HS-AFM observations of the non-specific transient binding of Cas9–RNA. a
Sequential HS-AFM images of Cas9–RNA molecules transiently bound to
non-target sites of the DNA. Transient binding of Cas9–RNA appears as a
bright spot in the images, as indicated by the white arrows. Most of the
binding events were completed within a single-line scanning time (1.9
ms; 150 ms / 80 lines). The scale bar is 50?nm. b, c Differences between the lowest and highest heights in each image during the HS-AFM observations of DNA only (b) and Cas9–RNA–DNA (c). In c, the spikes indicate the transient binding of Cas9–RNA to the DNA. d, e Frequency (d) and lifetime (e)
of the transient binding of Cas9–RNA to the DNA. The lifetime was
estimated by counting the successive line numbers on which the
spike-like spots were continuously seen. Spike-like spots with heights
over 3.5?nm were judged as Cas9–RNA molecules. The lifetime was fitted
by the 1st order exponential decay, with a time constant of
0.98?±?0.02?ms (n?=?656)
HS-AFM
enables the direct visualization of the structures and dynamics of
intact molecules, in contrast to other single-molecule imaging methods,
in which a molecule of interest must be labeled with fluorescent probes.
Using HS-AFM, we visualized the real-space and real-time dynamics of
CRISPR-Cas9 in action, thereby improving our mechanistic understanding
of the RNA-guided DNA cleavage by Cas9. Although our HS-AFM data are
essentially consistent with previous fluorescence-based imaging studies11,17,18,
there are some discrepancies between these studies. For example, a
recent single-molecule FRET study reported that the majority (90%) of
Cas9–RNA stably adopt the D state upon DNA binding, while only 3% of the
complexes undergo transitions between the I and D states18.
In contrast, our HS-AFM data showed that most of the Cas9–RNA complexes
fluctuate between the I and D states after DNA binding. This
discrepancy is likely due to the differences in the imaging techniques
and experimental conditions. On the basis of our HS-AFM data, together
with previous structural, biochemical and biophysical data11,12,13,14,15,16,17,18,28, we propose a model for the Cas9–RNA-mediated DNA cleavage (Fig. 7a–c).
Apo-Cas9 adopts a flexible modular architecture, and assembles with the
guide RNA to form the stable Cas9–RNA effector complex. The Cas9–RNA
complex interrogates the target sites on the DNA via three-dimensional
diffusion, and recognizes the complementary target site with the NGG
PAM. Cas9–RNA then unwinds the dsDNA target to form the R-loop. The HNH
domain undergoes conformational fluctuations upon R-loop formation, and
then adopts the catalytically-active docked conformation to cleave the
target strand, while the RuvC domain cleaves the non-target strand.
Overall, this study provides unprecedented details about the functional
dynamics of CRISPR-Cas9, and highlights the potential of HS-AFM to
elucidate the action mechanisms of RNA-guided effector nucleases from
distinct CRISPR-Cas systems29.
Fig. 7
Model of CRISPR-Cas9 action. a Assembly of the Cas9–RNA binary complex. b Target DNA interrogation by Cas9–RNA via three-dimensional diffusion. c
DNA recognition and cleavage by Cas9–RNA. DNA cleavages by the RuvC and
HNH domains are indicated by the cyan and magenta triangles,
respectively
Wild-type S. pyogenes Cas9 and GFP-dCas9(D10A/C81L/C574E/H840A) were expressed in Escherichia coli Rosetta2 (DE3), and then purified to homogeneity by column chromatography, as described with minor modifications15. Briefly, the Cas9 protein was expressed in E. coli
Rosetta2 (DE3) (Novagen), and was purified by chromatography on Ni-NTA
Superflow (QIAGEN), HiTrap SP HP (GE Healthcare), and HiLoad Superdex
200 16/60 (GE Healthcare) columns. The 98-nt guide RNA was transcribed
in vitro, and then purified by denaturing urea polyacrylamide gel
electrophoresis, as described15. The 600-bp target DNA was PCR-amplified using the pUC119 plasmid containing the 20-nt target sequence and the TGG PAM30
as the template, and then purified using a Wizard DNA Clean-Up System
(Promega). The sequences of Cas9, the guide RNA and the target DNA are
provided in Supplementary Data 1.
HS-AFM observations on an AP-mica surface
The laboratory-built high-speed AFM was used in the tapping mode31.
The cantilever deflection was detected with an optical beam deflection
detector, on which a 0.7?mW, 780?nm infrared laser was mounted. The
infrared laser beam was focused onto the back side of the cantilever
(Olympus: BL-AC7DS-KU4) through a ×60 objective lens (Nikon: CFI S Plan
Fluor ELWD 60×). The reflected laser from the cantilever was detected
with a two-segmented PIN photodiode. The spring constant of the
cantilever was ~100?pN?nm?1. The resonant frequency and the
quality factor of the cantilever in liquid were ~800?kHz and ~2,
respectively. An amorphous carbon tip was fabricated on the original AFM
tip by electron beam deposition (EBD). The length of the additional AFM
tip was ~500?nm, and the radius of the apex of the tip was ~4?nm. The
free oscillation amplitude of the cantilever was ~1?nm and the set-point
amplitude was set to 90% of the free amplitude. For HS-AFM observations
of Cas9, a mica surface was treated for 3?min with 0.011%
(3-aminopropyl)triethoxysilane (APTES) (Sigma-Aldrich). The complex of
Cas9, RNA and DNA was pre-assembled (Cas9:RNA:DNA?=?1:1:1 mole ratio) in
AFM-imaging buffer. HS-AFM observations of apo-Cas9 and Cas9–RNA were
performed in buffer, consisting of 20?mM Tris-HCl, pH 8.0, 100?mM KCl
and 0.01?mM EDTA. HS-AFM observations of the Cas9–RNA–DNA and
GFP-dCas9–RNA–DNA complexes were performed in buffer, consisting of
20?mM Tris-HCl, pH 8.0, 30?mM KCl and 0.01?mM EDTA. All HS-AFM
experiments were performed at room temperature.
HS-AFM observations on a lipid bilayer
The DNA was loosely immobilized on a mica-supported lipid bilayer31. In brief, 1,2-dipalmitoyl-sn-glycero-3-phosphocholine
(DPPC; Avanti Polar Lipids) and
1,2-dipalmitoyl-3-trimethylammonium-propane (DPTAP; Avanti Polar Lipids)
were suspended in chloroform, and 1,2-dipalmitoyl-sn-glycero-3-phosphoethanolamine-N-(cap
biotinyl) (biotin-cap-DPPE; Avanti Polar Lipids) was suspended in a
mixture of chloroform:methanol:water?=?65:35:8 (volume ratio). The lipid
solutions were mixed at a weight ratio of
DPPC:DPTAP:biotin-cap-DPPE?=?90:5:5. Small unilamellar vesicles (SUVs)
of the lipid mixture, at 0.2?mg?ml?1 in 10?mM MgCl2,
were prepared by sonication for 1?min, using a bus-sonicator (AS ONE). A
mica disk (1.0?mm in diameter) glued on the sample stage of the HS-AFM
was freshly cleaved, and the mica-supported lipid bilayer was formed on
it by depositing 2?μl of the SUVs solution for 3?min, followed by 1?μl
of 20?mM Tris-HCl, pH 8.8, for over 10?min. The sample surface was
rinsed with drops of Milli-Q water (20?μl?×?5) to remove the excess
SUVs, and then the solution was replaced with buffer A (20?mM Tris-HCl,
pH 8.0, 30?mM KCl, 0.01?mM EDTA). DNA (2?μl, 1 ng μl?1) in
buffer A was deposited on the surface for 3?min. After rinsing the
surface with buffer B (20?mM Tris-HCl, pH 8.0, 30?mM KCl, 2?mM MgCl2),
the sample stage was immersed in a liquid cell filled with buffer B
(~55?μl), and HS-AFM observations were performed. During the HS-AFM
observations, a drop (~5?μl) of either apo-Cas9 or Cas9–RNA (molar ratio
of Cas9:RNA?=?1:2) was added to the liquid cell, at a final
concentration of ~80?nM.