ISSN 0006-2979, Biochemistry (Moscow), 2024, Vol. 89, No. 4, pp. 674-687 © Pleiades Publishing, Ltd., 2024.
674
REVIEW
Studying Structure and Functions of Nucleosomes
with Atomic Force Microscopy
Alexander A. Ukraintsev
1#
, Mikhail M. Kutuzov
1#
, and Olga I. Lavrik
1,2,a
*
1
Institute of Chemical Biology and Fundamental Medicine, Siberian Branch of the Russian Academy of Sciences,
630090 Novosibirsk, Russia
2
Novosibirsk State University, 630090 Novosibirsk, Russia
a
e-mail: lavrik@niboch.nsc.ru
Received October 14, 2023
Revised February 19, 2024
Accepted February 22, 2024
AbstractChromatin is an epigenetic platform for implementation of DNA-dependent processes. Nucleosome,
as a basic level of chromatin compaction, largely determines its properties and structure. In the study of nucleo-
somes structure and functions physicochemical tools are actively used, such as magnetic and optical “tweezers”,
“DNA curtains”, nuclear magnetic resonance, X-ray crystallography, and cryogenic electron microscopy, as well as
optical methods based on Förster resonance energy transfer. Despite the fact that these approaches make it pos-
sible to determine a wide range of structural and functional characteristics of chromatin and nucleosomes with
high spatial and time resolution, atomic force microscopy (AFM) complements the capabilities of these methods.
Theresults of structural studies of nucleosome focusing on the AFM method development are presented in this
review. The possibilities of AFM are considered in the context of application of other physicochemical approaches.
DOI: 10.1134/S0006297924040072
Keywords: nucleosome, AFM, chromatin, single-molecule methods for studying biomolecules
Abbreviations: AFM, atomic force microscopy; cryoEM,cryogenic electron microscopy; DREEM,dual resonance frequency
enhanced electrostatic microscopy; FRET,Förster resonance energy transfer; HS-AFM,high-speed atomic force microscopy;
PARP,poly (ADP-ribose) polymerase; ssNCP,nucleosome with a single-stranded DNA.
* To whom correspondence should be addressed.
# These authors contributed equally to this work.
INTRODUCTION
DNA molecules are used by cells for storage and
implementation genetic information. In eukaryotic
cells, DNA is predominantly present in a chromatin
composition, and both the level of chromatin compac-
tion and chromatin spatial organization are important
[1]. The basic level of DNA compaction is nucleosome,
a complex consisting of eight histones and 147-bp DNA
with its structure defining properties of chromatin to
a large extent. The first ideas about the nucleosome
structure were formulated in the middle of the 1970s
[2-4]. Schematic representation of the nucleosome struc-
ture is shown in Fig.1.
To date, main characteristics of the composition
and structure of nucleosome, as well as its molecular
dynamics, have been studied in sufficient detail. This
knowledge was obtained largely due to the use of mod-
ern physicochemical research methods, including sin-
gle-molecule techniques such as optical and magnetic
tweezers, DNA curtains, an optical approach based on
Förster resonance energy transfer (FRET), etc. [5-7].
These methods enable to measure a wide range of be-
havior parameters of biomolecules and their complex-
es, including chromatin and nucleosomes, with high
spatial and time resolution.
Along with the listed methods, the technique of
atomic force microscopy (AFM) is actively used. AFM
is based on monitoring of the probe interaction with
the surface. A probe in the form of a needle at the end
of the cantilever scans the sample. To detect change in
the vertical coordinate of the probe, a laser directed
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Fig. 1. Nucleosome core particle structure (PDB ID: 1KX5). Spatial structure of nucleosome is shown as a ribbon diagram in two
projections.
at the cantilever and a photodetector recording the
reflected beam are used. The beam reflected from the
cantilever shifts according to the vertical displacement
of the probe. Force of the cantilever interaction with
the surface can be assessed based on the signal from
the photodetector. Then, depending on the scanning
mode, these data enable to obtain information on ver-
tical coordinate of the sample surface directly or in-
directly through the feedback mechanism. At present
there is a wide variety of scanning modes and variants
of scanning protocols developed.
CONTACT MODE AFM
The first nucleosome images were obtained using
contact mode AFM, during which the probe-surface
repulsive force regulated by the feedback loop [8, 9]
is recorded (Fig.2a). The authors of these works were
able to show polynucleosomal structure in the form of
“beads on a string” [8, 9]. In addition, main geometric
parameters of the nucleosome disk were determined:
its height and diameter, which were ~3 and ~32 nm, re-
spectively, not including radius of the probe curvature,
[9], as well as the number of DNA supercoil turns in
the nucleosome [9].
The contact mode is characterized by a relatively
large mechanical effect of the cantilever on the sur-
face, which leads to severe deformation and damage
to nucleosome samples during scanning. In addition,
this “hard” scanning mode requires the use of probes
with a curvature radius of at least 10nm, which, as a
whole, reduces sensitivity and accuracy of the mode.
As a result, the first nucleosome images obtained by
AFM contact mode are of a low quality, which largely
limited the use of this method in studying nucleosome
structure.
TAPPING MODE AFM
Introduction of the tapping mode AFM provided a
way to reduce significantly deformation of the sample
during scanning, which made it possible to use sharp-
er probes. In this mode, the cantilever oscillates at its
resonant frequency. The feedback loop records chang-
es in the cantilever oscillation parameters and corrects
the probe position relative to the surface, providing
an equilibrium position around which the cantilever
performs harmonic oscillations (Fig.2b). Such chang-
es dramatically increased resolution of AFM in exam-
ining biological molecules. In particular, Martin et al.
[10] demonstrated advantages of this scanning mode
over the contact mode in studying chromatin struc-
ture. In their work, the authors managed to determine
the size of nucleosome more accurately than in the
case of using contact mode by employing the tapping
mode. By using the tapping mode of AFM, height and
diameter of the nucleosome disk were determined
as 4.3 ± 1.2 nm and 23.2 ± 4.5 nm, respectively, which,
considering radius of the probe curvature, are close
to the values obtained by X-ray crystallography [11].
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Fig. 2. Schematic representation of AFM scanning modes exemplified with a device with position of a piezo scanner at the
bottom. a)Contact mode; b)tapping mode; c)non-contact mode; d)electrostatic AFM. Designations: FB,feedback; C,computer;
AC,alternating current; DC,direct current.
Moreover, use of this approach enabled visualization
of DNA in the linker region of chromatin (which was
impossible with the contact mode scanning) as well as
to confirm experimentally the nucleosome structure
calculated by means of mathematical modeling [12].
The use of tapping mode AFM by Qian et al. [13]
in their study of chromatin from the chicken red blood
cells made it possible to visualize different levels of
DNA compaction. Both individual nucleosome “beads”
and their clusters on DNA strands were demonstrat-
ed on the obtained images. Presence of the sites with
different DNA packing densities allowed the authors
to suggest the role of compaction in the regulation of
gene expression. In this work, geometric character-
istics of fibrils that have diameter of 15-60 nm were
determined, confirming the solenoid model of nucleo-
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BIOCHEMISTRY (Moscow) Vol. 89 No. 4 2024
some packaging. In addition, it has been shown for the
first time that the fibrils of lower compaction degree
(~30 nm) are further folded to form chromatin struc-
tures of higher order (~60 nm), which, in turn, fold
into even more highly organized chromatin structures
(~90-110nm or more).
Design of nucleosome-positioning DNA sequences
[14], characterized by the unambiguous location of the
nucleosome core on the DNA molecule and high stabil-
ity of the formed complexes, enabled to create mod-
el structures with predicted location of nucleosomes.
Use of such nucleosome-positioning DNA sequences
made it possible to show stochasticity of nucleosome
location in the natural chromatin using telomeric sites.
These results confirmed the corresponding theoretical
model of nucleosome positioning [15].
AFM is actively used to study effects of various
histone variants, their post-translational modifications,
and epigenetic DNA modifications on the nucleosome
structure. Histone tail modifications are the key factor
in regulation of both chromatin and cellular homeo-
stasis dynamics. A hallmark of an active chromatin is
hyperacetylation of histones, which likely results in a
more open chromatin structure. It was shown in the
work of Hizume et al. [16] by AFM that histone hyper-
acetylation causes decrease in the thickness of chro-
matin fibrils from HeLa cells. This result allowed to
confirm a model of chromatin decondensation based
on electrostatic interactions. Biotinylation, on the con-
trary, promotes chromatin condensation. In the works
by Filenko et al. [17] and Singh et al. [18] the use of
AFM made it possible to demonstrate that biotinyla-
tion of H4 histone at lysines 12 or 16 leads to compac-
tion of the nucleosome structure, which is manifested
by the increase in the number of DNA turns around
the histone octamer.
Histone replacement with variants, as well as
the nucleosome movement along the DNA molecule,
are the basic mechanisms for regulating chromatin
compaction, which, as a rule, are due to the work of
remodeler proteins. RSC (“remodeling the structure
of chromatin”) is an ATP-dependent protein complex
of chromatin structure remodelers that is homolo-
gous to the human SWI/SNF (“switch/sucrose non-fer-
mentable” family of chromatin remodeling complex-
es) and mediates the nucleosome shift. Some details
of its functioning were shown using the tapping mode
AFM. In particular, it was found out that RSC moves
nucleosome along the DNA until another nucleosome
is reached or the break in the DNA chain is encoun-
tered[19].
Comparative analysis of the results of studies on
the structure of nucleosome complex with the H3 his-
tone variant (CENP-A) performed using AFM allowed
to propose an alternative model of DNA folding in the
centromeric region of chromosomes. This model in-
volves DNA folding in the centromeric region as an ar-
ray of parallel sites in the form of a “snake” instead of
the characteristic canonical nucleosome zigzag folding
[20]. The study of nucleosome structural features by
AFM involving replacement of H2A core histone with
its recently discovered H2AL2 version of the mouse
histone, expression of which is associated with sper-
matogenesis, showed, that the DNA length in the nu-
cleosome decreases from 147 to 130 bp [21]. Shorten-
ing of the DNA in the nucleosome composition is due
to relaxation of its structure by partial unwrapping.
In the same work it was also shown using cryogenic
electron microscopy (cryoEM) that nucleosomes with
H2AL2 have a more relaxed structure with a larger an-
gle value between the DNA linker regions, which is in
agreement with the data obtained by the AFM method.
It is worth paying attention to the fact that the nucle-
osome becomes resistant to the action of such remod-
eler proteins as RSC and SWI/SNF in the process. Bio-
logical significance of this modulation of nucleosome
properties remains the subject of research.
Nucleosome structure may be modulated by bind-
ing of a protein or a protein complex. One of the most
illustrative examples is the study investigating the ef-
fect of the H1 linker histone on a nucleosome compac-
tion. Using the capabilities of AFM, it has been shown
Fig. 3. Images obtained by using the tapping mode AFM. a)Nucleosome; b)nucleosomes with PARP3 protein.
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that H1 does not affect the degree of nucleosome com-
paction, but significantly stabilizes it, reducing struc-
ture fluctuations [22]. In our work on the influence of
nuclear proteins poly(ADP-ribose) polymerases 1,2,
and 3 (PARP1, PARP2, and PARP3) on the degree of nu-
cleosome compaction, it was found by AFM that PARP3
contributes to compaction of the structure of mono-
nucleosomes [23] (Fig. 3,a andb). PARP1, PARP2, and
PARP3 take part in the most DNA-dependent processes
including regulation of the DNA transcription and DNA
repair. At the same time, they catalyze the reaction of
ADP-ribose moieties transfer to the target proteins us-
ing NAD
+
as a substrate in response to genomic DNA
damage. PARP3 catalyzes the mono(ADP-ribosyl)ation
reaction, while PARP1 and PARP2 catalyze synthesis
of the poly(ADP-ribose). In addition, unlike PARP1 and
PARP2, PARP3 does not interact with the HPF1 his-
tone ADP-ribosylation factor [24]. Using AFM, we were
able to establish a previously unknown feature of the
PARP3 functioning, in particular, its influence on the
nucleosome structure, which may indicate the role of
this protein in regulating chromatin structure. In this
work, catalytic reaction of the PARP enzymes proteins
on nucleosomes has not been investigated, but other
researches have observed synthesis of poly(ADP-ri-
bose) catalyzed by the PARP1 and PARP2 proteins on
the extended DNA substrates by the AFM method [25,
26], which indicated the possibility of similar studies
in the case of nucleosomes.
NON-CONTACT MODE AFM
Another modification of the AFM is the non-con-
tact mode AFM. It is based on the detection of changes
in attractive forces caused by van der Waals interac-
tions between the probe and the surface, which allows
scanning without the need for direct contact of the
cantilever with the sample. While realizing this mode,
the cantilever oscillates with low amplitude at a fre-
quency exceeding its resonant frequency, which leads
to the increase in sensitivity compared to the tapping
mode AFM. Scanning nucleosomes using this mode en-
abled to obtain an image with a resolution that even
exceeded capabilities of cryoEM at the time of this
work publication [27]. However, despite the impres-
sive advantage, this scanning mode has not been wide-
ly adopted due to technical limitations. For example,
scanning in the above-mentioned work of Davies etal.
[27] was performed under a deep vacuum. It should
be noted, that analysis of biomolecules and their com-
plexes is preferable to be carried out in a solution to
facilitate interpretation of the results, which is incom-
patible with operations under vacuum. In addition,
vacuum conditions limit the study of dynamics of the
investigated complexes.
Taking into account the limitations arising during
implementation of the non-contact mode and low
quality of the images that can be obtained by the con-
tact mode, today the tapping mode AFM has become
the most widespread in the study of biomolecules.
Moreover, such AFM variants as MAC mode, PeakForce
mode, high-speed mode, as well as electrostatic AFM
are also based on the tapping mode AFM.
MAC MODE AFM
An alternative to the classic tapping mode is the
MAC mode (magnetic alternating current mode AFM),
the principles of which are based on excitation of the
cantilever oscillations by magnetic field of the coil
located under the sample [28]. The use of MAC mode
provides lower force impact on the sample than the
classic tapping mode of AFM, which contributes to
maintaining sharpness of the cantilever tip and im-
proves quality of the resulting image. For example,
methylation of the nitrogenous base C in the CpG se-
quences has been shown to result in a tighter chroma-
tin packaging in the presence of the H1 linker histone
precisely using the MAC mode [29]. These results sug-
gested a mechanism for a transcription regulation in
large chromatin domains through methylation.
Further development of this scanning mode in-
volved modification of the cantilever with an affinity
agent; for example, an antibody, which allowed to com-
bine a topographic study of the surface with molecular
recognition of the objects in real time (PicoTREC AFM)
[30,31]. When the probe contacts the sample, the sur-
face relief is recorded, and presence of the antigen at
the scanning point could be detected from the change
of the amplitude of cantilever oscillations. The use of
this approach made it possible [32, 33] to demonstrate
the mechanism of action of the SWI/SNF chromatin
remodeler. In particular, SWI/SNF has been shown
to promote removal of the H2A histone from nucleo-
some, resulting in relaxation of the nucleosome struc-
ture and accompanied by the release of ~80bp DNA.
These results enabled characterization of the changes
in geometric parameters of the nucleosome in the case
of H2A histone deletion, although, there are data ob-
tained earlier by immunoprecipitation, quantitative
PCR, and gel electrophoresis, indicating that the H2A/
H2B histones are deleted from nucleosome under the
action of SWI/SNF chromatin remodeler [34, 35].
PEAKFORCE TAPPING MODE AFM
A non-resonant scanning mode developed by
Bruker (USA), PeakForce Tapping mode AFM, is one of
alternative modifications among the scanning probe
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Fig. 4. A cluster of nucleosome particles [37]. Three clusters of nucleosome particles are shown in the AFM image. Two lines(1,2)
are marked. The inset in the upper left corner shows height profiles for each line(1 and2) along the measured distance. The first
profile (black line) crosses DNA and shows height and width of the double-stranded DNA. The second profile (red line) crosses
the identified nucleosome.
AFM technologies, which is promising for studying bi-
ological molecules [36]. Implementation of this mode
includes contact of the cantilever with the sample
surface at a frequency significantly lower than the
resonant one, which enables to consider such kind of
contacts as a quasi-static process, and the signal is re-
corded as a fixed maximum contact force of the sam-
ple with the probe. This scanning mode additionally
reduces the force of cantilever impact on the sample
and allows topographic studies of “soft” objects to be
carried out with great accuracy. Using this mode of
AFM for the first time allowed to obtain nucleosome
images in solution without using vacuum with resolu-
tion approaching the resolution demonstrated by the
X-ray crystallography (Fig. 4) [37].
McCauley et al. [37] in their study uniquely iden-
tify nucleosomes from the height ~5.5 nm and diame-
ter ~1nm, which correlates with the data obtained by
X-ray crystallography (height was 5.7 nm; diameter
was 11 nm) [11]. Such high resolution allowed estab-
lishing that the non-histone proteins Nhp6A and Hmo1
of chromatin from the HMGB family destabilize the
nucleosome structure with release of the part of DNA,
and perform this in different ways. Hmo1 was shown
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BIOCHEMISTRY (Moscow) Vol. 89 No. 4 2024
to relax the nucleosome structure more than Nhp6A,
which is highly consistent with peculiarities of local-
ization of these proteins on chromatin. Hmo1 is con-
centrated in a highly transcribed histone-depleted
region enriched with the genes of translational ap-
paratus, where high DNA compaction is not needed,
while Nhp6A is localized in the rest of euchromatin.
ELECTROSTATIC AFM
Special attention should be paid to the scanning
probe microscopy techniques that allow to determine
electrostatic potential of a surface. They proved to be
significantly more informative for studying biomole-
cules after the single-pass scanning options were op-
timized by using the resonant cantilever frequencies
at two harmonics. Implementation of this approach
made it possible to increase dramatically sensitivity
of the method [38]. Depending on the implementation
features, the Kelvin probe force microscopy (KPFM)
[38] and the dual resonance frequency enhanced elec-
trostatic microscopy (DREEM) [39] are distinguished.
Fig. 2d shows principle of signal acquisition with
KPFM and DREEM.
DREEM allows minute changes in the electrostatic
force gradient to be detected at high resolution, mak-
ing it a powerful tool for characterizing the structure
of protein-nucleic complexes at the single-molecule
level. DREEM enables visualization of DNA located
both on the surface and inside the protein-nucleic
complex, as well as DNA in the composition of large
heterogeneous complexes with several proteins. This
approach has a great potential in studying the struc-
ture of both single nucleosomes and nucleosomes in
more complex systems.
The research of Wu et al. [39] is devoted to demon-
strating capabilities of the DREEM method to study
location of a DNA molecule in large multi-protein
complexes. A nucleosome was chosen as the example.
On the one hand, the authors showed that the over-
all topographic images of nucleosomes obtained by
DREEM and other AFM methods are the same. On the
other hand, the DREEM images demonstrate regions
with reduced intensity in the nucleosome core region
location of which correlates well with the trajectory
of DNA location in the nucleosome according to the
X-ray crystallography data (Fig. 5). This fact confirms
the validity of this approach and of the results inter-
pretation.
Fig. 5. Topographic images of nucleosomes obtained by AFM and DREEM [39]. Topographic (a, 1; b, 1) DREEM phase images
(a, 2; b, 2) and DREEM amplitude (a, 3; b, 3) of nucleosomes showing how a DNA molecule is wrapped around histones once.
c,topographic(1) and DREEM phase images of the nucleosome(2) showing that DNA is wrapped around the nucleosome twice.
Theinsets show height profiles along the line drawn through the nucleosome in topographic (c, 1) and DREEM images (c, 2).
Twodots in the graphs correspond to positions of the two dots shown on the line that mark position of the peaks correspond-
ing to DNA in the DREEM image. Schematic models of histone-wrapping DNA are shown in each DREEM image (not-to-scale
models). Crystal structure of the nucleosome superimposed on the DREEM-phase image is shown in the inset to the phase image
on thepanel(c,2)
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Fig. 6. Topographic AFM and DREEM images of repair complexes of mismatch repair nucleotides on 2-kb long DNA containing
mismatch repair GT nucleotides [39]. a)Spatial model of the Taq MutS crystal structure (created based on PDB: 1EWQ). Subunits
A, B, and DNA are colored blue, gold, and light blue, respectively. MutS bends DNA by about 60° as it passes through the DNA
binding channel. b)Topographic AFM (b, 1), as well as DREEM-phase(b, 2) and amplitude (b, 3) images of the Taq MutS-DNA
complex. c)Superimposing the of complex model on AFM images (c, 1) and to phase images (c, 2). d)Topographic AFM (d, 1) and
DREEM phase (d, 2 and 3) images of a large complex of MutSα-MutLα-DNA containing ~10 proteins. The DNA pathway is identi-
fied as the regions with the greatest reduction in the magnitude of DREEM signals, compared to the one protein, and marked on
the inset (d, 3) in blue color; MM, expected position of mismatched nucleotides.
As the second model, Wu et al. [39] used a multi-
protein complex of non-complementary base pair of
human DNA repair system consisting of MutSa and
MutLa. Application of DREEM allowed visualization of
location of the DNA containing a non-canonical pair of
nucleotides in the composition of this complex (Fig.6).
This model is designed to demonstrate applicabil-
ity of the method for determining location of the DNA
inside a protein complex. The obtained results were
included in the work devoted to studying the MutSa
and MutLa complex functioning [40].
The same approach was used by Adkins et al. [41]
to confirm the structure of nucleosome-like particles
reconstructed using single-stranded DNA (ssNCP).
Using DREEM, it has been shown that ssNCPs have a
structure and a size similar to the parameters of ca-
nonical nucleosomes, in particular, have a disk-like
shape and contain the same number of turns of the
single-stranded DNA on the histone octamer [41].
The authors of this research suggested that the his-
tones released from nucleosome composition during
the initial stages of the DNA double-strand break re-
pair process can bind to the single-strand DNA re-
gion. The possibility of reconstitution of ssNCP invitro
has been shown. ssNCPs proved to be more dynamic
than the canonical nucleosomes and capable of ATP-
independent transfer to other regions of one- or double -
-stranded DNA. Moreover, such ATP-dependent nucleo-
some remodelers as RSC and Fun30 bind effectively to
ssNCP and become activated. Based on these results,
the authors have suggested that ssNCP could be a
marker of various cellular processes accompanied by
formation of single-stranded DNA regions, and emer-
gence of these structures could be used to regulate one
or another specific cellular process.
Despite the impressive capabilities of this approach,
it has a number of technical limitations primarily re-
lated to high requirements for the quality of cantile-
vers, which must simultaneously have high sharpness
and sufficient conductivity to obtain high-resolution
topographic and DREEM images [39].
DREEM makes it possible to visualize DNA con-
formation both on the surface and within individual
protein–DNA complexes, as well as within the compo-
sition of large heterogeneous complexes with several
proteins. Ability of DREEMs to detect minute changes
in the electrostatic force gradient in combination with
high resolution makes it a powerful tool for character-
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BIOCHEMISTRY (Moscow) Vol. 89 No. 4 2024
izing structure of protein-DNA complexes at the single-
molecule level. This approach has a great potential in
studying structures of both single nucleosomes and
nucleosomes in more complex systems.
HIGH-SPEED AFM
One of the key disadvantages of the above-men-
tioned AFM modes is long time– required to obtain in-
dividual images. This feature of the method limits its
applicability for investigating dynamics of the process.
The first attempts to study dynamics of the process-
es involved the use of sequential samples scanning.
In this way, the data on the RNA polymerase moving
along DNA were obtained [42]. Using the same mode, it
was possible to demonstrate the process of nucleosome
“unwinding” [43]. Shlyakhtenko etal. [43] showed that
multiple continuous scans of the same nucleosome
field allowed eight images of the same nucleosome to
be obtained, demonstrating its transformations over
time. As a result, gradual “unwinding” of DNA from
the histone octamer culminating in the complete de-
struction of the complex was shown.
Further improvement of the method due to ap-
plication of a more productive device allowed the
Lyubchenko group to obtain more detailed data on
the dynamics of nucleosomes “unwinding” with the
H3 histone and its CENP-A centromeric version using
high-speed atomic force microscopy (HS-AFM) [44, 45].
The data obtained in these studies revealed such re-
laxation mechanisms of the nucleosome structure as
DNA bleaching, as well as the possibility of transloca-
tion of nucleosomes along DNA. The authors note that
dynamic rearrangements of centromeric chromatin
can occur in the absence of remodeling factors. At the
same time, CENP-A stabilizes nucleosome particles,
preventing complete histone dissociation during the
DNA loosening or unwrapping and ensuring rapid nu-
cleosome re-assembly during their core transfer [45].
Canonical nucleosome particles with H3 histone do
not demonstrate such plasticity, and rearrange only in
the presence of such remodeling factors as SNF2h [46].
Later some dynamics details of nucleosomes and chro-
matosomes were shown in the work by Onoa etal. [47]
using HS-AFM that clarified the mechanism of their
“unwrapping”. In particular, asymmetry of the nucle-
osome “unwrapping”, step-wise nature of the process
of histone heterodimers deletion from the nucleo-
some core, as well as lability of position of the histone
tetramer (H3-H4) × 2 in the dyad region have been
demonstrated in real time.
HS-AFM scanning made it possible to analyze dy-
namics of nucleoproteins and other biomolecule com-
plexes. An even greater increase in the scanning speed
is required to estimate kinetic characteristics of the
studied proteins. In the future, machine learning ca-
pabilities are likely be involved in achieving this goal.
Inthe study by Kato et al. [48] an approach based on
machine learning has been proposed to analyze inte-
grated simulation dynamics data from asynchronous
HS-AFM scanning. Peculiarity of the described ap-
proach is that in this case asynchronous nature of the
single passes during scanning is considered. Thus, this
method with appropriate resampling frequency has
been shown to be a powerful tool for assessing dynam-
ic behavior of the object based on the low spatial and
time resolution HS-AFM data.
COMPARISON OF AFM CAPABILITIES
WITH SOME PHYSICOCHEMICAL APPROACHES
IN NUCLEOSOME STUDIES
During the research of nucleosome structure and
functioning, including dynamics studies, a number of
physicochemical research tools are used, such as: mag-
netic and optical “tweezers”, “DNA curtains”, nuclear
magnetic resonance, X-ray crystallography analysis,
and cryoEM, as well as approaches based on FRET op-
tical methods. These methods provide a wide range of
detectable parameters with high spatial and time res-
olution.
One of these approaches that have become widely
used is based on optical tweezers that allow to apply
mechanical force directly to the molecule or complex
under study and simultaneously measure elongation
of the object. Strength of the nucleosome complex [49]
was first determined by this method. Magnetic twee-
zers which in addition to stretching can generate rota-
tional movement of an object, allowed creating model
DNA structures with supercoiling. In the work of Gupta
et al. [50] it was shown that intramolecular stress oc-
curring in the structure of DNA with positive super-
coiling alters its conformation, compared to the DNA
without supercoiling making nucleosome formation
less effective.
Nevertheless, applicability of both approaches is
limited to measuring changes of the object linear char-
acteristics and amount of the applied force. Combin-
ing these methods with fluorescence microscopy en-
hances greatly the possibilities for the researchers, but
still prevents investigation of conformational changes
within the complex. Employment of fluorescence mi-
croscopy in the FRET mode, a non-radiative mode of
transferring energy between fluorophores, partial-
ly release this limitation, however, conformational
changes recorded by this method could not be always
interpreted clearly. Despite this fact, use of FRET tech-
nique is a powerful tool for studying the structure and
conformational dynamics of protein-nucleic complexes.
For example, use of FRET allowed Andreeva et al. [51]
STRUCTURE AND FUNCTIONS OF NUCLEOSOMES BY AFM 683
BIOCHEMISTRY (Moscow) Vol. 89 No. 4 2024
to record the effect of buffer components on nucleo-
some structure. In particular, the stabilizing effect of
potassium ions has been shown, and this stabilization
of the nucleosome structure has also been demonstrat-
ed to create a barrier for such ATP-independent pro-
teins/complexes as FACT and PARP1.
Another approach facilitating examination of the
protein complexes with nucleic acids is based on for-
mation of a nanobarrier on the substrate surface,
which ensures anchoring of DNA molecule with for-
mation of DNA curtains. Nucleosome DNA curtains are
a unique system allowing to track behavior of thou-
sands of individual nucleosome particles containing a
fluorescent label in real time. The use of this approach
made it possible to monitor dynamics of DNA compac-
tion by condensinsI and II, as well as to clarify mech-
anistic model of chromatin loop formation by yeast
condensin and human cohesin [52-56]. Visnapuu and
Greene [57] were able to determine energy landscape
of the nucleosome localization on DNA and confirm
theoretical predictions based on the model designed
using this approach. In addition, in the same work, po-
sitions of the nucleosome assembly sites were shown
to correlate with the regulatory transcription regions.
Unfortunately, this approach does not allow investi-
gating explicitly structural changes within the nucleo-
somes themselves induced by various factors.
One of the most powerful tools in studying the
structure of biopolymers is the X-ray crystallography.
Atomic structure of nucleosome has been determined
using X-ray crystallography a long time ago [58]. De-
spite the high resolution, applicability of this method
is severely limited. Limitations are largely due to the
need to grow a crystal, which does not enable study-
ing dynamics of structural changes. Moreover, obtain-
ing a crystal is on itself not a trivial task, while the
image quality directly depends on the crystal quality.
Thetask is further complicated in the case of investiga-
tion of the structure of protein complexes with nucle-
ic acids, especially of such complexity as nucleosome,
and even more so chromatin. Obtaining a X-ray-suit-
able crystal is also difficult if the studied polymer
contains unordered regions in its composition. In ad-
dition, possible difference between the protein struc-
ture in the crystal and that in the solution should be
considered while interpreting the X-ray crystallogra-
phy data. The difficulties of decoding the obtained pri-
mary data should be also mentioned, it introduces ad-
ditional limitations on the size of the object selected
for research.
At present, cryoEM allows obtaining structures
with resolution approaching the X-ray crystallography
data. For example, in the study by Markert et al. [59]
an image of nucleosome associated with complete his-
tone deacetylation complex Rpd3S was obtained using
cryoEM with final resolution of 2.8 Å. This method is
deprived of some limitations specific to X-ray crys-
tallography. For example, cryoEM allows studying
proteins with unordered structures, while they are
difficult objects to investigate with X-ray crystallog-
raphy. Nevertheless, the use of this method has some
limitations. CryoEM works best for studying large ob-
jects over 200 kDa. Like X-ray crystallography, cryoEM
is poorly adapted to study conformational dynamics.
The achievements of recent years have provided a
possibility of time-resolution analysis in the range of
milliseconds to seconds, which allows studying con-
formational dynamics of the structure, but is hard-
ly applicable to studying such large-scale changes in
the structure as nucleosome translocation or its core
transfer.
Analysis of the biomolecule conformational dy-
namics including of their complexes such as a nu-
cleosome could be performed by NMR spectroscopy.
Advances in solution NMR spectroscopy have allowed
monitoring conformational dynamics of both the
bounded core of histones and their free N- and C-tails
[60]. Solid-state NMR techniques represent additional
tools of nucleosome research [61]. For example, second-
ary structure of the H2B histone in nucleosome was
obtained using solid-state NMR, which was consistent
with the structure obtained by X-ray crystallography.
The authors were able to show dynamic interactions
of H2B histone with H4 histone, as well as with DNA
[62]. Applicability of this method is mainly limited by
the need to introduce isotopes of different elements
into the sample for unambiguous interpretation of the
spectra. Thus, in the work of Shi etal. [62] the histone
containing
13
S and
15
N isotopes was used.
The use of AFM largely complements the data ob-
tained using the above-described approaches. In par-
ticular, AFM facilitates determination of geometric
parameters of nucleosomes, as well as their changes
due to nucleosome interactions with various protein
factors or histone replacements with their variants,
as has been shown in a case of H3 replacement with
CENP-A. The possibility of scanning in a liquid medi-
um allows simulating conditions closer to physiologi-
cal ones, and development of the high-speed scanning
made it possible to observe relaxation dynamics of the
nucleosome structure. Using the capabilities of electro-
static force microscopy facilitated observation of the
trajectory of DNA folding in the composition of nucle-
osome.
One of the considered AFM advantages is the
possibility of using this technique for investigation of
complex macromolecular structures, such as chroma-
tin fragments or model polynucleosomal fragments
[15, 63]. Investigation of such objects using FRET or
tweezers could be limited by the need to add fluo-
rescent labels or microspheres into the tested sample
structure.
UKRAINTSEV et al.684
BIOCHEMISTRY (Moscow) Vol. 89 No. 4 2024
CONCLUSION
Rapid development of AFM as a method of study-
ing complex protein-nucleic systems allowed to deepen
significantly understanding of the nucleosome struc-
ture. Importance of the scanning environment during
the AFM application should be emphasized. Itis well
known that implementation of AFM under vacuum
conditions has a positive effect on image quality. How-
ever, in order to simplify interpretation of the results,
it is preferable to carry out scanning in an aqueous en-
vironment when studying biomolecules. Drying of bio-
molecules like DNA, proteins, or their complexes leads
to disruption of their spatial structure [64]. In addi-
tion, scanning in an aqueous environment is necessary
to study dynamics of the processes. At the same time,
implementation of AFM in a liquid is accompanied by
a number of technical difficulties, in particular it lim-
its of the range of used substrates and methods for im-
mobilization of scanned objects, as well as it increases
requirements for cantilevers preparation.
AFM capabilities are likely to be enhanced by the
development and implementation of machine learn-
ing for primary data processing. This approach would
reduce the level of “noise” when scanning at the soft-
ware level and increase accuracy of the measurements
provided AFM. In addition, performance improvement
at the software level would increase the scan speed.
Some approaches based on the AFM technique
were not widely used so far for studying nucleosomes
should be noted. For example, combination of fluores-
cence microscopy and AFM could be used for studying
interactions of protein molecules or their complexes
with the substrates in the form of nucleosomes or
chromatin. At the same time, the AFM-derived data
on the sample topology could allow to localize inter-
action area in the protein complex with the substrate,
and the fluorescence data could facilitate identifica-
tion of the labeled molecule. A similar approach was
used by the Wyman group to investigate homologous
recombination [65].
Wide use of the combination of AFM and fluo-
rescence techniques is primarily limited by the need
to use a substrate which would be atomically smooth
while being optically transparent. At present, prepa-
ration of such substrates is a non-trivial task; one of
these solutions has been suggested by Rahman et al.
[66]. This problem is likely to be solved in the future,
opening up opportunities to an arsenal of fluorescence
detection-based approaches, including FRET and fluo-
rescence polarization combined with AFM.
Implementation of electrostatic force microscopy
in a liquid medium could significantly contribute to
studying dynamics of conformational DNA changes in
the protein-nucleic complexes including nucleosome
or chromatin. At present, measuring electrostatic po-
tential of biological molecules in liquids is limited by
high dielectric constant of the medium, by the possi-
bility of a solvate shell forming on the sample surface,
as well as by shielding the probe and sample surfaces
with solution ions. Nevertheless, some studies show
the possibility of using electrostatic force microscopy
of solid materials at low ionic strength [67, 68]. Scan-
ning electrostatic potential in liquid increases de-
mands primarily on cantilever preparation. It should
not only meet all the cantilever requirements for elec-
trostatic force microscopy in DREEM mode, but also
have a dielectric coating on the probe surface, exclud-
ing the area that is in direct contact with the sample.
Apparently, further development of the method asso-
ciated with increase in the device sensitivity would fa-
cilitate measurements of electrostatic potential of bio-
molecules in liquid.
In conclusion, it should be added that studies of
the last decade have dramatically changed the views
on the structure of chromatin and its basic unit, nu-
cleosome. The static image is now complemented by
the dynamic one, and methods providing the ability to
study single molecules have played an important role
in characterizing dynamic properties of nucleosomes.
The use of AFM offers an opportunity to characterize
a complex supramolecular system at the nanoscale,
allowing direct visualization of the structural features
of nucleosomes and changes within it such as, for ex-
ample, the process of their unwrapping. In addition,
the possibility of using small amounts of biopolymer
preparations is a favorable feature of AFM measure-
ments in comparison with some other methods.
Acknowledgments. The authors express their
gratitude to A. A. Lomzov and E. A. Belousova for a con-
sultation and productive discussions during the manu-
script preparation.
Contributions. A.A.U. and M.M.K. developed the
concept of the review and prepared the manuscript;
O.I.L. supervised the study and edited the manuscript.
Funding. This research was funded by the Rus-
sian Science Foundation (project no. 22-74-10059)
and State Budget Project of Institute of Chemical Bi-
ology and Fundamental Medicine No. 121031300041-4
(forO. I. Lavrik).
Ethics declaration. This work does not describe
any studies involving humans or animals as objects
performed by any of the authors. The authors of this
work declare that they have no conflicts of interest
infinancial or any other sphere.
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