-Aldrich) was carried out following a low pH procedure. First, thiolated DNA strands were incubated with TCEP [tris(2-carboxyethyl)phosphine] for 2 h. The ratio of DNA: TECP was 1:200. Second, the AuNRs (1 nM, 750 μL) were spun down and the supernatant was removed. The AuNRs were then mixed with thiolated DNA strands (250 μM 10 μL). In total, 845 μL modification buffer (0.59 × TBE, 0.023% SDS, pH = 3) was added. Ten microliter 5 M NaCl was added every 10 min for nine times. Fifty microliter 1 M NaOH was added subsequently to adjust the pH value to ~8, and the final concentration of NaCl reached 0.5 M. The AuNRs functionalized with DNA were then purified by centrifugation. Five times of centrifugations at a rate of 8000×g for 30 min were carried out. Each time, the supernatant was carefully removed and the AuNRs were resuspended in a 0.5 × TBE buffer containing 0.02% of SDS. The supernatant was then removed and the remained AuNRs were mixed with the DNA origami structures at a ratio of 10:1. The mixtures were annealed with the procedure of 35 °C–31 °C −1 °C/1 h, 30 °C–27 °C −1 °C/4 h, and held at 26 °C. Gel electrophoresis was used to purify the plasmonic nanoclocks with the same condition for purification of the DNA origami structures (Supplementary Fig. 13).
The CD spectra were measured using a Jasco-1500 CD Spectrometer with a Quartz SUPRASIL cuvette (path length, 10 mm). All measurements were carried out at 25 °C. The concentration of the blocking and removal strands was 250 μM.
For the individual CD spectrum measurements (Fig. 2a), one sample at position 1–1′ was divided into 17 copies. Each copy was 80 μL and the respective DNA fuels were added to drive the individual systems to their designated positions (Supplementary Table 2). To keep the concentration constant, equal volume of H2O was added, if no DNA strands were added. After each addition, the samples were incubated at 25 °C for about 1 h. The final concentrations of the AuNRs in all the systems were about 1 nM.
The time-course measurement for the stepwise rotation from position 5–5′ to position 5′–5 was carried out as follows. A 200 μL solution of the stepwise plasmonic nanoclock sample was used. The CD signal at 732 nm was monitored using the time-scan acquisition mode with a data pitch of 1 s. The respective blocking and removal strands were added to enable a programmed route (Supplementary Table 3). The initial concentration of the AuNRs was about 1.2 nM. After the process, the total volume increase was only about 9.6 μL (4.6%).
The time-course measurements for the autonomous rotation from position 1–1′ were carried out as follows. Hundred microliter solutions of different autonomous plasmonic nanoclock samples were measured. The CD signals at 732 nm were monitored using the time-scan acquisition mode with a data pitch of 1 s. The removal strands r and blocking strands B1 were added to actuate the autonomous rotation (Supplementary Table 9). The initial concentration of AuNRs was 0.8 ~ 1.2 nM. After the process, the total volume increase was only about 1.5 μL (1.5%).
All the data reported in this paper are available from the corresponding author upon request. The source data underlying Fig. 2a, b, c and 4a, b, c, d are provided with the paper.
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This project was supported by the Volkswagen foundation, and the European Research Council (ERC Dynamic Nano) grant. We thank Marion Kelsch for assistance with TEM. TEM images were collected at the Stuttgart Center for Electron Microscopy.
The authors declare no competing interests.
Peer review information Nature Communications thanks Jerome Plain, Hao Yan, and the other, anonymous, reviewer for their contribution to the peer review of this work.
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Xin, L., Zhou, C., Duan, X. et al. A rotary plasmonic nanoclock. Nat Commun 10, 5394 (2019). https://doi.org/10.1038/s41467-019-13444-3
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