Main

As a lentivirus, HIV-1 infects non-dividing immune cells, including resting CD4+ T cells, dendritic cells and macrophages1,2,3,4,5,6,7. Upon entering the cell, the HIV-1 capsid—which encapsulates its genetic material and viral enzymes, collectively termed the HIV-1 core—traverses the cytoplasm and enters into the nucleus, where integration of reverse-transcribed viral DNA occurs8. During this stage of the viral life cycle, the HIV-1 capsid is a key orchestrator, mediating multiple steps by interacting with various host factors to facilitate reverse transcription, cytoplasmic trafficking, nuclear import and post-import trafficking to chromosomes9,10. Traversing through nuclear pore complexes (NPCs) is critical for HIV-1 infection of non-dividing cells.

The HIV-1 capsid, composed of approximately 200–250 capsid protein (CA) hexamers and 12 CA pentamers, predominantly forms a conical shape with a wide-end diameter of 60 nm and a length of 120 nm (refs. 11,12,13,14), a size that substantially exceeds the ~45 nm inner diameter of the NPC as resolved from isolated nuclear envelopes15. However, recent studies suggest that HIV-1 nuclear import occurs with a nearly intact capsid lattice, with uncoating occurring in the nucleus, near sites of integration16,17,18,19,20,21,22. Supporting this idea, NPCs ‘dilate’ within cells compared with previously isolated forms23,24,25,26,27,28 and ‘crack’ to accommodate the passage of HIV-1 cores29.

HIV-1 nuclear import is mediated by complex interactions between the capsid and components of the NPC, particularly phenylalanine-glycine (FG)-nucleoporins (Nups), such as Nup358 and Nup153 (refs. 30,31,32,33,34,35,36,37,38,39,40). Recent studies show that capsid-like particles constructed from recombinant CA can penetrate in vitro-reconstituted condensates of FG-Nups, which mimic the selective barrier of the NPC’s central channel39,40. However, the native NPC presents a more complex environment, with overlapping capsid binding sites and diverse Nup oligomerization states25,28,34,35,37,39,41. Moreover, the pleomorphic nature of HIV-1 cores further complicates how shape, size and elasticity dictates its traversal through the NPC. Beyond Nups, nuclear factors, including cleavage and polyadenylation specificity factor subunit 6 (CPSF6), have been shown to facilitate HIV-1 nuclear import and intranuclear trafficking18,42,43,44,45,46,47. However, the fate of the HIV-1 cores following nuclear entry remains poorly understood.

Despite previous efforts to characterize HIV-1 nuclear import both in cells and in vitro16,21,29,39,40,46,48,49, the scarcity of this critical process has prevented a mechanistic understanding of the complex interplay between the core and NPC. To overcome this, we reconstituted a functional HIV-1 nuclear import system using permeabilized CD4+ T cells and isolated native HIV-1 cores, substantially increasing the nuclear import event. Combining targeted cryo-focused ion beam (cryo-FIB) milling with integrated cryo-correlative light and electron microscopy (cryo-CLEM) and cryo-electron tomography (cryo-ET), we effectively characterized capsid–NPC interactions and capsid integrity during nuclear import in a close-to-native environment. Analysis of nearly 1,500 cores revealed that successful nuclear import requires both the structural elasticity of the HIV-1 core and the expansion of NPCs, some of which undergo deformation. Intriguingly, nuclear pores function as selective filters, favouring the import of smaller tube-shaped and conical cores. Moreover, high-resolution tomograms reveal that brittle cores fail to enter the NPC, while CPSF6-binding-deficient cores successfully enter but stall within the NPC. Upon traversing the NPC, HIV-1 cores were found to be coated with nuclear factors, probably including CPSF6, to facilitate downstream nuclear trafficking. Collectively, our work establishes an innovative approach to dissect the HIV-1 nuclear import mechanism and downstream nuclear events.

Results

Permeabilized T cells markedly amplify HIV-1 nuclear import

Nuclear import events during HIV-1 infection are rare and transient16,21,46,50,51,52,53, making them extremely difficult to capture. To overcome this limitation, we developed a system to recapitulate functional nuclear import in situ using permeabilized CEM cells (an immortalized CD4+ T cell line) and isolated native HIV-1 cores (Extended Data Fig. 1a). Specifically, we used digitonin permeabilization of CEM cells, which selectively permeabilizes the plasma membrane while leaving the nuclear membrane intact54. Upon optimization, we determined that 0.018% digitonin provided optimal permeabilization while maintaining nuclear integrity, as confirmed by the exclusion of high-molecular-weight fluorescein isothiocyanate (FITC)-labelled dextran (500 kDa), a marker for nuclear envelope integrity (Extended Data Fig. 1b)55.

HIV-1 cores were purified from near-full-length genome-containing virions (Env-defective variants of the clade B strain R9)56 containing mNeonGreen-labelled integrase (mNeonGreen-IN) by sucrose gradient centrifugation following spin-through delipidation57 (Extended Data Fig. 1a). HIV-1 cores migrated as a distinct green-fluorescence band, confirmed by cryo-EM imaging (Extended Data Fig. 1c,d). We found that purified wild-type (WT) cores showed cone-shaped and tube-shaped structures in a ratio of approximately 5:1, similar to the proportion observed in virions (Extended Data Fig. 1e). Average sizes of both isolated cone-shaped and tube-shaped cores were indistinguishable to the cores observed within virions (Extended Data Fig. 1f,g), consistent with previous studies12,13,14.

Intriguingly, when isolated mNeonGreen-IN-labelled WT cores were mixed with permeabilized CEM cells, numerous cores were efficiently recruited to and accumulated around the nuclear envelope (Fig. 1a, left). Notably, about 1% of the green puncta were detected inside the nucleus (Fig. 1a,b). Given that cell permeabilization reduces cytosolic components and energy54, and that energy depletion has been shown to constrict NPCs24, we compared NPC sizes in permeabilized and intact CEM cells. The average diameter of NPCs in intact cells, 93.8 nm, was significantly larger than the 86.9-nm diameter in permeabilized cells (Extended Data Fig. 2). We thus supplemented permeabilized CEM cells with exogenous cytosol (rabbit reticulocyte lysate (RRL)) and an ATP-regenerating system (RRL-ATP), which are commonly used in nuclear import assays58,59, including those for other viruses60,61,62. Addition of RRL-ATP to the permeabilized CEM cells restored NPC size to 93.4 nm, closely matching that of native NPCs (Extended Data Fig. 2c). More importantly, a greater number of mNeonGreen-IN puncta were detected inside the nucleus using this near-native nuclear import system (Fig. 1a,b). Kinetic analysis showed that nuclear import reached steady state by 1 h (Fig. 1b). To capture and characterize intermediate stages of nuclear import, we selected the 30-min time point for further correlative and integrated in situ cryo-ET studies.

Fig. 1: Nuclear import of HIV-1 WT cores.
figure 1

a, Confocal microscopy images of permeabilized CEM cells incubated with WT cores in the absence (P-CEM) and presence (PS-CEM) of RRL-ATP. WT cores are labelled with mNeonGreen-IN (green) and nuclei are labelled with SiR-DNA (magenta). Representative single z-slice images (top) and maximum intensity projections (MIPs) of z slices (bottom) are shown. The arrows indicate mNeonGreen-IN signals inside the nucleus. Scale bar, 5 µm. b, Statistical analysis of the nuclear import of the mNeonGreen-IN puncta. The ratios represent the percentage of mNeonGreen-IN puncta localized inside the nuclei of permeabilized CEM cells under different conditions. Without RRL-ATP, 0.9% ± 1.2% (n = 61) for WT cores. With RRL-ATP for WT cores with an incubation time of 30 min, 6.2% ± 3.3% (n = 168); 1 h, 10.4% ± 3.7% (n = 117); 2 h, 11.5% ± 4.7% (n = 116); and 4 h, 10.8% ± 4.5% (n = 98). The black lines represent medians. Significance was determined using a one-way ANOVA test for all and two-sided Fisher’s exact test for each pair; ****P < 0.0001 (only significant differences are shown). c, A representative tomographic slice of a correlatively acquired tomogram of WT core nuclear import. Three WT cores are identified and indicated by the numbered purple arrowheads. Number 1 highlights an imported tube-shaped core with discernible surrounding densities (enlarged in the inset); number 2 shows a docked cone-shaped core with the wide end on the NPC; and number 3 shows a cone-shaped core traversing through the NPC with the narrow end facing inwards. The NPC, ribosomes, nucleosomes and prominent surrounding nuclear factors are labelled. The nucleus, nuclear envelope (NE) and membranes are annotated accordingly. Scale bar, 100 nm. d, The segmented volume of c, shown as an overview (left) and zoomed-in views of the imported, docked (top right; numbers 1 and 2) and traversing (bottom right; number 3) WT cores. WT cores, NPCs, nucleosomes, ribosomes, nuclear factors, NE and membranes are segmented and shown in the indicated colours. e, A bar chart illustrating the distribution of HIV-1 cores in each state of two groups: WT cores incubated with P-CEM cells (WT + P-CEM) and WT cores incubated with PS-CEM cells (WT + PS-CEM). Imported fractions are indicated. Significance was determined using a two-sided Chi-square test for all; P = 0.0464. f, A violin plot of the statistical analysis on the width of WT cores (width measured at the wide end) in each state. The imported WT cores measure 44.84 ± 6.519 nm (s.e. = 0.7429, n = 77), the traversing cores measure 52.97 ± 6.875 nm (s.e. = 0.6199, n = 123), the docking cores measure 54.53 ± 7.350 nm (s.e. = 0.4989, n = 217), the approaching cores measure 53.55 ± 7.432 nm (s.e. = 0.4540, n = 268) and the input cores measure 54.93 ± 7.442 nm (s.e. = 0.6578, n = 128). The white lines represent the medians, black lines represent the quartiles and black dots represent individual WT cores. Significance was determined using two-sided Brown–Forsythe and Welch ANOVA tests for all; ****P < 0.0001 (only significant differences are shown). g, A bar chart illustrating the composition of WT core shapes in each state. Cone-shaped WT cores are shown in purple and tube-shaped cores are in blue. Significance was determined using a two-sided Chi-square test for all; P < 0.0001. h, A bar chart showing the orientation distribution of cone-shaped WT cores in docking and traversing states, with the wide end in first (grey) and narrow end in first (purple). Significance was determined using a two-sided Fisher’s exact test for 1 comparison; P < 0.0001.

Three-dimensional correlative cryo-ET imaging of HIV-1 core nuclear import

A major challenge in detecting HIV-1 nuclear entry events for structural characterization using cryo-ET is how to precisely locate HIV-1 cores (50–100 nm) in a much larger cell nucleus (10 µm). To address this, we established an integrated correlative workflow using cryo-fluorescence microscopy, targeted cryo-FIB lamella preparation and subsequent cryo-ET imaging guided by the fluorescence signals on lamellae (cryo-CLEM) (Extended Data Fig. 3). We further adopted an automated cryo-FIB milling approach and produced thin (100–150 nm), narrow (5–10 µm) lamellae (Extended Data Fig. 3a). Cryo-FIB milling was guided by core-associated mNeonGreen-IN fluorescence and SiR-DNA fluorescence marking the nucleus, to specifically target cores associated with the nuclear envelope (Extended Data Fig. 3b). The final thin lamellae retained discernible mNeonGreen-IN fluorescence signal, facilitating targeted cryo-ET data collection (Extended Data Fig. 3c,d). A representative tomogram acquired from such a correlated position on a lamella readily enumerated nuclear envelopes, NPCs, abundant ribosomes and nucleosomes (Fig. 1c,d and Supplementary Video 1). Notably, three WT cores were observed in the tomogram: two successive cores interacting with one NPC; one tube-shaped core exiting the NPC, immediately followed by a cone-shaped core docking to the same NPC; and a third cone-shaped core traversing a separate NPC with its narrow end pointing toward the nucleus (Fig. 1c,d and Supplementary Video 1).

Using this integrated cryo-CLEM approach, we improved the success rate of capturing nuclear-associated HIV-1 cores from 1–3% (refs. 21,29) to 52%. We obtained 759 tomograms and captured 685 WT cores associated with the T cell nucleus, either in the vicinity or inside of an NPC or translocated into the nucleoplasm (Extended Data Fig. 4a), enabling detailed analyses with statistical confidence. Nuclear-associated WT cores were distributed across 4 distinct stages of nuclear import, which we define as approaching (39.1%), docking (31.7%), traversing the NPCs (18.0%) and imported into the nucleus (11.2%) (Fig. 1e), suggesting that traversing through the NPC is a rate-limiting step, consistent with previous studies46,52. Overall data statistics, experimental parameters for cryo-FIB lamella preparation, cryo-ET data collection and subtomogram averaging (STA) are described in Supplementary Tables 113.

Smaller HIV-1 cores enter the nucleus and recruit nuclear factors

Statistical analysis of cores at the four distinct import stages revealed that smaller cores were selectively imported into the nucleus (Fig. 1f). When cone-shaped and tube-shaped cores were considered separately, 66.2% of imported WT cores showed a tubular morphology compared with 18.0% in the input population (Fig. 1g). In contrast, the ratio of cone- and tube-shaped cores among the earlier stages of nuclear import remained consistent with the input ratio. Notably, tube-shaped cores showed little size variation across the four stages, whereas a significant reduction in size was observed in the imported cone-shaped cores (Extended Data Fig. 4b,c). Whereas both the wide and narrow ends of cone-shaped cores docked equally at the NPC, traversing cores almost exclusively entered the NPC through their narrow end first (Fig. 1h), in line with previous observations63.

Among the 685 captured WT cores, 77 were located inside the nucleus. Remarkably, nearly all these nuclear cores showed discernible extra densities surrounding the capsid (Fig. 1c,d, Extended Data Figs. 4a and 5a, and Supplementary Videos 1 and 2), a feature not readily observed in cores at the approaching and docking stages of nuclear import (Extended Data Fig. 4a). This observation indicated an association between the capsid and nuclear factors. Although most imported cores showed intact capsid hexagonal lattices, we detected several cores that appeared to show signs of capsid uncoating and viral RNA/DNA release (Extended Data Fig. 5b–d and Supplementary Videos 36). The mechanism of uncoating and its molecular triggers require further investigation.

To further investigate the roles of nuclear host factors in HIV-1 core import and trafficking, we performed STA64,65 of WT cores at three distinct stages: cytoplasmic (outside), traversing and imported. The CA hexamer structures were resolved at 11 Å, 12 Å and 16 Å for outside, traversing and imported WT cores, respectively (Fig. 2a and Extended Data Fig. 6a,b), all of which aligned well with the CA hexamer model (PDB 6SKK) derived from our previous CA tubular assemblies (Fig. 2a)66. Notably, the extent of core-associated extra densities attributable to host cell factors increased as the cores progressed inwards: outside cores contained the least amount of extra density, followed by traversing cores and then imported cores. Imported cores showed substantial extra densities on the CA hexamer surface. This additional density, located ~63 Å above the imported WT core surface, coincided with CPSF6 density resolved in a cryo-EM map of the capsid–CPSF6 complex obtained using recombinant CPSF6 protein and perforated virus particles (Extended Data Fig. 4d,e).

Fig. 2: STA of HIV-1 WT CA hexamers and NPCs during nuclear import.
figure 2

a, Structures of CA hexamers in capsid lattices of outside (approaching and docking cores combined), traversing and imported WT cores. Maps are aligned and contoured to the same level. The first column shows top views of coloured CA hexamer density maps (contoured at 3σ); the second column shows top views of CA hexamer density maps (contoured at 3σ) fitted with a CA hexamer model (PDB 6SKK); the third column shows the CA hexamer density maps (contoured at 0.5σ), coloured according to height, from white (bottom) to purple (top); and the fourth column shows the side views of CA hexamer density maps (major body density contoured at 3σ, floating top density contoured at 0.5σ), the distance between CA hexamer and the floating top density measures approximately 63 Å for the imported WT core. b, Structures of NPC ring moieties. The first four columns starting from the left show the structures of NPC CR, IR, LR and NR, respectively. The composite EM map is depicted in the fifth column. The top row depicts the central slice of EM maps in the xz plane; NPC densities and NE are annotated. The middle and bottom rows show two orthogonal views of EM maps. CR and IR are contoured at 3σ, LR is contoured at 1σ, NR is contoured at 1.5σ and the composite map is contoured at 2σ. Scale bars, 10 nm. c, Composite EM map of the whole CEM NPC with eight subunits. Two orthogonal views of the NPC are depicted.

We further analysed the structures of NPC subunits by STA, resulting in the following NPC ring moiety structures: the cytoplasmic ring (CR), inner ring (IR), luminal ring (LR) and nuclear ring (NR), at resolutions of 21.9 Å, 28.8 Å, 32.1 Å and 36.5 Å, respectively (Fig. 2b and Extended Data Fig. 6c,d). The overall symmetrized NPC structure from the composite EM map (Fig. 2b,c) resembled the ones from previous in-cell work21,29, validating the native state of the NPCs analysed here.

HIV-1 core traversal induces NPC expansion and deformation

When comparing empty and core-occupied NPCs, we observed a small but significant NPC expansion (93.4 nm to 95.2 nm) upon core traversal (Fig. 3a). Further analysis showed that this apparent NPC expansion was anisotropic, meaning that the structural changes were unevenly distributed, which was not due to the missing-wedge effect (Fig. 3b and Supplementary Video 7). In many cases, one to three subunits deviated from rotational symmetry, contributing to NPC deformation.

Fig. 3: Remodelling of NPCs during HIV-1 core import.
figure 3

a, A violin plot of the size distribution of PS-CEM NPCs with WT cores (purple; 95.22 ± 4.362 nm, s.e. = 0.5453, n = 64) and without cores (pink; 93.39 ± 4.315 nm, s.e. = 0.3756, n = 132). White lines represent the medians, black lines represent the quartiles and dots represent individual NPCs. Significance was determined using a two-sided t-test for one comparison; **P = 0.0062. b, Examples of occupied NPCs in which the eight subunits are well identified with high cross-correlation and correct orientation by template matching. Top: the six tomographic slices ((i)–(vi)) of WT cores traversing through the NPC. Middle: symmetry analysis by rotation based on the refined coordinates of each subunit. Bottom: mapped-back model of each NPC occupied by WT cores, using an adapted EM map EMD-51631 for better illustration. The WT cores and NPCs are labelled (indicated by white circles in the top view in some cases). The nucleus, NE and membranes are annotated accordingly. Scale bars, 50 nm. ce, Violin plots of the included angles between adjacent subunits in PS-CEM NPCs (n = 43) occupied by WT cores (c), empty PS-CEM NPCs (n = 95) (d) and in-cell empty CEM NPCs (n = 42) (e). Bottom right inset (c): the measurement of the included angles. The thresholds (red dashed lines) are set at 47.5° (top) and 42.5° (bottom), deviating from the 8-fold symmetry reference angle of 45° (green dashed lines). The black violin units indicate deformed NPCs, white violin units indicate regular NPCs and dots represent included angles measured in individual NPCs. Top inset (c): deformed NPCs are grouped to the left side (purple background) of the charts for ease of comparison. For empty PS-CEM NPCs, purple violin units indicate NPCs associated with WT cores (docking and just-imported cores). f, A bar chart depicting the distribution of NPCs in the aforementioned three conditions. Significance was determined using a two-sided Fisher’s exact test for each pair; for occupied versus empty, P = 0.0050; for occupied versus in-cell empty, P = 0.0024; and for empty versus in-cell empty, P = 0.4983 (not significant (NS)). g, A bar chart depicting the distribution of core-associated NPCs in regular and deformed empty NPCs. Significance was determined using a two-sided Fisher’s exact test for 1 comparison; P = 0.4570. h, A violin plot of the statistical analysis on the size of WT cores (width measured at the wide end) in regular and deformed occupied NPCs. The size of WT cores in regular occupied NPCs measures 55.32 ± 4.854 nm (s.e. = 1.035, n = 22), and the size of WT cores in deformed occupied NPCs measures 55.05 ± 6.960 nm (s.e. = 1.519, n = 21). The white and black lines represent the medians, purple lines represent the quartiles and dots represent individual WT cores. Significance was determined by two-sided t-test for one comparison; NS. i, A violin plot of the statistical analysis on the size of NPCs occupied by WT cores. The regular NPCs measure 95.74 ± 1.684 nm (s.e. = 0.3591, n = 22) and the deformed NPCs measure 95.95 ± 4.841 nm (s.e. = 1.056, n = 21). The white and black lines represent the medians, purple lines represent the quartiles and dots represent individual occupied NPCs. Significance was determined by two-sided t-test for one comparison; NS. ONM–INM, outer nuclear membrane–inner nuclear membrane.

To what extent might HIV-1 core-induced expansion lead to NPC structural deformation, or even cracking, as recently reported29? To address this question, we analysed the architecture of NPCs in the following 3 states: WT core-occupied NPCs (n = 43), empty NPCs (n = 95) and NPCs from uninfected intact CEM cells (n = 42) (Fig. 3c–e). Given the eight-fold symmetry of the NPC, we performed symmetry analysis to assess whether NPCs undergo deformation during WT core traversal. Specifically, we used template matching64,65 to identify individual NPC subunits, with an NPC selection cut-off of more than three matched subunits (Extended Data Fig. 6c). The angles between adjacent template-matched and refined subunits were measured for each NPC, with deviations exceeding 2.5° classified as deformed (Fig. 3c–e). Our analysis showed that 50% of WT core-occupied NPCs were deformed, compared with 23% of empty NPCs and 16.6% of NPCs in native CEM cells (Fig. 3f), suggesting that the presence of cores inside NPCs promotes their deformation. Among empty NPCs (Fig. 3d), NPC deformation occurred more frequently when HIV-1 cores were docked at the cytoplasmic side compared with core-free NPCs (Fig. 3g). Interestingly, NPC deformation did not correlate with HIV-1 core size (Fig. 3h) nor NPC expansion (Fig. 3i).

CPSF6-binding-deficient cores stall within the NPC

CPSF6 is thought to compete with Nup153 at the nuclear basket to release the HIV-1 core from the NPC35,38. Increasing evidence suggests that CPSF6 forms condensates that co-localize with the capsid in the nucleus44,67,68, facilitating core nuclear trafficking and integration into transcriptionally active speckle-associated domains16,18,35,36,37,38,43,44,45,47,68. We found that imported WT cores were surrounded by extra densities consistent with recombinant CPSF6 binding to mature capsid lattices (Extended Data Fig. 4d,e). To assess how CPSF6 interactions affect HIV-1 nuclear import, we characterized HIV-1 cores derived from the N74D mutant, which is deficient for CPSF6 binding69. Confocal fluorescence microscopy revealed a reduced nuclear import efficiency for N74D cores compared with WT cores (Fig. 4a,b), consistent with a previous immunofluorescence microscopy study of N74D-infected cells18. Moreover, the penetration depth of N74D cores was compromised compared with that of WT cores (Fig. 4c), in agreement with previous fluorescence imaging studies following HIV-1 infection16,45,46.

Fig. 4: Nuclear import of N74D cores.
figure 4

a, Confocal microscopy images of permeabilized CEM cells incubated with N74D cores in the presence of RRL-ATP. N74D cores are labelled with mNeonGreen-IN (green) and nuclei are labelled with SiR-DNA (magenta). Representative single z-slice images (top) and MIPs of z slices (bottom) are shown. Arrows indicate mNeonGreen-IN signals inside the nucleus. Scale bar, 5 µm. b, The nuclear import efficiency of mNeonGreen-IN puncta was analysed for WT and N74D cores. The percentage of mNeonGreen-IN puncta localized inside the nuclei of permeabilized CEM cells under different incubation times was as follows: WT 30 min, 6.2% ± 3.3% (n = 168); WT 1 h, 10.4% ± 3.7% (n = 117); WT 2 h, 11.5% ± 4.7% (n = 116); WT 4 h, 10.8% ± 4.5% (n = 98); N74D 30 min, 4.3% ± 2.2% (n = 97); N74D 1 h, 6.8% ± 3.4% (n = 72); N74D 2 h, 7.4% ± 3.1% (n = 80); and N74D 4 h, 7.4% ± 3.2% (n = 66). The black lines represent medians. Significance was determined using a one-way ANOVA test for all and two-sided Fisher’s exact test for each pair; ****P < 0.0001, ***P = 0.001 for WT 0.5 h versus N74D 0.5 h, ***P = 0.0004 for N74D 0.5 h versus N74D 1 h. c, The penetration depth of WT and N74D cores from the nuclear envelope were enumerated as follows: WT 30 min, 0.38 ± 0.31 µm (n = 3,010); WT 1 h, 0.50 ± 0.48 µm (n = 8,540); WT 2 h, 0.56 ± 0.53 µm (n = 8,713); WT 4 h, 0.57 ± 0.53 µm (n = 7,548); N74D 30 min, 0.29 ± 0.21 µm (n = 1,311); N74D 1 h, 0.35 ± 0.30 µm (n = 2,257); N74D 2 h, 0.39 ± 0.32 µm (n = 2,872); and N74D 4 h, 0.39 ± 0.33 µm (n = 2,413). The black lines represent medians. Significance was determined using a one-way ANOVA test for all and two-sided Fisher’s exact test for each pair; ****P < 0.0001 and ***P = 0.0009. d, A representative tomographic slice of a correlatively acquired tomogram of HIV-1 N74D core nuclear import. One just-imported cone-shaped N74D core with the wide end facing inwards is identified and indicated by the light blue arrowhead. No discernible surrounding densities are observed (enlarged in the inset). The NPC, ribosomes and nucleosomes are labelled. The nucleus, NE and membranes are annotated accordingly. Scale bar, 100 nm. e, The segmented volume of d, shown as an overview (left) and zoomed-in views of the just-imported N74D core from the top (top right) and side (bottom right). The N74D core, NPCs, nucleosomes, ribosomes, NE and membranes are segmented and shown in the indicated colours. f, A bar chart showing the distribution of N74D cores in each state; the import fraction is annotated above the imported bar. g, Right: a line chart depicting the change of density as a function of the distance from the surface of HIV-1 cores. The first solid arrow approximately indicates the surface of the core, and the second solid arrow approximately indicates the centre of the surrounding density. Left: the measurement of grey values along the normal lines (dashed arrows) extending from the core surface, including partial densities of CA (~3 nm) due to the resolution of images. Black density is assigned a value of zero, while white is assigned one. Higher density corresponds to lower numerical values. For all conditions, 20 lines are drawn for each core. The numbers of HIV-1 cores analysed are as follows: WT outside, n = 10; WT traversing, n = 10; WT imported, n = 10; E45A imported, n = 10; E45A/R132T imported, n = 10; and N74D imported, n = 5. h, A line chart illustrating the distribution of all HIV-1 cores in each state (in percent). Significance was determined using a two-sided Chi-square test for all; P < 0.0001. i, A bar chart depicting the distribution of all imported HIV-1 cores based on their distances from the nuclear envelope within the nucleus. The reference distance is calculated as the sum of the longest axis of the HIV-1 core (~120 nm) and the length of the nuclear basket (~80 nm). Significance was determined using a two-sided Fisher’s exact test for all; P = 0.8641.

Correlative cryo-ET analyses showed that N74D cores more frequently stalled within the NPC (36%) compared with WT cores (18%), translating to a much-decreased import fraction (6.8%) (Fig. 4d–f,h, Extended Data Fig. 7 and Supplementary Video 8). These observations were consistent with a deficiency in core release from the NPC. Furthermore, imported N74D cores appeared comparatively ‘clean’ with little extra surrounding densities (Fig. 4d,e, Extended Data Fig. 7a and Supplementary Video 8) relative to WT cores. Due to the limited availability of imported N74D cores for STA, we used density profile analysis to illustrate the change in density as a function of distance from the surface of HIV-1 cores (Fig. 4g). Unlike imported WT cores, which showed a drop in grey value starting around 6.5 nm from the capsid surface, N74D cores lacked this characteristic and showed a density profile similar to WT cores before nuclear entry (Fig. 4g). Moreover, 80% of imported N74D cores were located comparatively close to the nuclear envelope (<200 nm), whereas more than 40% of WT cores penetrated further into the nucleus, consistent with our fluorescence data and previous studies45,46 (Fig. 4i). Together, these results provide evidence that CPSF6 is, at least in part, a component of the nuclear factors bound to imported HIV-1cores, and that CPSF6 binding is important for releasing HIV-1 cores from NPCs and subsequent nuclear trafficking.

Capsid elasticity is essential for entering the NPC

Previous studies suggested that HIV-1 core elasticity is essential for nuclear import, and that the capsid undergoes remodelling for efficient transport through the NPC56,70,71. Brittle cores, such as those derived from the hyperstable E45A mutant, show impaired nuclear import, yet the nature of the interaction between these cores and the NPC remains unclear. To investigate the effect of HIV-1 core elasticity in nuclear import, we examined the nuclear import of E45A cores and its second-site revertant mutant E45A/R132T56,72,73. In infection assays, the R132T change stimulated basal E45A infection >10-fold, with E45A/R132T achieving ~30% of the level of WT virus infection73. In addition, whereas E45A is markedly impaired for infection of non-dividing cells, both WT and E45A/R132T are competent, reflecting their ability to enter the nucleus through NPCs. Confocal fluorescence microscopy showed that the E45A mutation significantly decreased the number of nuclear green puncta, with an import ratio of 1.3% compared with 6.1% for WT cores (Fig. 5a,b). As expected, E45A/R132T cores showed an intermediate phenotype, with 3.5% nuclear import capacity (Fig. 5a,b). The behaviours of E45A and E45A/R132T mutant cores further support the utility of our in situ HIV-1 nuclear import system for studying biologically relevant nuclear entry events.

Fig. 5: Nuclear import of E45A and E45A/R132T cores.
figure 5

a, Confocal microscopy images of permeabilized CEM cells incubated with E45A and E45A/R132T cores in the presence of RRL-ATP. Cores are labelled with mNeonGreen-IN (green) and nuclei are labelled with SiR-DNA (magenta). Representative single z-slice images (top) and MIPs of z slices (bottom) are shown. The arrows indicate mNeonGreen-IN signals inside the nucleus. Scale bar, 5 µm. b, Statistical analysis of the nuclear import of the mNeonGreen-IN puncta for brittle E45A revertant mutant E45A/R132T cores. The ratios represent the percentage of mNeonGreen-IN puncta localized inside the nuclei of permeabilized CEM cells under different conditions. WT cores, 6.2% ± 3.3% (n = 168); E45A cores, 1.3% ± 1.2% (n = 99); and E45A/R132T cores, 3.5% ± 2.4% (n = 111). The black lines represent medians. Significance was determined using a one-way ANOVA test for all; ****P < 0.0001. c, A representative tomographic slice of a correlatively acquired tomogram of E45A cores clashing on the NPC. Five E45A cores were identified and indicated by pink arrowheads and numbered as follows: numbers 1, 3 and 4 show clashing cone-shaped E45A cores; number 2 shows a clashing tube-shaped E45A core; and number 5 shows a docked cone-shaped E45A core with the narrow end on the NPC. The E45A cores labelled number 4 and number 5 are shown on other slices of the same tomogram (white framed). The NPC, ribosomes and nucleosomes are labelled. The nucleus, NE and membranes are annotated accordingly. Scale bar, 100 nm. d, The segmented volume of c, shown as an overview (left) and zoomed-in views of the clashed (top right; numbers 1–4) and docked (bottom right; number 5) E45A cores. E45A cores, NPCs, nucleosomes, ribosomes, NE and membranes are segmented and shown in the indicated colours. e, A representative tomographic slice of a correlatively acquired tomogram of HIV-1 E45A/R132T core nuclear import. Two E45A/R132T cores are identified and indicated by light purple arrowheads and numbered as follows: number 1 shows a docked cone-shaped E45A/R132T core with the wide end on the NPC; and number 2 shows an imported tube-shaped E45A/R132T core with discernible surrounding densities, also shown on another slice of the same tomogram (white framed). The NPC, ribosomes, nucleosomes and prominent surrounding nuclear factors are labelled. The nucleus, NE and membranes are annotated accordingly. Scale bar, 100 nm. f, The segmented volume of e, shown as an overview (left) and zoomed-in views of the docked (top right; number 1) and imported (bottom right; number 2) E45A/R132T cores. E45A/R132T cores, NPCs, nucleosomes, nuclear factors, ribosomes, NE and membranes are segmented and shown in the indicated colours. g, A bar chart showing the distribution of HIV-1 cores in each state across three samples: WT, E45A and E45A/R132T. The imported fraction in each case is annotated. Significance was determined using a two-sided Chi-square test for all; P < 0.0001. h, A violin plot of the statistical analysis of the size of E45A cores (width measured at the wide end) in each state. Imported E45A cores measure 44.80 ± 5.644 nm (s.e. = 1.262, n = 20), traversing cores measure 46.79 ± 6.658 nm (s.e. = 1.780, n = 14), docking cores measure 55.51 ± 6.993 nm (s.e. = 0.4135, n = 286), approaching cores measure 54.82 ± 7.250 nm (s.e. = 0.5842, n = 154) and input cores measure 55.17 ± 9.483 nm (s.e. = 0.6147, n = 238). The white lines represent the medians, black lines represent the quartiles and black dots represent individual E45A cores. Significance was determined using two-sided Brown–Forsythe and Welch ANOVA tests for all; **P < 0.01 (**P = 0.0038 for input versus traversing, **P = 0.0053 for approaching versus traversing, **P = 0.0028 for docking versus traversing), ****P < 0.0001 (only significant differences are shown). i, A violin plot of the statistical analysis on the size of E45A/R132T cores (width measured at the wide end) in each state. Imported E45A/R132T cores measure 44.84 ± 5.965 nm (s.e. = 1.369, n = 19), traversing cores measure 52.33 ± 6.670 nm (s.e. = 1.362, n = 24), docking cores measure 55.43 ± 9.228 nm (s.e. = 1.776, n = 27), approaching cores measure 53.88 ± 9.925 nm (s.e. = 1.754, n = 32) and the input cores measure 55.43 ± 10.53 nm (s.e. = 0.7763, n = 184). The white lines represent the medians, black lines represent the quartiles, and black dots represent individual E45A/R132T cores. Significance was determined using two-sided Brown–Forsythe and Welch ANOVA tests for all; **P < 0.01 (**P = 0.0018 for approaching versus imported, **P = 0.0038 for traversing versus imported), ***P = 0.0003, ****P < 0.0001 (only significant differences are shown).

Using correlative cryo-ET, we analysed 474 nucleus-associated E45A cores at different stages of nuclear translocation (Fig. 5c,d, Extended Data Fig. 8a and Supplementary Video 9). Despite their morphological similarity to WT cores (Extended Data Fig. 1d–g), their interaction with the NPC differed significantly. Tomographic analysis revealed a marked reduction not only in the number of imported E45A cores (20 of 474) but surprisingly also in the number of cores traversing NPCs (Fig. 5g). As a result, there was a substantial accumulation of cores stalled at the docking stage (Figs. 4h and 5g). The NPC appeared to act as a bottleneck to prevent E45A cores from entering and, on average, more E45A cores docked to the same NPC compared with WT cores (Extended Data Fig. 8a,c). As WT and E45A cores were morphologically indistinguishable (Extended Data Figs. 1d–g and 9a–b), these observations implied that the decreased elasticity of E45A cores impeded their ability to enter the NPC channel, emphasizing the importance of capsid remodelling for efficient nuclear import. Inherent E45A inelasticity also influenced the types of cores that passed through nuclear pores. The size of the 14 E45A cores found inside NPCs were smaller than those in docking and approaching stages and had a higher percentage of tube-shaped cores, similar to those that were imported (Fig. 5h and Extended Data Figs. 8e and 9c,d), a clear distinction from WT cores (Fig. 1f and Extended Data Fig. 9c,d). These observations reinforced that smaller-sized cores provide a selective advantage for nuclear import, particularly when the capsid lattice is inherently resistant to remodelling. As expected, E45A/R132T cores closely mirrored the nuclear docking, traversing and import dynamics of WT cores (Fig. 5e–g,i, Extended Data Fig. 10 and Supplementary Video 10).

Discussion

In this work, we developed a near-native functional HIV-1 nuclear import system that substantially increases import events compared with infected T cells and macrophages, enabling direct in situ visualization of individual cores undergoing nuclear import for structural investigation. It allowed imaging of a substantial number of HIV-1 cores at multiple stages of nuclear translocation along with their counterpart NPCs, facilitating systematic analysis with robust statistics. Furthermore, the system reliably recapitulated nuclear entry defects associated with HIV-1 mutants, showing its physiological relevance.

Confocal fluorescence imaging and cryo-ET analysis consistently showed that HIV-1 cores engage robustly with NPCs, underscoring the capsid’s high specificity and affinity for NPCs39,40. The pronounced accumulation of cores at the nuclear envelope compared with the nucleoplasm confirms that nuclear import is a rate-limiting step in HIV-1 infection. These findings further reveal that HIV-1 nuclear import is highly selective, favouring the traversal of smaller cone-shaped and tube-shaped cores, which is unlikely an artefact of our import system, as the NPCs closely resemble those in intact CEM cells (Fig. 2b,c and Extended Data Fig. 2c).

The elasticity of the HIV-1 core is crucial for HIV-1 infection, impacting nuclear import and subsequent uncoating56,63,74. Recent atomic force microscopy and molecular dynamics simulation studies showed that core elasticity is essential for traversing through NPCs56,63. Mutations that reduce core elasticity (for example, E45A and Q63A/Q67A), or the addition of capsid inhibitors such as PF74 and lenacapavir, inhibit HIV-1 nuclear import56. Here, we provide in situ evidence of HIV-1 capsid remodelling within NPCs, along with a major ‘bottleneck’ at the entry of nuclear pores for E45A cores. As the E45A mutation does not directly affect the capsid’s FG-binding pocket, its failure to enter the NPC channel reinforces the importance of capsid elasticity for successful NPC traversal70,71.

NPCs are known to be flexible, dynamic and capable of adapting to constricted or dilated forms depending on cell state23,24,25,26,28,75. We observed a small but distinct expansion (~2 nm) of NPCs during WT core translocation. In addition to the expansion, substantial NPC deformation was detected upon core entry. These findings align with recent studies showing that HIV-1 core traversal cracks NPCs29,63. Of note, we preferred the term ‘deform’ over ‘crack’.

CPSF6 has been implicated in facilitating the release of the HIV-1 cores from the NPC and downstream translocation to nuclear speckles18,38. We observed N74D cores, which are defective for CPSF6 binding, accumulated and stalled within NPCs, consistent with previously observed prolonged residence time of N74D cores at the nuclear envelope16. We further observed a distinct density layer surrounding imported WT, E45A and E45A/R132T cores, but not N74D cores. This density is consistent with the CPSF6 density observed in our cryo-EM map of capsid–CPSF6 complexes, suggesting that CPSF6 is a major component of the nuclear factors mediating core trafficking in the nucleoplasm, in line with previous cell-based assays18,38,43,44,45,46,68.

In summary, our study revealed individual stages of HIV-1 nuclear import, downstream trafficking, and the detailed interplay between HIV cores and NPCs (shown in Fig. 6). The system we developed will permit direct analysis of the role of specific host proteins, such as CypA and CPSF6, and of drugs, such as lenacapavir, in HIV nuclear entry and uncoating. Combined with our recent cryo-ET characterization of chromatin76, we envision that this system may one day lead to in situ visualization of HIV-1 integration. Advanced imaging techniques—such as super-resolution fluorescence microscopy, including minimal fluoroescence photon fluxes (MINFLUX), especially when combined with direct capsid labelling22,48—and the powerful correlative cryo-ET platform established herein will offer comprehensive mechanistic insights into the dynamic process of HIV-1 infection.

Fig. 6: Model for HIV-1 and NPC interplay during nuclear import.
figure 6

Left: WT cores are shown. First, comparatively small and tube-shaped cores are preferentially imported through the NPC. Once inside the nucleus, imported cores are transported by nuclear factors, including CPSF6, to integration sites, where uncoating occurs, releasing the viral genome. Second, the docking orientation of HIV-1 cores is random; however, traversal through the NPC favours entry via the narrow end of cone-shaped cores. Third, NPCs expand during HIV-1 core traversal and this process can deform the NPC, as depicted in the top left (framed by dashed lines). Right: the influence of capsid elasticity and CPSF6 binding on HIV-1 nuclear import is shown, exemplified by the E45A mutant, which has a brittle capsid, and the N74D mutant, which is defective for CPSF6 binding. Brittle capsids cause HIV-1 cores to pile up on the NPC and disruption of CPSF6 binding hinders accumulation of core-associated extraneous nuclear density and directional inward movement.

Methods

Mammalian cell culture

Cell lines were maintained in an incubator at 37 °C and 5% CO2. Human embryonic kidney (HEK) 293T Lenti-X cells (632180; Takara/Clontech) were obtained directly from the vendor. According to the manufacturer, the cells undergo quality-control testing, including mycoplasma detection and short-tandem-repeat profiling, to confirm identity. HEK293 T Lenti-X cells were cultured in DMEM (Gibco) supplemented with 10% fetal bovine serum (FBS), 2 mM l-glutamine (Gibco) and 1% MEM non-essential amino acids (neAA; Gibco). CD4+ T lymphocyte CEM cells (ARP-117; NIH HIV Reagent Program) have not been authenticated. CEM cells were cultured in RPMI-1640 (Sigma-Aldrich) medium supplemented with 10% FBS and 2 mM l-glutamine (Gibco); these cells were not further authenticated.

HIV-1 virion production

For ‘in-virion’ core analysis, HIV-1 virus particles were produced by transfecting HEK293T cells with pNL4-3 (Env) vectors together with NL4-3 Env expression vector pIIINL4env using Lipofectamine 2000 (Invitrogen) as previously described77. Culture media from transfected cells were collected at 48 h post-transfection and cleared by filtration through a 0.45-µm polyvinylidene fluoride filter. The virions were concentrated by ultracentrifugation through an 8% OptiPrep (Sigma-Aldrich) density gradient (100,000g; AH-629 rotor; Sorvall) for 1 h at 4 °C. The concentrated virions were further purified by ultracentrifugation (120,000g; TH-660 rotor; Sorvall) through a 10–30% OptiPrep gradient for 2.5 h at 4 °C. The opalescent band was collected, diluted with PBS and ultracentrifuged at 110,000g at 4 °C for 2 h. Pelleted particles were resuspended in 5% sucrose in PBS solution and stored at −80 °C until use.

Production of HIV-1 virus-like particles

HIV-1 virus-like particles (VLPs) were produced by transfecting Lenti-X HEK293T cells seeded in 8 T75 flasks at ~80% confluence. Transfections were performed using GenJet II reagent (SignaGen Laboratories). A transfection mixture was prepared by adding 40 µg of psPAX2 plasmid (psPAX2 was a gift from Didier Trono; Addgene plasmid number 12260; RRID:Addgene_12260) DNA in 2 ml DMEM lacking FBS. Separately, 100 µl of GenJet II was diluted in 2 ml of DMEM without FBS, added to the plasmid DNA mixture and incubated at room temperature (RT) for 10 min. Before transfection, each flask was refreshed with 7.5 ml of DMEM supplemented with 10% FBS, 1% neAA and 1% l-glutamine. Then, 500 µl of the transfection mixture was added dropwise to each flask. Cells were incubated for 48 h to allow VLP production before the supernatant was collected.

CPSF6 binding to streptolysin-O-treated HIV-1 VLPs

Recombinant MBP-tagged CPSF6 was purified as previously described78. To permeabilize the membrane of HIV-1 VLPs for CPSF6 binding, streptolysin O (SLO) was first reconstituted by adding 100 µl of STE buffer to a vial containing 25,000–50,000 U SLO, followed by gentle mixing. The reconstituted SLO solution was then added to the VLPs at a ratio of 1.5:10 (SLO:VLP, v/v), immediately followed by the addition of inositol hexaphosphate (IP6) to a final concentration of 1 mM. Following incubation at RT for 30 min, 5 µM MBP-tagged CPSF6 was added and the sample was incubated at RT for another 30 min before plunge freezing.

Production of mNeonGreen-IN-labelled HIV-1 particles containing near-full-length HIV-1 RNA

HIV-1 particles containing the viral RNA genome were produced by transfecting Lenti-X HEK293T cells seeded in 4 T175 flasks at ~80% confluence. Transfections were performed using polyethyleneimine (PEI; branched, molecular weight of ~25,000; Sigma-Aldrich). A transfection mixture was prepared by combining 24 µg of Env-defective HIV-1 constructs (R9ΔE-CA-WT, R9ΔE-CA-E45A, R9ΔE-CA-E45A/R132T or R9ΔE-CA-N74D)56 and 6 µg of Vpr-mNeonGreen-IN plasmid DNA (a gift from Prof. Zandrea Ambrose’s laboratory at the University of Pittsburgh) with 120 µg of PEI in OptiMEM medium. Mixtures were incubated at RT for 20 min before flask addition. After 16 h, the OptiMEM medium was replaced with fresh DMEM supplemented with 10% FBS, 1% neAA and 1% l-glutamine. Cells were incubated for 24 h before the HIV-1-containing supernatant was collected.

mNeonGreen-IN-labelled HIV-1 core isolation

Virus core isolation was performed using a previously described protocol57 with adjustments. The virus-containing supernatant was filtered using a 0.45-μm filter (Sarstedt). The filtered supernatant was added to 38.5 ml ultracentrifuge tubes (344058; Beckman Coulter) and underlaid with 5 ml 20% sucrose in 1× STE (10 mM Tris-HCl pH 7.4, 100 mM NaCl, 1 mM EDTA pH 8.0). The HIV-1 particles were pelleted by centrifugation using the SW32Ti rotor (Optima XPN-90; Beckman Coulter) for 3 h, 85,527g at 4 °C. After centrifugation, the supernatant and sucrose cushion were removed, and the tube was inverted onto a tissue to dry for ~5 min. The remaining liquid was removed by cleaning the inside walls of the tube using a tissue (Kimtech) without touching the pellet. Each pellet was resuspended in 400 μl 1× STE supplemented with 1 mM IP6.

A sucrose gradient was prepared in a 13.2 ml ultracentrifuge tube (344059; Beckman Coulter). All buffers were supplemented with 1× STE and 1 mM IP6. The layers were added from bottom to top using 2 ml stripettes: 2 ml 85% sucrose, 1.7 ml 70% sucrose, 1.7 ml 60% sucrose, 1.7 ml 50% sucrose, 1.7 ml 40% sucrose and 1.7 ml 30% sucrose. The gradient was then stored at 4 °C for ~7–8 h. Before use, 250 μl 15% sucrose supplemented with 1% Triton X-100 was added on top of the gradient, and a layer of 7.5% sucrose was added on top of the Triton X-100 layer to provide a barrier between the HIV-1 particles and the Triton X-100 before centrifugation. Finally, 800 μl of concentrated HIV-1 particles was added on top of the 7.5% sucrose layer and topped off with 1× STE and 1 mM IP6. The sample was separated by centrifugation using a SW41Ti rotor (Optima XPN-90; Beckman Coulter) for 15–17 h, 182,625g at 4 °C.

The sample was collected immediately after stopping the centrifuge. The mNeonGreen band corresponding to HIV-1 cores was visualized using a blue light transilluminator and collected by side puncturing the ultracentrifugation tube using a 25-G needle (BD Microlance 3). HIV-1 cores were quantified using a p24 ELISA kit. The isolated cores were either snap frozen in single-use aliquots with liquid nitrogen and stored at −80 °C or dialysed overnight at 4 °C against 500 ml of 1× SHE buffer (10 mM HEPES-NaOH pH 7.4 + 100 mM NaCl + 1 mM EDTA pH 8.0) supplemented with 0.8 mM IP6 using a 0.1–0.5 ml 7 kDa cut-off Slide-A-Lyzer Dialysis Cassette (Thermo Fisher Scientific) before mixing with permeabilized T cells.

T cell membrane permeabilization

T cell membrane permeabilization was performed using cells in the exponential growth phase at a concentration of ~1 × 106 cells ml−1. Cells were pelleted by centrifugation at 500g for 5 min at 4 °C, washed twice with 10 ml ice-cold PBS and pelleted again under the same conditions. For permeabilization, the washed pellet was resuspended in lysis buffer (20 mM HEPES pH 7.5, 25 mM KCl, 5 mM MgCl2, 1 mM DTT and 1× protease inhibitor) supplemented with 0.018% digitonin. The incubation was carried out at RT with rotation for 10 min, following the protocol described previously58. After incubation, cells were subjected to a brief centrifugation at 200g for 1 min and the supernatant was removed. The pellets were resuspended in fresh lysis buffer without digitonin to eliminate residual digitonin. To evaluate nuclear integrity, digitonin-permeabilized CEM cells were incubated with 0.2 mg ml−1 FITC-dextran (500 kDa; catalogue number 46947; Sigma-Aldrich) in lysis buffer for 15 min at RT. Imaging was performed using a Leica TCS SP8 confocal microscope.

Mixing mNeonGreen-IN-labelled HIV-1 cores with permeabilized T cells

The nuclei of permeabilized T cells were stained with 1 μM SiR-DNA (Spirochrome) on ice for 30 min. Digitonin-permeabilized CEM cells (400,000) were incubated with HIV-1 cores (WT, E45A, E45A/R132T or N74D) at a 20 µg ml−1 CA concentration in a 40 µl reaction containing a buffer composed of 0.2 mM IP6, 20 mM HEPES (pH 7.5), 18.8 mM KCl, 20 mM NaCl, 0.25 mM EDTA, 3.8 mM MgCl2, 1 mM DTT and 1× protease inhibitor. After 30 min on ice, 10 µl of a supplement mix was added to the 40 µl reaction, achieving a final concentration of 16% (v/v) RRL (catalogue number L4151; Promega), 0.6 mM ATP, 0.06 mM GTP, 5 mM creatine phosphate and 10 U µl−1 creatine kinase. The reaction was then incubated at 37 °C for 30 min. For cryo-FIB and cryo-ET, samples were fixed with 5 mM ethylene glycol bis(succinimidyl succinate) (EGS) (30 min, RT), inactivated with 50 mM Tris-HCl (pH 7.5) and kept on ice before grid preparation.

Confocal microscopy and fluorescence image processing

For all light microscopy imaging, we used the Leica TCS SP8 confocal microscope equipped with a HC PL Apo x63 MotCORR Water CS2 Objective numerical aperture (NA) 1.2 and a HyD GaAsP detector, controlled with LAS X software (Leica). Excitation with 488 nm, 561 nm and 633 nm laser lines was used and dynamic filter settings were applied. z stacks were collected with a 0.3- to 0.5-μm step size. For both imaging and z stacks, a 1 a.u. pinhole and a 1,024 pixel × 1,024 pixel resolution was used. Images, z stacks, were processed using Leica Application Suite X (Leica), Fiji ImageJ79 and Arivis Vision4D.

To analyse mNeonGreen-IN puncta representing HIV-1 cores associated with nuclei or located inside nuclei, confocal image stacks were processed using Arivis Vision4D software (v.4.1.2). Nuclei were segmented using the Cellpose algorithm integrated into Arivis Vision4D. The SiR-DNA channel was used to guide segmentation. The Cellpose settings were optimized with the cyto2 model for nuclear detection. Optimized parameters to ensure accurate identification of nuclear boundaries included a mask threshold of 2.5, a mask quality threshold of 0.2 and a nuclear diameter of 10 µm. The resulting nuclear segmentations were exported as three-dimensional (3D) objects for further analysis. For mNeonGreen-IN puncta detection, the Blob Finder tool in Arivis was applied to the mNeonGreen fluorescence channel. The following parameters were applied to optimize detection while minimizing false positives: normalization, manual; thresholding, auto threshold; blob size, 0.35 µm; probability threshold (P, threshold), ~30%; and split sensitivity, 40%. Puncta were classified as either ‘imported’ or ‘decorating’ based on spatial colocalization with nuclear boundaries. Puncta entirely enclosed within a nucleus were classified as imported, whereas those partially overlapping with nuclear boundaries were categorized as decorating. Quantitative analyses and measurements were performed using the built-in tools in Arivis Vision4D, and data were exported for statistical analysis. To ensure reliable and accurate results, counts for each individual nucleus were inspected manually.

Plunge-freezing vitrification

The samples were plunge frozen on glow-discharged gold finder grids, R2/2 Au G300F1 (Quantifoil), or copper grids, R2/1 Cu 300 (Quantifoil), using the Leica EM GP2 automated plunge freezer (Leica). Sample preparation was conducted in the blotting chamber at 20 °C with 95% humidity. The mixture of HIV-1 cores with permeabilized CEM cells was incubated with 10% glycerol for 2 min before plunge freezing. A mixture of 3–6 μl of HIV-1 cores and permeabilized CEM cells (~4,000 cells μl−1) was added to the carbon side of the grid, while 1 μl of PBS was added to the back side of the grid. The grids were back-blotted for 6 s using filter blotting paper (Whatman) and immediately plunge frozen in liquid ethane. For control groups, 3.5 μl of native HIV-1 virions, HIV-1 cores and MBP-tagged CPSF6 bound to the perforated VLPs were added to the carbon side of the grid, blotted from the back for 3 s and then plunge frozen in liquid ethane. For intact CEM cells, ~3,000 cells μl−1 were blotted for 8 s using EM GP2 automated plunge freezer (Leica).

Correlative cryo-FIB milling

The vitrified mixture of permeabilized CEM cells with or without supplementation of RRL-ATP and HIV-1 cores was further thinned by cryo-FIB milling to prepare lamellae, guided by cryo-CLEM in two systems. Eight grids were then loaded by a robotic delivery device (Autoloader) onto an Arctis dual-beam FIB–scanning electron microscope (SEM) (Thermo Fisher Scientific). This microscope is equipped with a cryogenic stage cooled to −191 °C, a wide-field integrated fluorescence microscope system with a 100× objective (NA 0.75) and a plasma multi-ion source (argon, xenon and oxygen), with argon used as the FIB source in this study.

Before milling, an organometallic platinum layer was deposited on the grid using the gas injection system (GIS) (Thermo Fisher Scientific) for 50 s. The 3D correlative milling was performed using the embedded protocol in WebUI v.1.1 (Thermo Fisher Scientific), with the milling angle adjusted to 10°. For each position, a 15-μm stack composed of fluorescence (GFP) and reflection images was acquired at a step size of 500 nm after rough milling using default parameters. The positions of targeted fluorescence spots were calculated using discernible ice chunks as fiducial markers in both SEM and FIB images, guiding the placement of lamella preparation patterns. The lamellae were produced in a stepwise sequence: (1) opening at 2 nA, (2) rough milling at 0.74 nA and 0.2 nA, and (3) polishing at 60 pA, with the final thickness of lamellae set to 140 nm. To enhance signal detection on polished lamellae, the step size was changed to 100 nm, resulting in a 15-μm stack composed of 101 images in both GFP and far-red channels.

Sixteen grids were loaded onto a dual-beam FIB–SEM microscope, Aquilos 2 (Thermo Fisher Scientific), equipped with a cryo-transfer system and rotatable cryo-stage cooled to −191 °C by an open nitrogen circuit. The Aquilos 2 FIB–SEM microscope was modified to accommodate a fluorescence light microscopy system, METEOR, with a 50× objective (NA 0.8; Delmic Cryo BV). Grids were mounted on a METEOR shuttle with a pre-tilt of 26°, followed by coating with an organometallic platinum layer using the GIS (Thermo Fisher Scientific) for 30 s. The milling angle was set to 10°. Cells seeded in optimal positions (near the centre of the grid square) were selected for lamella production. Before milling, fluorescence stacks were collected for all selected positions in both GFP and far-red channels at a step size of 200 nm, ranging ±6 μm from the focal point. The stacks were further processed in ImageJ80 to enhance the signal-to-noise ratio. FIB and SEM images were then acquired and correlated with the fluorescence images using the open-source software 3D Correlation Toolbox81, with discernible ice chunks used as fiducial markers. Lamella preparation patterns were then placed based on the correlated positions, followed by sequential milling conducted by the software AutoTEM 5 (Thermo Fisher Scientific) at 0.5 nA (rough milling), 0.3 nA (medium milling), 0.1 nA (fine milling), 60 pA (first polishing) and 30 pA (final polishing), with the final thickness of lamellae set to 120 nm. After final polishing, fluorescence stacks of lamellae were acquired in both GFP and far-red channels at a step size of 100 nm, ranging ±2 μm from the focal point. The light intensity and exposure time were set to 400 mW and 300 ms for the METEOR system. In total, 35 lamellae and 85 lamellae with discernible fluorescence were produced in Arctis and Aquilos 2, respectively.

For intact CEM cells, blind milling was conducted. Thinning was performed using the dual-beam FIB–SEM microscope Aquilos 2 (Thermo Fisher Scientific) equipped with a cryo-transfer system and a rotatable cryo-stage maintained at −191 °C via an open nitrogen circuit. Before milling, grids were mounted onto a shuttle, transferred to the cryo-stage and coated with an organometallic platinum layer using the GIS (Thermo Fisher Scientific) for 5–6 s. Cells located near the centres of grid squares were selected for thinning. The process was carried out stepwise using the automated milling software AutoTEM 5 (Thermo Fisher Scientific), with currents decreasing incrementally from 0.5 nA to 30 pA at 30 kV. The final thickness of the lamellae was set to 120 nm.

Cryo-ET data collection and data processing

For the experimental group, lamellae were transferred to 3 FEI Titan Krios G3 (Thermo Fisher Scientific) electron microscopes operated at 300 kV and equipped with a Falcon 4i detector and a Selectris X energy filter (Thermo Fisher Scientific). Objective apertures of 100 µm were inserted. Lamella overviews were generated by stitching images acquired at a magnification of ×8,100. The transmission electron microscopy lamella overviews were then correlated with the fluorescence lamella images in ImageJ80. Following that, tilt series were collected on the correlated sites and neighbouring areas without overlap. The collection was performed using Tomography 5 software (Thermo Fisher Scientific) at a magnification of ×64,000.

For permeabilized CEM cells incubated with WT cores, a total of 138 tilt series were collected with a nominal physical pixel size of 1.94 Å pixel−1. The pre-tilts of lamellae were determined at ±10° and a dose-symmetric scheme was applied, ranging from −44° to +64° with an increment of 2°. A total of 55 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 2.5 e Å−2 per tilt, resulting in a total dose of 137.5 e Å−2 and the defocus value was set from −3 µm to −5 µm.

For permeabilized CEM cells incubated with WT cores supplemented with RRL-ATP, a total of 460 tilt series were collected with a nominal physical pixel size of 1.903 Å pixel−1, and 161 tilt series were collected with a nominal physical pixel size of 1.94 Å pixel−1. The pre-tilts of lamellae for each series were determined at ±10° and ±12°, respectively, and a dose-symmetric scheme was applied, ranging from −42° and −45° to +66° and +65° with an increment of 2°. A total of 53 and 55 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 2.5 e Å−2 per tilt, resulting in a total dose of 132.5 e Å−2 and 137.5 e Å−2, and the defocus value was set from −3 µm to −5 µm.

For permeabilized CEM cells incubated with E45A cores supplemented with RRL-ATP, a total of 207 tilt series were collected with a nominal physical pixel size of 1.903 Å pixel−1. A total of 115 tilt series were collected with a nominal physical pixel size of 1.94 Å pixel−1. The pre-tilts of lamellae were determined at ±10° and a dose-symmetric scheme was applied, ranging from −44° to +64° with an increment of 2°. A total of 55 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 2.5 e Å−2 per tilt, resulting in a total dose of 137.5 e Å−2, and the defocus value was set from −3 µm to −5 µm.

For permeabilized CEM cells incubated with E45A/R132T cores supplemented with RRL-ATP, a total of 122 tilt series were collected with a nominal physical pixel size of 1.903 Å pixel−1. The pre-tilts of lamellae were determined at ±10° and a dose-symmetric scheme was applied, ranging from −44° to +64° with an increment of 2°. A total of 55 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 2.5 e Å−2 per tilt, resulting in a total dose of 137.5 e Å−2, and the defocus value was set from −3 µm to −5 µm.

For permeabilized CEM cells incubated with N74D cores supplemented with RRL-ATP, a total of 179 tilt series were collected with a nominal physical pixel size of 1.94 Å pixel−1. The pre-tilts of lamellae were determined at ±10° and a dose-symmetric scheme was applied, ranging from −44° to +64° with an increment of 2°. A total of 55 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 2.5 e Å−2 per tilt, resulting in a total dose of 137.5 e Å−2, and the defocus value was set from −3 µm to −5 µm.

For intact CEM cells, a total of 47 tilt series were collected with a nominal physical pixel size of 2.18 Å pixel−1 using an FEI Titan Krios G2 (Thermo Fisher Scientific) electron microscope operated at 300 kV and equipped with a Gatan BioQuantum energy filter and post-GIF K3 detector (Gatan). A 100-µm objective aperture was inserted. Areas that include nuclei were selected for the data acquisition. Tilt series were recorded using Tomography 5 software (Thermo Fisher Scientific). The pre-tilts of lamellae were determined at ±12° and a dose-symmetric scheme was applied, ranging from −42° to +66° with an increment of 3°. A total of 37 projection images with 10 video frames each were collected for each tilt series, with the dose rate set to 3 e Å−2 per tilt, resulting in a total dose of 111 e Å−2, and the defocus value was set from −3 µm to −5 µm.

For the control groups, grids were loaded onto an FEI Titan Krios G2 (Thermo Fisher Scientific) electron microscope operated at 300 kV and equipped with a Gatan BioQuantum energy filter and post-GIF K3 detector (Gatan). A 100-µm objective aperture was inserted. For the grid of near-full-genome virions and CPSF6-bound perforated VLPs, 58 and 100 tilt series, respectively, were collected using Tomography 5 software (Thermo Fisher Scientific) at a magnification of ×81,000 with a nominal pixel size of 1.34 Å pixel−1. A dose-symmetric scheme was applied with a tilt range of ±60° from 0° with an increment of 3°. Defocus was set from −1.5 µm to −3 µm, and the dose rate was set to 3 e Å−2 per tilt. A total of 41 projection images with 10 video frames each were collected for each tilt series, resulting in a total dose of 123 e Å−2. Micrographs of HIV-1 cores (3,000 micrographs for WT, 2,000 for E45A, 2,500 for E45A/R132T and 2,500 for N74D) were acquired using EPU (Thermo Fisher Scientific) on a Glacios microscope. Data were collected at a magnification of ×73,000 with a nominal pixel size of 2 Å pixel−1. For each micrograph, a total of 40 frames were recorded with a cumulative dose of 40 e Å−2. The defocus was value was set between −3.0 µm and −4.0 µm.

Alignment of tilt series

The frames of each tilt series were corrected for beam-induced motion using MotionCor2 (ref. 82). For the alignment and generation of tomograms, tilt series were aligned in IMOD v.4.11 (ref. 83) by patch tracking, using patches of 200 pixels × 200 pixels and a fractional overlap of 0.45 in both x and y. The alignment results were inspected manually and bad frames were removed. For the control group of native virions, 58 tomograms were reconstructed at a pixel size of 8.04 Å pixel−1. For permeabilized CEM cells incubated with WT cores, a total of 138 tomograms were reconstructed at bin 6 at a pixel size of 11.64 Å pixel−1. For permeabilized CEM cells incubated with WT cores supplemented with RRL-ATP, a total of 621 tomograms were reconstructed at bin 6, with 460 tomograms at a pixel size of 11.418 Å pixel−1 and 161 tomograms at a pixel size of 11.64 Å pixel−1. For permeabilized CEM cells incubated with E45A cores supplemented with RRL-ATP, a total of 322 tomograms were reconstructed at bin 6, with 207 tomograms at a pixel size of 11.418 Å pixel−1 and 115 tomograms at a pixel size of 11.64 Å pixel−1. For permeabilized CEM cells incubated with E45A/R132T cores supplemented with RRL-ATP, a total of 122 tomograms were reconstructed at bin 6 at a pixel size of 11.418 Å pixel−1. For permeabilized CEM cells incubated with N74D cores supplemented with RRL-ATP, a total of 179 tomograms were reconstructed at bin 6 at a pixel size of 11.64 Å pixel−1. For WT HIV-1 virions and CPSF6-bound perforated VLPs, a total of 58 and 100 tomograms, respectively, were reconstructed at bin 6 at a pixel size of 8.04 Å pixel−1. For intact CEM cells, a total of 47 tomograms were reconstructed at bin 6 at a pixel size of 13.08 Å pixel−1. Simultaneous Iterative Reconstruction Technique-like filtering was applied to all reconstructed tomograms with 8 iterations for better visualization.

Measurements of HIV-1 cores and NPCs

To measure the diameters of NPCs and the width of HIV-1 cores at different stages of nuclear import, tomograms were reconstructed using IMOD v.4.11.1 with a binning factor of 4. This resulted in pixel sizes of 7.64 Å pixel−1 for permeabilized CEM cells incubated with WT cores, 7.612 Å pixel−1 and 7.76 Å pixel−1 for permeabilized CEM cells incubated with WT and E45A cores supplemented with RRL-ATP, 7.612 Å pixel−1 for permeabilized CEM cells incubated with E45A/R132T cores supplemented with RRL-ATP, 7.76 Å pixel−1 for permeabilized CEM cells incubated with N74D cores supplemented with RRL-ATP, 8.72 Å pixel−1 for intact CEM cells and 5.36 Å pixel−1 for HIV-1 cores in native virions. The central slices of each NPC and HIV-1 core were then imported into ImageJ80 for precise measurements. Lines (five lines on average) were drawn between the measuring points (outer nuclear membrane–inner nuclear membrane fusion points for NPCs and the widest part for cores) and grey values were calculated along the lines. The average distance between two dropping points was recorded. Grey-value measurements were taken to assess the change in density as a function of distance from the surface of native HIV-1 cores. For each core, 20 lines were drawn, starting from the capsid surface including partial density of the CA (~3 nm). Black density was assigned a value of zero and white was assigned a value of one, with higher densities corresponding to lower values. The number of cores used for the measurement was as follows: WT outside (n = 10), WT traversing (n = 10), WT imported (n = 10), E45A imported (n = 10), E45A/R132T (n = 10) and N74D imported (n = 5).

For the experimental groups, 685 WT cores, 474 E45A cores, 102 E45A/R132T cores and 73 N74D cores were measured, with the remainder being unmeasurable because they partially resided within the tomogram. For native virions, 214 cores were measured. For input cores, 128 WT cores, 239 E45A cores, 184 E45A/R132T cores and 196 N74D cores were measured directly on the motion-corrected micrographs. For NPCs with clearly definable double nuclear envelope boundaries, 170 NPCs were measured in permeabilized CEM cells without supplementation, while 196 NPCs were measured in permeabilized CEM cells supplemented with RRL-ATP and 50 NPCs were measured in intact CEM cells.

Template matching

To localize individual CA hexamers in the tomogram, template matching was performed using emClarity v.1.5.0.2 (ref. 64) with non-CTF-corrected tomograms binned at 6×. The procedure used a template derived from EMD-12452 (ref. 14), which was low-pass filtered to 30 Å. An exhaustive search was performed using a threshold of 2,000 peaks in the small cropped-out tomogram region (150 nm3) containing HIV-1 cores. HIV-1 CA hexamer peaks were selected with the MagpiEM tool (available at https://github.com/fnight128/MagpiEM), and particle selection was identified based on the geometric constraints of the capsid lattice. Any hexamers that did not conform to the expected hexagonal lattice geometry were automatically excluded, followed by manual inspection to ensure selection precision (see Extended Data Fig. 6a). To localize 80S ribosomes and nucleosomes, the same procedure was used without the MagpiEM inspection, using low-pass-filtered maps derived from EMD-1780 (ref. 84) and EMD-16978 (ref. 76), respectively. To match the subunits of NPCs, 1/8 of the original density map EMD-11967 (ref. 21) was cropped out based on the 8-fold symmetry and further low-pass filtered to 60 Å. The same exhaustive search was used by giving a peak threshold of 200 in the small cropped-out tomogram region (300 nm3) containing the NPC. NPC subunit peaks were initially examined in Chimera by thresholding the cross-correlation value, and then selecting using the MagpiEM tool. Particle selection was identified based on the geometric constraints of NPC symmetry. Any subunit that did not align with the expected symmetry of the NPC and orientation were automatically excluded, followed by manual inspection with original tomograms to ensure selection precision (Extended Data Fig. 6c).

STA

The 3D alignment and averaging of hexameric CA were refined through progressive binning steps, from 6× to 2× binning, using emClarity v.1.5.3.10 (ref. 65) and maintaining C6 symmetry throughout the alignment process. The final density map at 2× binning was enhanced by sharpening with a Debye–Waller factor (B-factor) of −10. For the CA hexamer of outside (approaching and docking) WT cores, 128 tomograms were selected and 11,915 particles were used. For the CA hexamer of WT cores in the traversing state, 54 tomograms were selected and 5,545 particles were used. For the CA hexamer of imported WT cores, 51 tomograms were selected and 7,825 particles were used. The resolution of the reconstructed structure was calculated using a gold-standard Fourier shell correlation cut-off of 0.143. The final resolution was determined at 11 Å, 12 Å and 16 Å for CA hexamer structures of WT cores in outside, traversing and imported states, respectively (Extended Data Fig. 6b). Structural fitting was conducted in ChimeraX85, enabling detailed comparison of the density maps with PDB 6SKK (ref. 66). For the NPC, 1,121 matched particles were used for the structural determination of each NPC ring moiety. Each NPC ring moiety was included using the same box, shifting along the z axis from the original matched coordinates. Refinement was performed through progressive downsampling from binning of 8× to 4×. The resolution of the reconstructed structure was calculated using a gold-standard Fourier shell correlation cut-off of 0.143. The final resolution was determined at 22 Å, 29 Å, 32 Å and 36 Å for CR, IR, LR and NR, respectively (Extended Data Fig. 6d).

Segmentation

To enhance the segmentation, reconstructed bin-6 tomograms were corrected for the missing wedge and denoised using IsoNet v.0.2 (ref. 86), applying 35 iterations with sequential noise cut-off levels of 0.05, 0.1, 0.15, 0.2 and 0.25 at iterations 10, 15, 20, 25 and 30, respectively. Membranes and nuclear envelopes in all tomograms were initially segmented using MemBrain-seg87 and then imported into ChimeraX85 for manual cleaning and polishing. For the top view of nuclear envelopes, segmentation was performed in Amira (Thermo Fisher Scientific).

Nucleosomes and 80S ribosomes were mapped back to the tomograms with segmented membranes using ChimeraX85 and ArtiaX88, based on their positions and orientations after template matching. NPCs were manually placed back based on the positions of holes (occupied by NPCs) on segmented nuclear envelopes. HIV-1 cores were mapped back based on the refined coordinates and orientations of CA hexamers from STA, with missing CA hexamers manually placed back using the in situ CA hexamer structures resolved in this study. CA pentamers were only placed back on cores in which most CA hexamers were matched and the five surrounding hexamers identified and then modelled based on EMD-13422 (ref. 14). For deformed HIV-1 cores, CA hexamers were mapped back using the in situ CA hexamer structure of HIV-1 cores in the traversing state. For better visualization, 80S ribosomes depicted in the segmented volume were generated by applying a low-pass filter with a cut-off of 15 Å to the original model EMD-1780 (ref. 84). Nucleosomes and NPCs were depicted using EMD-16978 (ref. 76) and EMD-11967 (ref. 21), respectively. The viral RNA/DNA was traced along the prominent string-shaped densities and segmented in ChimeraX using ArtiaX.

Symmetry analysis of NPCs

To examine the symmetry of NPCs, template-matched and cleaned coordinates of individual NPCs were first visualized using the MagpiEM tool (available at https://github.com/fnight128/MagpiEM). NPCs meeting the following two criteria were retained: (1) at least three subunits were clearly matched with the correct orientation, and (2) at least one diameter was definable between two opposing subunits. Then, the direct distance between two adjacent subunits (assumed as subunit 1 and subunit 2 for simplification) was measured as D. The distance between subunit 1 and its opposing subunit was measured as d1, and the distance between subunit 2 and its opposing subunit was measured as d2. In cases where only one diameter could be measured, d1 and d2 were set to the same value. The two radii were then calculated as r1 and r2. The included angle (θ) between these two adjacent subunits was then determined using the following formula (also see Extended Data Fig. 6c):

$${{\rm{\theta }}=\cos }^{-1}\left(\frac{{{r}_{1}}^{2}+{{r}_{2}}^{2}-{D}^{2}}{2{r}_{1}{r}_{2}}\right)$$

NPCs with included angles calculated larger than 47.5° or smaller than 42.5° were regarded as deformed.

Statistical analysis

To assess the significance of size differences across HIV-1 cores in multiple states, Brown–Forsythe and Welch analysis of variance (ANOVA) tests were used. The Chi-square test was used to determine whether the distributions of cone-shaped and tube-shaped HIV-1 cores were independent of their states (Supplementary Tables 15). The Fisher’s exact test was used to examine whether the orientation of cone-shaped HIV-1 cores was independent of the two states: docking and traversing (Supplementary Tables 69). The significance of size differences in NPCs was assessed using an unpaired two-tailed t-test and one-way ANOVA test, including 170 empty NPCs in permeabilized CEM cells, 64 HIV-1-occupied NPCs and 132 empty NPCs in permeabilized and supplemented CEM cells, and 50 empty NPCs in intact CEM cells. The significance of size differences in HIV-1 cores across all groups was also assessed using an unpaired two-tailed t-test and one-way ANOVA test. Fisher’s exact and Chi-square tests were used to examine the import efficiency of all HIV-1 cores, to examine the distribution of all HIV-1 cores in terms of shape and states in all samples, and to assess the symmetry analysis of NPCs. The unpaired two-tailed t-test was used to assess the difference in size between regular and deformed occupied NPCs and the HIV-1 cores within them. All statistical analyses were calculated and plotted using Prism 10.

Reporting summary

Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article.