Results
AND DISCUSSION
Fluorescent silica nanoparticles (SiNPs) , doped with the dye A TTO 633 , were
successfully synthesized as spherical structures, with a mean diameter of 135 ± 16 nm
determined from the analysis of 250 individual particles by STEM imaging ( Figure S1,
Supporting Information ). The obtained size range (<200 nm) is particularly relevant for
biomedical applications, as it favors efficient cellular uptake and intracellular trafficking 35.
The overall experimental workflow is illustrated in Figure 1a, where SiNPs were coated with
bovine serum albumin (BSA) to form a protein corona , thereby improving biocompatibility
by reducing cytotoxicity while enhancing the cellular uptake16,32. Cells were then incubated
with these BSA-coated SiNPs for controlled periods, washed, and analysed at different time
points, enabling us to monitor the intracellular distribution of nanoparticles across successive
cell divisions. The framework represents the experimental model adopted in this study,
relating nanoparticle concentration to post -exposure time, during which increasing cell
number reflects ongoing proliferation (Figure 1b). By systematically varying nanoparticle
concentration and post-exposure time, we correlated the extent of SiNPs internalization with
cell proliferation dynamics, providing mechanistic insight into the redistribution of
nanoparticle load during the mitotic cycle .
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Figure 1. Experimental workflow and conceptual framework. a) 1- SiNPs are treated with BSA for 8
minutes to form a protein corona . 2 - SiNPs are incubated in RAW 264.7 cells for 1 h, subsequently
washed with phosphate buffered saline (PBS), and analysed at different time points . b) Schematic
representation of SiNP s distribution as a function of nanoparticle concentration and post -exposure
time. The increase in cell number arises from proliferation along the time axis.
Understanding how nanoparticles interact with immune cells is essential for
predicting their biological behavior and long -term in vivo fate. Regardless of their intended
biomedical application, SiNPs inevitably encounter immune cells, which serve as the first
line of recognition and clearance of foreign materials 36,37. To evaluate how nanoparticle load
influences cellular responses, RAW 264.7 macrophages were exposed to three SiNP s
concentrations (0.003, 0.03, and 0.3 mg/mL). This range was selected to capture potential
dose-dependent effects on internalization efficiency, vesicular organization, and overall
intracellular distribution 38. Flow cytometry (Figure S5 Supporting Information) was used to
quantify nanoparticle uptake across the three tested concentrations. Cells were stained with
propidium iodide (PI) while SiNP s (containing ATTO 633) w ere detected in the APC
channel, enabling discrimination between nanoparticle -positive (ATTO +PI) and
nanoparticle-free (PI) populations. At the lowest concentration (0.003 mg/mL), only 79.6%
of cells were nanoparticle-positive (Figure S5c), indicating limited extracellular availability.
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This incomplete initial loading leads to progressive dilution of nanoparticles and a decrease
in the fraction of nanoparticle -positive cells across successive divisions. In contrast, at 0.03
and 0.3 mg/mL, nearly all cells contained SiNPs at the initial time point (Figure S5a, b). This
near-uniform loading ensures that most cells retain nanoparticles after division, maintaining
a high fraction of nanoparticle -positive cells over multiple cell cycles. This strong
concentration dependence reflects the high pha gocytic activity of macrophages and their
capacity to modulate uptake in response to particle abundance 39,40.
A multimodal imaging strategy was used to resolve how intracellular nanoparticle
organization evolves with concentration. Confocal fluorescence microscopy provided an
initial overview of nanoparticle distribution after 1 h of incubation (Figure 2a). The AT TO
633 signal from the particles increased progressively from 0.003 to 0.3 mg/mL, reflecting the
higher nanoparticle availability in the extracellular medium and is consistent with the flow
cytometry results. To solve the ultrastructural context of these fluorescent signals, cryo-SXT
at B24 Beamline ( Diamond) was employed under near -native conditions (Figure 2b).
Tomographic slices revealed high -contrast dense objects, highlighted by orange arrows,
corresponding to SiNPs encapsulated within vesicles , indicating that across all
concentrations SiNPs were internalized via vesicular pathways 41,42. However, their spatial
organization strongly depended on nanoparticle dose. At low concentration, only a small
vesicle containing SiNPs w as detected in the cytoplasm. At intermediate concentration,
multiple vesicles containing SiNPs were observed in the cytosol . Notably, at the highest
concentration (0.3 mg/mL), large vesicular structures containing SiNPs were distributed
throughout the cytosol and within the nuclear region. This concentration -dependent
progression is summarized schematically in Figure 2c. Correlative cryogenic structured
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illumination microscopy (cryo -SIM) and cryo -SXT imaging further validated these
observations (Figure 2d). Cryo -SIM identified SiNPs (red) within vesicular compartments
that colocalized with lysosomal markers (blue), confirming their endolysosomal
confinement 41. Overlay with cryo-SXT showed that the colocalization of lysosomal and SiNP
signals corresponds to the high -contrast structures observed in the tomograms. Also, both
cryo-SXT and cryo -SIM revealed vesicle -encapsulated SiNPs located within the nuclear
region. Cryo-SIM confirmed that these particles remained enclosed by vesicular membranes,
excluding free diffusion into the nucleoplasm, as also confirmed by the fluorescence confocal
(Figure 2a), where the white arrows point to the overlap of the nuclear and nanoparticle
signals. While nuclear localization has previously been reported mainly for ultrasmall
nanoparticles or systems engineered for nuclear targeting43–45, this observation demonstrates
vesicle-encapsulated access of non-functionalized silica nanoparticles larger than 100 nm to
the nuclear region, without nucleoplasmic entry. The combined X-ray and fluorescence data
suggest that this phenomenon arises from vesicle -induced deformation and invagination of
the nuclear envelope, rather than active transport through nuclear pores, consistent with
mechanical stress –induced nuclear envelope remodeling 46.
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Figure 2. Internalization and intracellular distribution of SiNPs in RAW 264.7 cells at different
concentrations. a) Fluorescence confocal micrographs of cells exposed to SiNPs at 0.003, 0.03, and
0.3 mg/mL (green : actin; blue: nucleus; red: SiNP ). b ) Slices from cryo -SXT tomographic
reconstructions. Orange arrows indicate internalized SiNPs. c) Schematic representation illustrating
the evolution of SiNP concentration inside macrophages as a function of exposure. d) Correlative
imaging combining cryo -SIM and cryo -SXT shows lysosomes (blue), mitochondria (green), and
SiNPs (red), followed by grayscale tomographic slices at 0.3 mg/mL and the merged image.
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Building upon these concentration -dependent results, we next examined how cell
proliferation dynamics influence nanoparticle redistribution across successive division
cycles. Determining the doubling time (DT) was crucial to ensure experimental
reproducibility, as cell growth rates can vary significantly between laboratories and culture
conditions. Monitoring DT also allowed normalization of exposure periods to the cells’
biological rhythm, enabling comparison across equivalent proliferative stages. Fluorescence
confocal and cryo-SXT imaging (Figure 3a –c) reveal a clear temporal evolution in SiNP s
intracellular distribution at 0.3 mg/mL concentration over two division cycles. At the initial
time (Figure 3a), SiNPs appear dispersed throughout the cytoplasm and within the nuclear
region, as indicated by white arrows, with minimal clustering. After the first doubling (Figure
3b), fluorescence intensity increased and small perinuclear aggregates emerged, indicating
progressive clustering of SiNPs , and cryo-SXT also revealed vesicles containing SiNPs
relocating away from the nuclear region. By the second doubling (Figure 3c) , SiNPs are
predominantly concentrated around the nucleus, forming distinct high -intensity clusters
consistent with late endosomal /lysosomal trafficking 9,41,42. Segmented cryo -SXT volumes
provide complementary ultrastructural confirmation of these patterns, highlighting both the
redistribution of SiNP -containing vesicles during cell division and their preferential
perinuclear accumulation. Correlative cryo-SIM and cryo-SXT analyses (Figure 3d) further
elucidate the subcellular context, revealing the spatial relationship between SiNPs (red) and
lysosomes (blue). After two division cycles, SiNPs remain confined within vesicular
membranes in the perinuclear region 47 suggesting that the observed redistribution results
from active vesicular transport and maturation rather than passive diffusion.
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Figure 3. Multimodal imaging of intracellular SiNP distribution across two cell -division cycles in
macrophages.(a–c) Fluorescence confocal micrographs (actin, green; nucleus, blue; SiNPs, red),
corresponding cryo–SXT tomographic slices, and segmented volumes corresponding to the evolution
of intracellular SiNP localization over time: a) initial time, b) first doubling time, and c) second
doubling time. d) Correlative cryo –SIM and cryo –SXT imaging of lysosomes (blue), SiNPs (red),
and mitochondria (green), followed by grayscale tomographic slices at the second d oubling time and
the merged correlation image.
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Furthermore, X-ray mosaic projections of whole cells obtained at Mistral Beamline
(Alba Synchrotron) (Figure 4a–c) extend this analysis to near–whole-cell volumes, showing
that at the initial time SiNP s-containing vesicles are broadly distributed throughout the
cytoplasm, whereas over successive division cycles they progressively concentrate toward
the perinuclear region. Three -dimensional rendered and segmented volumes obtained from
stitched cryo-SXT tomograms (Figure 4d–f) confirm this redistribution at the ultrastructural
level, revealing a gradual relocation of vesicle-confined SiNPs toward the nuclear periphery.
The schematic representations (Figure 4g –i) summarize this dynamic process, highlighting
the progressive perinuclear aggregation across division stages . Together, this whole -cell
perspective rules out local sampling effects and confirms that the observed perinuclear
accumulation reflects a global intracellular reorganization rather than a region -specific
phenomenon. This localization likely reflects a combination of endocytic processing, vesicle
trafficking, and sequestration mechanisms that preserve cellular homeostasis during
proliferation 47. Together, these findings demonstrate that SiNP intracellular organization is
dynamic and responsive to cell division, with progressive perinuclear accumulation
reflecting coordinated endocytic activity and stable vesicular entrapment 38. Such behavior
provides structural insight into how proliferative cells adapt to nanoparticle exposure,
revealing vesicular confinement as a key mechanism governing long -term nanoparticle
retention and intracellular fate.
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Figure 4. Time-dependent intracellular distribution of SiNPs at 0.3 mg /mL. ( a–c) X -ray mosaic
projections of whole cells at a) initial time, b) first doubling time, and c) second doubling time. Pink
and blue squares indicate adjacent, partially overlapping regions used for tomographic reconstruction.
(d–f) Three -dimensional rendered and segmented volumes obtained from stitched tomograms
corresponding to the regions highlighted in panels (a –c) at d) initial time, e) first doubling time, and
f) second doubling time. Highlighted structures include the cell nucleus (pink), vesicles (gold), and
SiNPs (cyan); the cell boundary is indicated by a purple contour.(g –i) Schematic representations
summarizing the progressive perinuclear aggregation of SiNP s-containing vesicles at g) initial time,
h) first doubling ti me, and i) second doubling time.
We next employed X -ray ptychography, an advanced configuration of coherent
diffractive imaging (CDI), to investigate these interactions at nanoscale resolution ,
particularly under higher SiNP concentrations. This technique provides quantitative, label -
free imaging based on phase shifts induced by variations in the specimen's electron density,
enabling visualization of dense intracellular regions that are otherwise inaccessible to
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conventional microscopy. To enable this analysis, a nuclear isolation protocol 48,49 was
developed to lyse the plasma membrane while preserving the nuclear envelope selectively. It
provides an essential means to investigate the potential structural influence of nanoparticle
exposure on the nucleus. The optimized treatment with 1% Triton X-100 for 3 min, followed
by glutaraldehyde fixation and critical-point drying, provided optimal preservation of nuclear
integrity and compatibility with coherent X -ray diffraction imaging (Figure 5a). The
experimental optical layout of the ptychography setup at Cateretê Beamline (Sirius) is
schematically illustrated in Figure 5b. Unlike conventional lens -based imaging, X -ray
ptychography reconstructs the complex electron density of a sample from overlapping
diffraction patterns acquired during a scanning sequence 28. Each illuminated position
generates an interference pattern (“speckle”), which is computationally processed through
iterative phase-retrieval algorithms 50 such as the Ptychographic Iterative Engine (PIE) 51 or
the Difference Map (DM)52 to recover both amplitude and phase information. When extended
to ptychographic X -ray computed tomography (PXCT)53, this approach enables three -
dimensional visualization of entire cells with spatial resolutions reaching tens of nanometers.
Despite its high resolving power, the application of X-ray ptychography to biological systems
remains challenging due to the intrinsically low scattering contrast of biological materials
and their susceptibility to radiation damage. However, recent advance s in beam coherence
and scanning stability (enabled by fourth -generation synchrotron light sources such as
SIRIUS)24,54,55 have begun to overcome these limitations, allowing high -resolution imaging
of intact cells. In this context, our study extends the use of ptychography to probe
nanoparticle–nucleus interactions in immune cells, providing a three-dimensional, nanoscale
view of how intracellular SiNPs influence nuclear architecture.
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Figure 5. Experimental workflow and ptychographic imaging setup. a) Stepwise preparation of SiNP-
treated cells for ptychography, including decellularization with 1% Triton for 3 min, fixation,
dehydration, and critical point drying. b) Schematic representation of the ptychography optical layout,
showing the path of the coherent X -ray beam through the sample membrane toward the detector.
Despite the higher radiation dose required, this approach enables detailed visualization
of nuclear morphology, subnuclear organization, and intracellular nanoparticle distribution
at different exposure times (Figure 6). The time-dependent intracellular distribution of SiNPs
revealed by X -ray ptychography is summarized in schematic representations of the spatial
organization shown in (Figure 6a, e, i, m ). Two-dimensional ptychographic reconstructions
revealed clear contrasts between the nucleus and cytoplas m (Figure 6b, f, j, n), with SiNPs
appearing (Figure 6f, j, n) as high-density domains surrounding and occasionally deforming
the nuclear envelope. These findings are consistent with the previously observed vesicle -
mediated internalization pathways, suggesting that mechanical interactions between enlarged
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endosomal vesicles and the nucleus may drive local invaginations of the nuclear membrane
(Figure 6e, f, g, h) . Three-dimensional ptychographic tomograms (Figure 6h, l, p ) further
confirmed the progressive perinuclear accumulation of SiNPs over time 47. After 1 h of
incubation (Figure 6e, f, g, h ), nanoparticles were observed near the nuclear periphery and
within the nuclear region (MovieS6, Supporting Information), while after 9 h (Figure 6i, j, k,
l; MovieS7 ) and 18 h (Figures 6m, n, o, p ; MovieS8 ), dense clusters formed around the
nucleus, in agreement with the confocal and cryo -SXT data. These results indicate that
nanoparticle redistribution during successive cell -division cycles is accompanied by
structural remodeling of the perinuclear compart ment, reinforcing the notion of persistent
vesicular entrapment rather than direct nuclear diffusion. Such PXCT analyses underscore
the potential of coherent X -ray imaging to elucidate nanoscale interactions at the bio -nano
interface with unprecedented clarity.
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Figure 6. Time-dependent intracellular distribution of SiNPs revealed by X -ray ptychography.
Schematic representation of the spatial distribution of silica nanoparticles (cyan) around the nucleus
(purple) at each time point : a) Control cell; e) 0.3 mg /mL after 1 h; i) 0.3 mg /mL after 9 h (first
doubling time); m) 0.3 m g/mL after 18 h (second doubling time). Two-dimensional ptychographic
reconstructions of nucleus of RAW 264.7 cells: : b) Control cell; f) 0.3 mg/mL after 1 h; j) 0.3 mg/mL
after 9 h; n) 0.3 mg /mL after 18 h. Magnified views of the boxed regions in two-dimensional
ptychographic reconstructions , highlighting nuclear morphology and nanoparticle localization : c)
Control cell; g) 0.3 mg /mL after 1 h; k) 0.3 m g/mL after 9 h; o) 0.3 mg /mL after 18 h. Three-
dimensional renderings of the tomographic reconstructions : d) Control cell; h) 0.3 mg/mL after 1 h;
l) 0.3 mg/mL after 9 h; p) 0.3 mg/mL after 18 h.
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Materials and methods
Synthesis and purification of fluorescent SiNPs. The nanoparticles were synthesized using
a modified Stöber method 56. One milligram of A TTO633-NHS-ester (λex/em: 630/651 nm)
was dissolved in 800 µL of anhydrous dimethylformamide (DMF). Four hundred µL of this
solution were added to 2 mL of anhydrous ethanol, followed by 9.6 µL of (3-aminopropyl)
triethoxysilane (APTES). The reaction was maintained at room temperature with constant
stirring for 20 hours, resulting in A TTO633-APTES. Then, 7 mL of ammonium hydroxide
solution was added to 120 mL of ethanol and kept under stirring at room temperature. After
30 min, 2.4096 mL of A TTO6 33-APTES and 2.5 mL of tetraethoxysilane (TEOS) were
added. After 3 hours, an additional 2.5 mL aliquot of TEOS was added, and the reaction was
maintained under stirring for 24 hours. The nanoparticles were purified by centrifugation.
The final volume of the synthesis was divided into three Falcon tubes (approximately 40 mL
each) and centrifuged at 10,000 rpm for 15 min at 20 °C. After centrifugation, the supernatant
was discarded, and 30 mL of ethanol was added to each Falcon tube. The nanoparticles were
resuspended using a vortex and sonicated for 30 min. After another ce ntrifugation step, the
supernatant was discarded, and the nanoparticles were resuspended in 40 mL of ultrapure
water. They were then placed in an ultrasonic bath for 30 min. This washing procedure with
water was repeated four times. The final suspension was stored at 8°C, and the concentration
was determined by gravimetry.
Confocal fluorescence microscopy of RA W 264.7. RAW 264.7 macrophages cells were
seeded at a density of 1.0 × 10 5 cells per well in 6 -well plates containing sterile glass
coverslips. Prior to cell seeding, coverslips were sequentially cleaned under agitation in nitric
acid (HNO₃, 15 min), rinsed thoroughly with distilled water, incubated in 1 N NaOH (15
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min), rinsed again with distilled water, and treated with 70% ethanol (30 min). Coverslips
were air-dried on filter paper, transferred to glass containers, and sterilized by autoclaving.
SiNPs were used at concentrations of 0.3, 0.03, and 0.003 mg /mL. Prior to cell exposure,
nanoparticles were incubated for 8 min in DMEM containing 1% BSA. Cells after 24 h were
treated with the nanoparticle suspensions for 1 h at 37 °C. After incubation, cells, including
untreated controls, were washed with PBS and fixed with 250 µL of 4% paraformaldehyde
per coverslip for 10 min at room temperature. Fixation was followed by three washes with
cold PBS (5 min each). This procedure was repeated for experimental time points of 9 h
(calculated DT for BR-cultured cells ) and 18 h following nanoparticle incubation at a
concentration of 0.3 mg /mL. For permeabilization and blocking, coverslips were incubated
with 250 µL of a solution containing Triton X-100 and BSA for 60 min at room temperature,
followed by three additional washes with cold PBS (5 min each). The actin cytoskeleton and
cell nuclei were subsequently labeled with Alexa Fluor 488–conjugated phalloidin and DAPI,
respectively. Fluorescence imaging was performed using an inverted Zeiss LSM confocal
microscope equipped with an Airyscan detector, located at INFABiC (National Institute of
Science and Technology in Applied Photonics to Cell Biology), University of Campinas
(UNICAMP). Images were acquired using a 63× oil immersion objective (NA 1.4 ).
Cryo-SXT and Cryo-SIM of RA W 264.7 at Diamond Light Source. Gold and carbon grids
(Quantifoil AU G200F1 finder) were cleaned with 70% ethanol, rinsed with PBS, and placed
in 6-well plates containing 10% FBS in water for 24 h, with the carbon side facing upward.
RAW 264.7 cells (250,000 cells/well) were seeded onto the carbon side of the grids for 24 h
(37 °C, 5% CO₂). SiNPs at concentrations of 0.3, 0.03, and 0.003 mg/mL were preincubated
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with 1% BSA in DMEM for 8 min. Cells were then treated with the nanoparticles for 1 h and
washed with PBS. Control samples were prepared without nanoparticle treatment .
Accordingly, after 1 h, 16 h (calculated DT for UK-cultured cells), and 32 h, cells were treated
for 30 min with LysoTracker Blue 100 nM (λex/em 373/422 nm) and MitoTracker Green 100
nM ( λex/em 490/516 nm), diluted in DMEM + 10% FBS . The cells were then vitrified
immediately in liquid ethane, without prior washing, and kept in liquid nitrogen until the
analyses were performed. All protocols pertaining to this sample preparation have been
described elsewhere 57. Firstly, the grids were mapped using the Zeiss Axio Imager M2
coupled to a Linkam cryostage. Subsequently, images were collected using the cryo-SIM, at
beamline B24 at the Diamond Synchrotron Light Source (Didcot, UK) to determine the
location of lysosomes and nanoparticles. The samples were kept on a cryo-stage (CMS196M,
Linkam Scientific), and a 100x magnification objective, numerical aperture 0.9, and 2 mm
working distance were used (Nikon). Subsequently, analyses by cryo -SXT of these same
regions were performed on an UltraXRM-S220C microscope (Carl Zeiss X-ray Microscopy
Inc.), also on beamline B24 at the Diamond Synchrotron Light Source (Didcot, UK). This
analysis was performed in the energy range known as the water window (284 eV - 543 eV)
at 520 eV. A depth of focus of 1 µm was selected, achieving a resolution of 25 nm. The
reconstructed tomograms were segmented using Avizo software (Thermo Fisher Scientific).
This software was employed for surface rendering and three-dimensional visualization of the
intracellular distribution of nanoparticles. Segmentation was performed manually based on
the reconstructed tomograms.
Cryo-SXT of RA W 264.7 at Alba Synchrotron. Gold–carbon grids were cleaned by glow
discharge and exposed to UV radiation for 30 min. Subsequently, the grids were placed
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carbon-side up in 60 mm culture dishes containing FBS diluted in water and incubated for 1
h. RAW 264.7 cells (300,000 cells per well) were seeded onto the carbon side of the grids
and cultured for 24 h at 37 °C under 5% CO₂. SiNPs at a concentration of 0.3 mg/mL were
pre-incubated with 1% BSA in DMEM for 8 min. Cells were then treated with the
nanoparticles for 1 h and washed with PBS. Control samples were prepared under the same
conditions without nanoparticle treatment. The DT of RAW 264.7 cells cultured in Barcelona
was previously determined to be 15 h. Based on this value, samples were collected after 1 h,
15 h, and 30 h, in addition to untreated controls. At each time point, samples were washed
with PBS to remove excess medium and ensure optimal X-ray transmission. For tomographic
alignment, 1 µL of a 100 nm gold nanoparticle suspension (3.60 × 108 particles/mL,
EMGC100, BBI Group, Cardiff, UK) was added onto the grids. The grids were rapidly
vitrified by plunge freezing in liquid ethane using a Leica EMCPC system. Frozen grids were
imaged and selected using a LINKAM CMS196 stage mounted on a Zeiss Axio Scope
fluorescence microscope. The vitrified grids were subsequently stored in liquid nitrogen until
imaging. Cryo-SXT was performed at the Mistral beamline of the ALBA Synchrotron using
an UltraXRM-S220C microscope (Carl Zeiss X-ray Microscopy Inc.)58,59. Tomographic data
were collected at 520 eV , with exposure times of 1 –2 s per projection. Projection images
acquired at different sample orientations were computationally combined to generate three -
dimensional (3D) reconstructions of whole-cell subcellular ultrastructure 60. A tilt series was
acquired for each cell area using an angular step of 1° over a ±70° range, employing a Fresnel
zone plate (FZP) with a 40 nm outermost zone width and an effective pixel size of 13 nm.
Each transmission projection image of the tilt series was normalized using flat -field images,
accounting for exposure time and storage ring current. Wiener deconvolution, considering
the experimental impulse response of the optical system, was applied to the normalized data
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to enhance image quality 61. The Napierian logarithm was then used to reconstruct the linear
absorption coefficient (LAC). The resulting image stacks were loaded into IMOD software62,
and individual projections were aligned to a common tilt axis using the 100 nm gold
nanoparticles as fiducial markers. Aligned stacks were subsequently reconstructed using
algebraic reconstruction techniques (ART) 63. Tomographic reconstructions were segmented
manually using Avizo software (Thermo Fisher Scientific) based on the reconstructed
tomograms.
2D Ptychography and PXCT. RAW 264.7 cells were cultured in DMEM supplemented with
10% FBS at 37 °C in a 5% CO₂ atmosphere. Cells were seeded at a density of 10,000 cells
per well in 6-well plates onto 100 nm-thick silicon nitride membranes, previously sterilized.
After 24hrs they were then incubated with SiNPs coated with 1% BSA at a concentration of
0.3 mg/mL for 1 h. After this internalization period, cells were washed with PBS and
maintained in DMEM . Untreated cells were used as controls. After 9 h and 18 h , the cells
were washed with PBS and treated with 1% Triton for 3 min to lyse the plasma membrane
while preserving intact nuclei. Cells were subsequently fixed with 2.5% glutar aldehyde in
0.1 M cacodylate buffer for 24 h, washed with 0.1 M cacodylate buffer and progressively
dehydrated in a graded ethanol series (15%, 30%, 50%, 80%, 90%, 100%) , followed by
critical point drying with CO₂. Samples were first screened under an optical microscope to
identify the most suitable regions for three-dimensional imaging, which was performed at the
Cateretê beamline of the LNLS (Brazilian Synchrotron Light Laboratory). The area to be
imaged was selected using the Arinax on-axis optical microscope. The 2D ptychographic and
PXCT were carried out at the energy of 6 keV . The sample was illuminated by a beam defined
by a set of central stop (CS), Fresnel Zone Plate (FZP) (50 um diameter and outermost zone
width of 50 nm) and an order sorting aperture (OSA). The sample was placed 2.4 mm from
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25
the FZP focus, resulting in a beam size of 10 um, which scanned the sample with steps of
1.75 µm. The acquisition of each scanning point was 25 ms. The s cattered X-rays were
detected the in vacuum PiMega 540d detector (PiTec- LNLS, 55 um pixel size) positioned 7
m downstream from the sample. Bidimensional projections and tomographic reconstructions
were performed using the PtychoShelves package 64. Each projection was reconstructed into
two-dimensional (2D) images using 500 iterations of the difference map (DM) algorithm.
Subsequently, the set of 2D reconstruction were assembled to reconstruct the tomographic
image, using Filter Back Projection (FBP) algorithm. Tomographic reconstructions were
segmented using Avizo software (Thermo Fisher Scientific).
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26
ACKNOWLEDGMENTS
The authors gratefully acknowledge the financial support provided by the Fundação de
Amparo à Pesquisa do Estado de São Paulo (FAPESP – Processes 2021/12071 -6,
2023/00103-6, 2024/00989-7). The authors also thank the Electron Microscopy Laboratory
of LNNano for access to the electron microscopy facilities (Proposal SEM -20233386),
LNBio for access to the flow cytometer (Proposal 20231954) . We thank the access to
equipment and assistance provided by the National Institute of Science and Technology on
Photonics Applied to Cell Biology (INFABIC) at the State University of Campinas;
INFABIC is co -funded by Fundação de Amparo a Pesquisa do Estado de São Paulo
(FAPESP) (2014/50938 -8) and Conselho Nacional de Desenvolvimento Cientifico e
Tecnológico (CNPq) (465699/2014 -6) for the ac cess to the confocal fluorescence
microscopy, LNLS for access to ptychography at the Caterete beamline (20250854 and
20250988), Diamond Light Source for access to cryo-SIM and cryo-SXT at the B24 beamline
(BI34928), and Alba Synchrotron for access to cryo -SXT at the Mistral beamline
(2024078502). The authors further acknowledge iNext (PID 24410 and VID 43520) for
financial support during the experiments performed at Diamond Light Source. Special thanks
are due to Vitor B. Pelgati for his assistance with confocal fluorescence microscopy, to Jessica
do N. Faria for support with sample preparation for cryo -SXT experiments at the ALBA
Synchrotron and to Archana Jadhav and Kamal L. Nahas for experimental support at
Diamond Light Source. The authors also appreciate the contributions of Tiago A. Kalile and
Pedro H. Z. Guidolim to the ptychography experiments.
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27
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