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Micro-homology intermediates: RecA’s transient sampling revealed at the single molecule level

Abstract Recombinase A (RecA) is central to homologous recombination. However, despite significant advances, the mechanism with which RecA is able to orchestrate a search for homology remains elusive. DNA nanostructure-augmented high-speed AFM offers the spatial and temporal resolutions required to study the RecA recombination mechanism directly and at the single molecule level. We present the direct in situ observation of RecA-orchestrated alignment of homologous DNA strands to form a stable recombination product within a supporting DNA nanostructure. We show the existence of subtle and short-lived states in the interaction landscape, which suggests that RecA transiently samples micro-homology at the single RecA monomer-level throughout the search for sequence alignment. These transient interactions form the early steps in the search for sequence homology, prior to the formation of stable pairings at >8 nucleotide seeds. The removal of sequence micro-homology results in the loss of the associated transient sampling at that location.


INTRODUCTION
The process of homologous recombination--which exchanges one strand of a double-stranded DNA (dsDNA) with an identical or very similar sequence of single-stranded DNA (ssDNA)--is fundamental to all forms of life, maintaining genomic integrity, overcoming DNA lesions, rescuing DNA replication failures and affecting genetic diversity (1)(2)(3). Moreover, homologous recombination plays a significant role in the acquisition and horizontal transfer of antimicrobial resistance genes within bacterial populations.
Central to this pathway are the ubiquitous recombinases, such as the widely studied Escherichia coli Recombinase A (RecA), which catalyse the alignment and subsequent exchange of DNA strands at regions of sequence homology (4)(5)(6). While these proteins play a critically important role in a biological context, their programmable specificity and fidelity have made them appealing for use in bionanotechnological applications (7)(8)(9)(10).
The RecA-mediated strand-exchange can be split up into three distinct steps. It begins with the polymerisation of RecA monomers onto single-stranded DNA in the presence of magnesium and ATP to form a right-handed helical nucleoprotein filament (NPF) (11)(12)(13)(14). In this complex, each RecA monomer binds three nucleotides of the ssDNA through interactions with the backbone, leaving the nucleobases exposed at the core of the nucleoprotein complex (15).
The nucleoprotein filament subsequently probes dsDNA for regions of sequence homology between either of the constituent strands and the encapsulated ssDNA by forming a pre-synaptic joint (2,16). For this, the dsDNA substrate interacts with the NPF through the secondary binding site (binding site II) in the helical groove of the NPF (15,17,18). Here, the incoming dsDNA is transiently bound and a kink is induced in the backbone enabling the basepairs to be probed between the NPF-encapsulated ssDNA and the incoming dsDNA (17).
If base-pairing occurs--at a region of sequence homology--the originally transient NPF-dsDNA complex is stabilised and subsequent regions of the incoming duplex are probed in a processive manner, ultimately leading to the formation of a synaptic joint. It is noteworthy that the alignment of the dsDNA with the ssDNA encapsulated within the NPF, and the resulting strand-exchange, can occur without the input of chemical energy (2). In contrast, the final step of the recombination process--the disassembly of the NPF-dsDNA complex and thus the release of the new dsDNA duplex--requires hydrolysis of the RecA-bound ATP throughout the complex (19). Furthermore, while it has been shown that in vitro RecA can orchestrate the recombination of DNA molecules in isolation, the RecA-facilitated process is only one stage in the in vivo homologous recombination pathway which involves several other proteins to recruit and prepare the dsDNA as well as finalise the new pairing, and as such, RecA contains no known cleavage abilities (2).
The RecA-mediated homologous recombination process has been studied in its entirety, from formation of the nucleoprotein filament, alignment of homologous sequences, to strand exchange using an array of eloquent single molecule techniques, including magnetic tweezers (20)(21)(22)(23), DNA curtains (24), tethered particle motion (25) and FRET-based systems (26)(27)(28). These studies reveal mechanistic subtleties that would otherwise be averaged out by more classical ensemble approaches. However, when paired with the plethora of biochemical (29,30) and structural studies (15) then a holistic understanding of the complex recombination process is formed. While these extensive studies provide invaluable contributions, they are mostly indirect observation of the homologous recombination process.
In contrast, our previous work focused on the investigation of the mode and specific interaction geometry of free RecA nucleoprotein filaments during a homology search, observed directly in real-time with high-speed atomic force microscopy (HS-AFM) (18). We showed that 1D facilitated diffusion along the dsDNA is utilised by the RecA NPF for the registration of DNA nucleotides at the 'local' level. Furthermore, this work has validated the interaction geometry derived through molecular dynamics modelling by Yang et al. (17) which proposed that the incoming dsDNA is being loaded into the binding site II in line with the right-handed helical groove of the nucleoprotein complex (18).
As such, direct observation with HS-AFM of the homologous recombination process arguably has a key role to play in providing novel insight where considerable gaps still remain in our understanding. Here, we directly observe the full RecA-orchestrated homologous recombination of DNA molecules within a DNA nanostructure and identify the transient (those which exist for <10 s) searching intermediates at the early stages of sequence alignment. We employ a DNA origami-based experimental platform (DNA frame) (18,31,32) to host the different DNA components required for homologous recombination, creating an environment that replicates a resected DNA break point as an initial substrate. The DNA frame not only provides the framework to host the reaction but also acts as a geometrical reference within which the orientation and relative positions of the interacting species can be measured, enabling the sequence-specific locations of shortlived interaction intermediates to be directly determined when observed in real-time with high-speed atomic force microscopy (HS-AFM).

Materials
The DNA oligonucleotides used to form the internal DNA strands, including those which contained a photo-cleavable linker, were sourced from Integrated DNA Technologies (IDT) (Coralville, USA). The DNA oligonucleotide staples required to form the DNA frame were purchased from Eurofins Genomics (Tokyo, Japan). The M13mp18 ssDNA was purchased from Tilibit nanosystems GmbH (Munich, Germany). The sequences for all DNA used in this study are provided in supplementary information.
RecA protein (E. coli) was purchased from New England Biolabs (NEB; Ipswich, USA) at a concentration of 2 mg/ml and was diluted in a buffer containing 20 mM Tris-HCl (pH 7.5), 1 mM DTT, 0.1 mM EDTA and 5% glycerol to a 20 ug/ml working stock.

Formation of DNA origami nanostructure
The DNA frame was designed using the caDNAno software (36,37). The DNA origami structure was formed from the collective self-assembly of 223 oligonucleotide staples (sequence list, Supplementary Table S1 & Supplementary Figure S10) and M13mp18 ssDNA scaffold. Structures were folded in 10 mM Tris acetate (pH 7.4), 10 mM Mg(OAc) 2 and 1 mM EDTA by heating the mixture to 85 • C followed by slowly cooling to 15 • C at a gradient of -1 • C min −1 . The internal dsDNA strands were hybridised from their constituent oligonucleotides (sequence list, Supplementary Table S2) using the same heating/cooling protocol and were then incorporated into the DNA frame by adding a 5-fold excess to the DNA frame solution, heating the mixture to 45 • C, followed by slowly cooling to 15 • C at a gradient of -0.5 • C min −1 . Completed frames were purified using a Sephacryl S400 (GE Healthcare, Buckinghamshire, UK) size-exclusion matrix in a buffer containing 10 mM Tris-acetate, (pH 7.4), and 2 mM Mg(OAc) 2 , 1 mM EDTA to remove excess staples and unincorporated internal DNA.

Polymerisation of RecA
RecA nucleoprotein filaments were formed within the DNA nanostructures as described previously (7). Briefly, RecA protein was introduced to the DNA origami at a ratio of 0.1-0.5 RecA monomers to three nucleotides (1 unit) of exposed ssDNA in the presence of 500 M ATP␥ S, 10 mM Tris acetate (pH 7.4) and 2 mM Mg(OAc) 2 . The reaction was incubated at 37 • C for 30 min.

Recombination statistics
The reaction volume of DNA nanostructures containing RecA was adjusted to contain 10 mM Tris acetate (pH 7.4) and 10 mM Mg(OAc) 2 . The structures were exposed to UV ( = 340 nm, 6.1 mW/cm 2 ) for 10 s in order to break the photo-cleavable linker, thus releasing the nucleoprotein filament and enabling it to interact with the neighbouring internal dsDNA molecules. The reaction was allowed to proceed for 30 min at 37 • C. The reaction volume was deposited upon Ni 2+ pre-incubated mica and imaged with HS-AFM.

In situ recombination
DNA nanostructures containing RecA were deposited upon Ni 2+ pre-incubated mica, incubated for 20 mins, rinsed with deionised water and imaged using HS-AFM in buffer containing 10 mM Tris acetate (pH 7.4) and 10 mM Mg(OAc) 2 .
The nucleoprotein filament was released from the anchor following exposure to UV ( = 340 nm, 6.1 mW/cm 2 ) for 10 s in situ, and the subsequent nucleoprotein-DNA interactions followed at 22 • C, while continually scanning with HS-AFM.

HS-AFM imaging
All samples were imaged in tapping mode (amplitude modulation), in aqueous buffer, with a Bruker Dimension Fastscan AFM (Bruker Nanosurfaces, Santa Barbara, USA), using Fastscan D etched Si 3 N 4 cantilevers (nominal spring constant = 0.25 N/m, Resonant frequency approximately 110 kHz in liquid) containing Si tips (nominal radius of curvature approximately 5 nm). Cantilevers were driven close to resonance under liquid and images were typically acquired at scan speeds between 38 and 60 Hz and a tapping amplitude of 10 nm. Typical images are acquired at 1 m × 1 m and 256 × 256 pixels giving a pixel size of ∼4 nm. Images were flattened by plane-fitting using the associated Nanoscope analysis software (Bruker Nanosurfaces, Santa Barbara, USA). ImageJ (http://rsbweb.nih.gov/ij/) was subsequently used to determine the position of the internal DNA strands throughout sequential images in a series by vectorising the AFM image as described in supplementary information ( Figure S8).

Formation of DNA frame and polymerisation of RecA
The DNA frame contains an empty space at its centre ( Figure 1B) within which three 128 basepair (bp)-long DNA molecules are incorporated parallel to each other to serve as the templates on which the single-molecule recombination experiments are conducted. The middle suspended DNA molecule ( Figure 1C) is only partially double-stranded and contains a 30 nucleotide (nt) region of ssDNA at the 3 termini upon which RecA can be selectively bound to form an active nucleoprotein filament ( Figure 1D)--herein termed the NPF DNA. A 30 nt length was chosen due to the geometrical constrains of the DNA nanostructure system, which contains an ∼40 nm reaction window, and is consistent with the length scales used by other single molecule studies (24,33). RecA preferentially binds to ssDNA at low Mg 2+ concentrations and hence its selectivity for this region of the structure can be modulated (2). The bottom dsDNA molecule features a 30 nt region on the upper strand which is homologous in sequence and parallel in orientation to the single-stranded region of the NPF DNA held within the DNA frame ( Figure  1C)--herein this is called the Reaction DNA. In contrast, the sequence of the top dsDNA molecule does not feature the 30 nt homologous region and is utilised as an inbuilt heterologous control for recombination specificity ( Figure 1C)--hence termed the Control DNA. Therefore, the active nucleoprotein filament formed on the termini of the NPF DNA is expected to create only a single specific recombination product upon completion of the reaction ( Figure 1E). The orientation of the DNA frame, and therefore the identity of the different DNA molecules and the configuration of any recombination products, can be identified via the inbuilt polarity marker ( Figure 1C, black triangle).
RecA has no known restriction activity (2) and hence a method for releasing the nucleoprotein filament from the DNA frame is required. Here, we use a UV photocleavable linker incorporated in the backbone of the NPF DNA ( Figure 1C, yellow star) between the 3 end of the ssDNA region and the anchor sequence used to hybridise it into the DNA frame. This enables cleavage and thus release of the nucleoprotein filament -initiating the recombination interaction--which can be triggered by exposure to UV light during the HS-AFM imaging.
The successful assembly of the internal suspended DNA molecules and cleavage of the photocleavable linker was verified prior to (Supplementary Figure S1) and post incorporation (Figure 2) into the DNA frame by gel electrophoresis and AFM, respectively. From Figure  2A, B, clear identification of the polarity marker (white triangle) and inclusion of all three suspended DNA molecules within the central cavity can clearly be seen. The incorporation efficiency was found to be ∼60% when all the DNA molecules were introduced at a 5:1 (DNA:frame) ratio.
Despite the presence of a large single-stranded region at the end of the NPF DNA it was found to be able to bridge across the central void in the DNA frame and assemble to both anchor points, albeit with diminished efficiency when compared to the fully double-stranded Reaction and Control DNA.
We note that during HS-AFM imaging the DNA frame remains securely attached to the mica substrate, while the internal suspended DNA molecules remain clearly flexible--yet individually discernable--throughout sequential images. This suggests that they are not attached to the mica surface and therefore remain available for subsequent homologous recombination interactions. In particular, the region of ssDNA present within the NPF DNA is overtly flexible, in many cases observed as a gap in the DNA molecule due to the limited temporal response of the HS-AFM (Figure 2 B).
To study the homologous recombination reaction, a RecA nucleoprotein filament was formed on the ssDNA portion of the NPF DNA in the presence of the ATP␥ S. In order to ensure that the RecA only bound to the singlestranded portion and not to either the DNA frame or any of the suspended dsDNA molecules, the concentration of the protein was kept low at a ratio of RecA to three nucleotides of 0.1-0.5, and the Mg 2+ was kept at 2 mM to maintain the single-strand specificity. Where these concentrations were exceeded unintended binding of RecA to other DNA components of the system were noted (Supplementary Figure S2).
From the AFM characterisation in Figure 2C, the presence of RecA at the expected location (white arrow) can clearly be seen. However, the structure differs slightly from the ones reported in earlier work (7,18,33,34), and in particular no significant difference in height between the dsDNA and the RecA nucleoprotein filament was observed. We speculate that at the concentrations of RecA required for this work, incomplete polymerisation occurs, and that although RecA is seen to bind to the DNA and is unambiguously demonstrated to be responsible for the homologous pairing later in this work (Supplementary Figure S4) it is likely to be a collection of small groups of bound monomers along the singlestranded region of the NPF DNA and that the extent of continuous polymerisation may be limited. This is also consistent with reports that 6-8 monomers are required to initiate polymerisation (2), and the 30 nt region employed here can only accommodate a maximum of 10 monomers.

RecA-mediated recombination of DNA
To characterise the efficiency of the RecA-mediated recombination between the nucleoprotein filament on the suspended NPF DNA and the homologous region on the suspended Reaction DNA, the recombination reaction in the DNA frame was carried out in solution and the products characterised by AFM after deposition on the mica surface. Following the introduction of RecA, the formed nucleoprotein filaments were released with a 10 s UV exposure and allowed to interact for 30 min at 37 • C in the absence of ATP hydrolysis. We note that the absence of the photo-cleavable linker prevents the release of the nucleoprotein filament during UV exposure (Supplementary Figure S3), confirming that nonspecific DNA damage is not responsible for the release and that the cleavage remains controllable. The 5 end of the suspended NPF DNA remains tethered to the DNA frame through the dsDNA region of the molecule.
There is an equal probability for the tethered nucleoprotein filaments to interact with either the Control or Reaction DNA. However, we note that stable synaptic joints are only expected to form on the homologous region of the latter. Figure 3 shows the results of a typical recombination experiment. We observe successful RecA-mediated recombination, i.e. the formation of a synaptic joint on the Reaction DNA with an efficiency of 52.5 ± 1.6%. In contrast, the presence of stable joints formed with the heterogeneous Control DNA are found to exist with a much lower yield of only 7.4 ± 0.6%. A similar number, 4.6%, showed no RecA-mediated recombination. We note that around a third of all imaged DNA frames could not be analysed (35.5%) as they could not be classified. A number of representative examples of such unclassified frames is shown in Supplementary Figure  S5 D. To rule out any geometrical bias in the difference of the yield, potentially imposed through the DNA frame, the positions of the Control and Reaction DNA within the frame were swapped. A similar ratio between homologous synaptic joints formed on the Reaction DNA, and incorrectly formed joints on the Control DNA, were found (Supplementary Figure S5).

Characterising the observed synaptic joints
Despite the semi-flexible nature of the DNA frame support structure and the suspended DNA molecules, it remains possible to track the stable position of synaptic joints over time with HS-AFM. The position of the synaptic joints formed with the Reaction DNA can be measured via the distance along the DNA molecule. Figure 4A shows three representative joints which remain stably bound at the center of the designated region of homology (∼19 nm, ∼55 bp along the DNA strand from the end furthest from the polarity marker) ( Figure 4A). This indicates that the observed synaptic joints are not transient intermediates but represent the correct formation of new base pairs, resulting in a strong complex able to resist the scanning probe of the HS-AFM. A notable outlier is highlighted ( Figure 4A, black star) -this is the result of a probe-induced dislocation in the HS-AFM image, which occurs when the DNA frame moves slightly on the substrate during imaging (Supplementary Figure S6) thereby leading to an artefact.
Furthermore, the length of the paired complexes can be analysed to estimate the extent of sequence alignment within each synaptic joint. Figure 4 B shows a representative distribution of measured synaptic joint lengths. Given our limited knowledge of the extent to which RecA is polymerised upon the ssDNA section of the NPF DNA it is difficult to estimate the length of joint we would expect for full sequence pairing. However, it is known that RecA underwinds DNA by 1.5 times (2), and consequently it could be argued that a full 30 nt nucleoprotein filament would be expected to be 15.3 nm in length--the equivalent of 45 nt. However, in the present case, the RecA is unlikely to be fully polymerised and hence the underwinding is likely to be <1.5 times. Therefore, to estimate a lower limit of the nucleoprotein filament length, we assume the minimal case with no RecA underwinding present which yields a joint length of 10.2 nm. Here, we expect a distribution of RecA coverage on the ssDNA portion of the NPF strand and thus nucleoprotein filament lengths. Both limits are indicated in Figure 4 B and it can be seen that the observed distribution is indeed centered around this range with an average joint length of 11.1 ± 3.5 nm. It is notable that we observe a distribution of joint lengths below the lower bound suggesting that a proportion of nucleoprotein filaments are only partially aligned.
However, we note that given the observed variations of pairing length and bound RecA monomers, it is impossible to discern the exact sequence alignments from the length data alone in this work.

In situ HS-AFM observation of homologous recombination
The RecA-mediated recombination can be observed in realtime and at the single molecule level using HS-AFM ( Figure  5 and Supplementary movie S1). At the beginning of the experiment, the NPF DNA containing the nucleoprotein filament at its end can be seen suspended across the central void of the frame clearly tethered on both ends. Immediately following cleavage of the UV photocleavable linker, the NPF DNA is released and becomes difficult to track due to its rapid movement relative to the speed of the scanning HS-AFM probe. The NPF has equal probabilities of reaching either the Reaction or the Control DNA and is therefore able to search all of the available sequence space. In all observed cases alignment is achieved at the region of sequence homology in the Reaction DNA resulting in a stable synaptic complex as intended. This is evident from the 198 s time-point in Figure 5 and persists at the same location throughout the remainder of the image series, revealing the first direct single-molecule observation of RecA-mediated homologous recombination.
Typically, the formation of a synaptic joint is observed within 30-40 s from initiation of the interaction upon release of the nucleoprotein filament from the DNA frame by UV cleavage (Figure 5, Supplementary Movie S1 & Supplementary Figure S7). Interestingly, in contrast the observation of a low number of heterologous pairings (those which occur with the Control DNA) when the reactions were conducted in solution prior to deposition on the mica surface (Figures 2-4), here no evidence for the formation of such heterologous pairings was seen when directly observing the homologous recombination via HS-AFM.

The influence of micro-homology
Following RecA-mediated recombination events in realtime with HS-AFM reveals a landscape of transient sampling intermediates which appear at consistent locations between samples along the Reaction DNA in the absence of any artificial fixation agents. Such transient sampling events are defined as those interactions that exist for no more than 10 s in our experiments. One RecA monomer of a NPF binds to three nucleotides of one strand of a double-stranded DNA with the same sequence as the 3 nt encapsulated in this RecA monomer. It is therefore reasonable to assume that for any observable interaction to occur between the NPF and the Reaction DNA, homologous sequences of at least 3 nt have to be present. When the underlying sequence of the Reaction DNA was analysed for instances of micro-homology shared between itself and the ssDNA region of the NPF DNA, nine domains--each 3-5 nt in length--were identified ( Figure  6). In order to reconcile the existence of micro-homology with the observed transient sampling, the position of each   Figure S8). The corresponding position in the sequence of the Reaction DNA was determined by assuming a B-form DNA helix. All observed interactions are represented as a frequency distribution of measured interaction locations in Figure 6 B. To ensure stability of the nucleoprotein filaments, the duration of all experiments was kept significantly shorter than the halflife of ATP␥ S (∼120 mins). The measurement uncertainty is dominated by the flexibility of the DNA molecules within the DNA nanostructure, and has been estimated to be around 1-2 nm or 3-6 nt. We also note that the suspended NPF DNA is formed from three overlapping oligonucleotides and therefore retains a higher degree of flexibility than dsDNA (see Supplementary Figure S11), as it is able to bend and rotate around the nicks in the backbone. This limits a potential geometrical bias that the fixed tether may otherwise impose. It can clearly be seen that the NPF is not limited to a restricted distal region of, but in fact has access to, the entire suspended Reaction DNA. Interestingly, we find a strong correlation between the observed transient interactions ( Figure 6C, ivii) and the identified areas of micro-homology ( Figure 6B, [1][2][3][4][5][6][7][8][9], indicating that transient interactions occur at areas of micro-homology as short as 3 nt. Of the observed interactions, we find that the most common distribution occurs around the designed region of homology, where the potential for sequence alignment is the highest (Figure 6B, green text). In contrast, all other transient sampling observed outside of this region was found to be distributed with an even frequency suggesting that there is no particular sequence preference, but that the length of the sequence homology is important, consistent with previous observations (2). This was also the case where micro-homology was shared with the suspended Control DNA (Supplementary Figure S9).
In order to confirm further the specificity of the observed correlation, the micro-homology in domains 1, 2, 3, 5, 8 and 9 of the Reaction strand were all disrupted by shuffling of the nucleotide sequence. The resulting frequency distribution is shown in Figure 6B (red plot). From this it can be seen that the change in underlying sequence successfully leads to the loss of transient sampling intermediates being located in those regions (e.g. i, iii, vi and vii). In contrast, where the micro-homology domain is switched, in this case from domain 4 (GTCCA) to domain 8 (GTG), the transient sampling intermediate ii is still observed despite the sequence change ( Figure 6B, black diamond).
This clearly demonstrates that the transient interactions during the RecA-mediated homology search observed with HS-AFM are governed by the sequence of the interacting dsDNA, and that sequences of micro-homology as short as 3 nt, corresponding to the interaction footprint of a single RecA monomer, lead to such transient interactions. These observed transient states therefore represent an early stage in the homology searching process, constituting an often ignored sampling step prior to the occurrence of stable pairing when a sequence of homology of 8 nt or longer has been located (24).

CONCLUSIONS
Homologous recombination is critically important in maintaining genetic integrity across all forms of life. A breakdown of this recovery pathway results in deleterious cell activity such as carcinogenesis. Central to this process is the RecA family of recombinase enzymes which pair regions of sequence homology and enact a strand exchange in order to recover the damaged DNA. We have employed HS-AFM in conjunction with DNA origami nanostructures that display loosely-bound DNA molecules internally to visualise directly the dynamics of RecAmediated homologous recombination in situ and at the single molecule level.
We have demonstrated that RecA-mediated homologous recombination can take place in the context of a DNA nanostructure with high specificity for the desired homologous sequence. In this setup, the initial spatial constraints on the active RecA nucleoprotein filament can be relaxed upon request, allowing the filament to interact with dsDNA within a determined radius. This opens up a range of avenues to exploit the capabilities of recombination enzymes in vitro for non-native applications such as bio-nanotechnology and molecular information processing.
Using our approach of HS-AFM augmented with DNA nano-reference structures, we demonstrate the direct observation and decode the transient interaction intermediates of the RecA-mediated homology searching process. Evidence of such initial transient contacts has been found previously through single molecule experiments (24)(25)(26)(27)(28)(29)(30)(31)(32)(33)(34)(35), but their relevance has generally been overshadowed by the more stable pairings occurring at homologous sequences of 8 nt or more in length. Here we directly observe the transient sampling during the search for sequence homology, prior to stable synaptic joints being formed. Using the DNA nanostructure as a measurement reference we were able to identify the locations of the transient sampling interactions and correlate them with the occurrence of microhomology of three or more nucleotides in length. This demonstrates that RecA nucleoprotein filaments are able to transiently sample sequence space at the single RecA monomer level on short time scales (<10 s) in the early stages of a sequence alignment. Such contacts remain short-lived unless additional sequence alignment greater than 8 nt occurs which would lead to energetically stable homologous pairing, which would require ATP hydrolysis to resolve.
In conclusion, this work directly explores the early stages in the RecA-mediated homology searching mechanism by directly mapping interaction intermediates and thereby decoding the transient interaction space of RecA in realtime with HS-AFM. It provides the first direct observation of the initial transient basepair-driven homology sampling at the single-RecA-monomer-level, which is an early step in the homology searching mechanism.

DATA AVAILABILITY
Data supporting this work can be accessed via the University of Leeds repository: https://doi.org/10.5518/945.

SUPPLEMENTARY DATA
Supplementary Data are available at NAR Online.