Promyelocytic leukemia nuclear bodies (PML-NBs) are mobile subnuclear organelles formed by PML and Sp100 protein. They have been reported to have a role in transcription, DNA replication and repair, telomere lengthening, cell cycle control and tumor suppression. We have conducted high-resolution 4Pi fluorescence laser-scanning microscopy studies complemented with correlative electron microscopy and investigations of the accessibility of the PML-NB subcompartment. During interphase PML-NBs adopt a spherical organization characterized by the assembly of PML and Sp100 proteins into patches within a 50- to 100-nm-thick shell. This spherical shell of PML and Sp100 imposes little constraint to the exchange of components between the PML-NB interior and the nucleoplasm. Post-translational SUMO modifications, telomere repeats and heterochromatin protein 1 were found to localize in characteristic patterns with respect to PML and Sp100. From our findings, we derived a model that explains how the three-dimensional organization of PML-NBs serves to concentrate different biological activities while allowing for an efficient exchange of components.
PML (promyelocytic leukemia) nuclear bodies (PML-NBs), also referred to as PML oncogenic domain (POD), Nuclear domain-10 (ND10) or Kremer (Kr) bodies, are mobile organelles that form distinct subcompartments in the cell nucleus as described in detail in a number of reviews (Bernardi and Pandolfi, 2007; Borden, 2008; Dellaire and Bazett-Jones, 2004; Melnick and Licht, 1999; Salomoni et al., 2008; Takahashi et al., 2004). PML-NBs appear as globular structures, 0.25 to 1 μm in diameter, in microscopy images. Typically, 5-30 PML bodies are found in a single cell, but their size and number can vary. About 80 proteins have been reported to colocalize with PML protein, as reviewed previously (Bernardi and Pandolfi, 2007; Borden, 2008; Dellaire and Bazett-Jones, 2004; Melnick and Licht, 1999; Salomoni et al., 2008; Takahashi et al., 2004). Among them are Sp100, the small ubiquitin-related modifier (SUMO), CBP (CREB-binding protein), Daxx, the Bloom's syndrome gene product (BLM) and NDP55. According to the colocalizing proteins, numerous diverse biological activities have been assigned to PML-NBs. These include transcription, antiviral defense, DNA replication and repair, telomere lengthening, chromatin organization and cell cycle control, as well as senescence, apoptosis and tumor suppression. PML protein is regarded as the central structural component of PML-NBs because these structures do not form in PML−/− cells (Ishov et al., 1999). Considerable interest in the biological function of PML originates from its role in acute promyelocytic leukemia (APL), in which a chromosomal translocation fuses the PML gene on chromosome 15q22 with the retinoic acid receptor (RAR) gene on chromosome 17q21 (Melnick and Licht, 1999). Furthermore, PML expression appears to be lost or reduced in many different human tumors, and PML−/− mice are highly susceptible to chemically induced or spontaneous tumorgenesis, pointing to the role of PML as a tumor suppressor (Bernardi and Pandolfi, 2007; Salomoni et al., 2008).
Seven splicing variants of the PML protein have been identified, with PMLI and PMLII being the most abundant. All PML isoforms include the N-terminus, but differ in the central core domain as well as the C-terminus. The N-terminus of PML contains three cysteine-rich metal-binding motifs (Goddard et al., 1991), a RING finger and two B-boxes (Borden et al., 1996), followed by a coiled-coil domain (Kastner et al., 1992; Perez et al., 1993). These three motifs are referred to as RBCC or TRIM domains, and are important for self-association of PML protein (Kentsis et al., 2002). In addition, PML has three modification sites for SUMO at Lys65, Lys160 and Lys490 (Kamitani et al., 1998a; Lallemand-Breitenbach et al., 2001) as well as a SUMO-interacting motif (SIM) (Fu et al., 2005; Kamitani et al., 1998b; Shen et al., 2006; Song et al., 2004; Sternsdorf et al., 1997). In addition, it has been proposed that PML itself has an E3 SUMO ligase activity that is located in its RING domain (Quimby et al., 2006; Shen et al., 2006). PML-NBs are highly sumoylated at interphase, but not during the metaphase, when the PML protein is found in particles that lack most of the PML colocalization partners (Everett et al., 1999). In particular, the Sp100 protein, which is regarded as a constitutive structural component of interphase PML-NBs and itself contains a sumoylation site and a SIM (Seeler et al., 2001; Sternsdorf et al., 1999; Sternsdorf et al., 1997), no longer associates with PML protein during metaphase. Thus, the formation of distinct PML-NBs appears to be critically dependent on: (1) the self-association properties of PML protein via its RBCC domain; (2) sumoylation in conjunction with the presence of a SIM in the PML protein; and (3) the incorporation of Sp100 into PML-NBs.
The structure of PML-NBs is usually described as ring-like or doughnut-shaped (Bernardi and Pandolfi, 2007; Dellaire and Bazett-Jones, 2004; Melnick and Licht, 1999; Salomoni and Pandolfi, 2002). This notion is based on imaging of immunostained PML protein (or colocalizing proteins) by confocal laser-scanning microscopy (CLSM) and electron microscopy (EM) (Boisvert et al., 2000a; Koken et al., 1994; Weis et al., 1994). The EM micrographs of immuno-gold-labeled PML-NBs in HeLa cells were described as ‘dense black grains lying over roughly spheroid particles that often display a doughnut-like morphology with typical diameters of 0.3 to 0.5 μm’ (Weis et al., 1994). PML-NBs visualized by immunostaining of a stably transfected CHO cell line as well as primary human haematopoietic cells showed spherical structures of 0.3-1 μm in diameter, with an outer electron-dense fibrillar capsule stained by the PML antibody (Koken et al., 1994). By transmission electron microscopy and electron spectroscopic imaging (ESI) of human neuroblastoma SK-N-SH cells, PML-NBs were characterized as spherical, dense and protein-based structures of 250 nm in diameter (Boisvert et al., 2000b). The structure of PML-NBs in two human cell lines was found to be insensitive to RNase and DNase treatment (Weis et al., 1994) and devoid of nucleic acids (Boisvert et al., 2000b). In agreement with this result, the mobility of PML-NBs in HeLa cells resembled that of a bona fide inert particle, and no indication for (transient) chromatin binding was detected (Görisch et al., 2004). However, in other cell types, chromatin can be an integral part of PML-NBs. Most notably, a particular class of PML-NBs exists in tumor cells that maintain their telomeres in the absence of telomerase activity by a process referred to as alternative lengthening of telomeres (ALT) (Neumann and Reddel, 2006). In these cells, specific complexes of PML-NBs and telomeres exist, which are termed ALT-associated PML bodies (APBs) (Neumann and Reddel, 2006; Yeager et al., 1999). Furthermore, in lymphocytes of patients with immunodeficiency, centromeric instability and facial dysmorphy (ICF) syndrome, extremely large PML bodies (~3 μm in diameter) are found that are organized in several protein layers around a heterochromatin core of satellite DNA (Luciani et al., 2006).
PML-NBs seem to be functionally heterogeneous and dynamic structures. They have been associated with a remarkably large number of activities in the nucleus. In general, these are not directly related to the PML or Sp100 protein itself but to proteins that colocalize with PML-NBs. This suggests that the subcompartment formed by PML per se does not provide a specific activity but rather acts like a ‘mobile toolbox’ in the nucleus, in which specific nuclear activities are enriched. Thus, the question is raised how the structure of PML-NBs could provide such an assembly platform for other factors. Although PML-NBs were imaged in numerous fluorescence microscopy studies, the diffraction-limited resolution prevented a detailed elucidation of the PML-NB ultrastructure. The high-resolution electron micrographs, by contrast, lack information on the three-dimensional structure of the PML body and the distribution of its components within this domain. It is noted that the circular arrangement of PML protein observed on EM images would also be compatible with other shapes besides a doughnut or ring. These limitations of previous studies can be addressed by making use of the recent advancements in fluorescence microscopy techniques that yield three-dimensional (3D) images with resolutions significantly better than those obtained by conventional CLSM (Hell, 2007). The first concept to substantially improve the 3D optical resolution, 4Pi microscopy (Hell and Stelzer, 1992; Hell, 2007), has already advanced beyond the stage of an experimental optical set-up. It has been applied successfully for studies of cell membrane delineation, cytoskeleton structures, mitochondria, the Golgi complex, histone H2A.X chromatin structures and nuclear pore complexes (Bewersdorf et al., 2006; Egner et al., 2002; Hüve et al., 2008; Lang et al., 2007b). In 4Pi microscopy, an axial resolution (i.e. the resolution along the z-axis) of 100 nm is achieved by using two opposing high numerical aperture objectives. The coherent superposition of the focused beams enlarges the effective solid angle of the wave front of the focused laser light and/or of the collected fluorescence. This yields a narrowed maximum of the PSF accompanied by axially shifted side lobes. These side lobes can be removed by image processing to obtain images with a five- to sevenfold improved axial resolution compared with conventional confocal microscopy (Gugel et al., 2004).
Here, PML bodies in U2OS and HeLa human cell lines were investigated with respect to their ultrastructure by 4Pi microscopy and correlative electron microscopy and their accessibility for diffusing molecules was assessed. The results demonstrate that during interphase, PML-NBs are spheres defined by a shell of PML and Sp100 proteins in distinct patches. Furthermore, the relative location of SUMO-1, SUMO-2/3, heterochromatin protein 1 (HP1) and telomeres to the PML-Sp100 spherical shell was determined. From the results of the ultrastructure analysis a model is derived that explains how various biological activities can be concentrated in PML-NBs in a dynamic manner.
PML-NBs are spheres with a shell of PML and Sp100 protein in distinct patches
To elucidate the structure of the PML-NBs, we acquired images of immunostained PML protein by 4Pi microscopy and conventional CLSM (Fig. 1A,B, supplementary material Fig. S1-S3). The x-z and x-y sections of the 4Pi images with 1-photon or 2-photon excitation revealed that the PML protein formed a spherical shell of variable diameter in human U2OS and HeLa cells (Fig. 1A,B, supplementary material Fig. S2). With both types of excitation, equivalent images were obtained. Accordingly, 1-photon excitation was used in further experiments, because it provided a better signal intensity and bleaching was reduced. In contrast to the images acquired by 4Pi-microscopy, the conventional CLSM images showed a reduced fluorescence signal in the interior of PML-NBs only for the unusual large PML-NBs with a diameter above 1 μm in the x-y optical section (supplementary material Fig. S3A). The labeling of PML-NBs via autofluorescent mRFP1-PML-III yielded the same distribution of PML protein in a spherical shell as in the immunostaining experiments (supplementary material Fig. S2D, Fig. S3B-D). This confirmed that the antibody staining provided a faithful representation of the PML protein distribution. By two-color labeling of PML and Sp100 protein, it was apparent that Sp100 occupied the same spherical shell as PML protein in both U2OS and HeLa cells (Fig. 1C). Both proteins assembled into distinct patches with no apparent overlap whereas in some parts of the shell, PML and Sp100 colocalized. To ensure that the observed variation in PML protein density was not an artifact of the dual antibody labeling procedure, an analysis of immunostaining to PML only was conducted (supplementary material Fig. S3B,C), as well as a transfection of PML fusion proteins with autofluorescent mRFP1 or GFP domains (supplementary material Fig. S3D,E). With all three methods, the PML protein showed a patchy distribution with intensity variations well above the noise of the fluorescence signal (supplementary material Fig. S3B).
In PML-NBs, the spherical shell of PML and Sp100 protein has a thickness of 50-100 nm independent of the body diameter
The dimensions of the spherical shell formed by PML-Sp100 can be inferred from line scans as shown in Fig. 2A for three PML bodies from the PML-NB x-z images (insets in Fig. 2B). However, the patchwork-like distribution of the two proteins made a systematic quantification of the shell dimensions difficult. Accordingly, an evaluation was conducted by image correlation spectroscopy (ICS). In this type of analysis, the averaged correlation of pixel intensities depending on their radial distance is computed from the images (Görisch et al., 2005). The resulting curve yielded two peaks for a spherical shell (Fig. 2B). The correlation length lc for the first peak centered around zero represents the width of the shell. For the ICS analysis conducted here, it is equivalent to the average of the full-width at half-maximum sections through the shell. The maximum of the second peak in the ICS curve yielded the mean diameter of the sphere, because pixel intensities are also correlated at this separation distance. The results from the ICS analysis are presented in a plot of the shell thickness as given by lc versus the PML-NB diameter for PML and Sp100 protein in U2OS and HeLa cells in Fig. 2C,D. The following results were obtained: (1) No difference between PML (Fig. 2C) and Sp100 protein (Fig. 2D) or between U2OS and HeLa cells (solid vs open squares in Fig. 2C,D) was detected except for the observation that the average PML-NB diameter was somewhat smaller in HeLa cells. (2) For PML protein, a shell thickness of 126±13 nm (n=56, 38 in U2OS, 18 in HeLa) was determined, which was independent of the body diameter between 300 and 1000 nm (Fig. 2C). (3) Sp100 had a shell thickness of lc=130±13 nm (n=22, 11 in U2OS, 11 in HeLa) and again no dependence on the body diameter was detected (Fig. 2D).
In our 4Pi microscopy set-up, the optical resolution, i.e. the capability to distinguish two adjacent objects labeled with the same type of fluorophore, was limited to ~110 nm in the axial direction. Therefore, the true wall thickness of the PML-NBs might be significantly smaller than the width of ~130 nm determined from the image analysis. To address this point, we compared the measured modulation depth of the line profile along the z-axis (Fig. 2E) of the 4Pi raw data (Fig. 2F), with the axial intensity profiles of calculated model images. In 4Pi microscopy, the minima between the main lobe and the side lobes quickly fill up as a structure becomes thicker than 100 nm. For thin objects, the depth of the minima is more sensitive to the shell thickness than the main lobe width. This effect is also exploited in spatially modulated illumination microscopy for measuring object dimensions below the diffraction limit (Failla et al., 2002). Thus, in 4Pi microscopy, the modulation depth of the line profile along the z-axis can be used as a measure of the object dimensions (Egner et al., 2002). Fig. 2E shows calculated axial profiles for model shells with a thickness of 50 nm, 100 nm and 150 nm, respectively, in comparison to the experimentally determined profile. These model structures with varying thickness were convolved computationally with the 4Pi-PSF that was calculated according to the vectorial theory of Richards and Wolf (Richards and Wolf, 1959). The overlay of the theoretical and experimental curves showed good agreement with a wall thickness of 100 nm (Fig. 2E). Because residual aberrations led to an additional decrease of the modulation depth of the 4Pi signal, this should be considered to be an upper estimate. Thus, it is concluded that the average shell thickness was between 50 nm and 100 nm.
These results were further corroborated by electron microscopy studies. PML-NBs on electron micrographs were identified using U2OS cells transfected with autofluorescent GFP-PMLIII. Via correlation with the fluorescence signal detected beforehand on the CLSM images (Fig. 1D), PML-NBs could be identified as roughly spherical structures with a fibrillar composition. Typically, few layers of fibrillar appearance constituted a thin shell of their surface. Measured at five to eight different positions along the periphery, the median of this shell for 12 PML-NBs out of four nuclei was determined, which yielded a mean value of 56±7 nm in thickness. The fibrillar pattern was modulated by globular parts, which appeared attached (supplementary material Fig. S4A,B). Although fibrillar parts could also pervade PML-NBs, their core was typically loosely occupied by convoluted material (Fig. 1D and supplementary material Fig. S4A,B). By contrast, other PML-NBs featured an accumulation of dense matter (supplementary material Fig. S4C,D). Thus, two types of PML-NBs could be distinguished with respect to their inner composition.
The PML-NB subcompartment is accessible for diffusing nuclear factors
To determine the protein mobility within PML-NBs, we performed FRAP (fluorescence recovery after photobleaching) and FCS (fluorescence correlation spectroscopy) experiments (Fig. 3). U2OS cells were co-transfected with plasmids encoding GFP tagged with a nuclear localization sequence (NLS-GFP) and mRFP1-tagged PMLIV. Confocal imaging of fixed and living cells demonstrated that the GFP fluorescence was evenly distributed throughout the nuclear volume. No difference in signal intensity was observed at positions where PML-NBs were located. The NLS-GFP fluorescence in a rectangular region containing a PML-NB was bleached, and images were taken over several seconds. Fluorescence recovery was then quantified within the bleached region containing the PML-NB and a similarly sized region adjacent to the nuclear body. This approach revealed that the dynamics of NLS-GFP fluorescence recovery in PML-NBs and in the nucleoplasm were indistinguishable within the resolution limits of FRAP (Fig. 3). To evaluate the diffusive behavior of NLS-GFP in PML-NBs at higher spatial and temporal resolution, an FCS analysis was conducted (Fig. 3C). The FCS laser was focused into the center of a PML-NB or into the nucleoplasm. Because the confocal volume used for the FCS measurements is very close to, or even smaller than the dimensions of a PML-NB, this approach allowed us to determine the diffusion coefficient and the anomaly parameter of NLS-GFP in nuclear bodies. A threefold reduction of the diffusion coefficient inside the PML-NB was measured. In addition, the anomalous diffusion parameter α decreased from 0.93±0.03 in the nucleoplasm to 0.79±0.02 inside the PML-NBs. Thus, the exchange of NLS-GFP between the nucleoplasm and the PML-NB was somewhat impeded. However, the mobility of a relatively small and inert particle such as GFP was only slowed down by a factor of three, and its diffusion in and out of a PML-NBs occurred on a time scale of seconds.
SUMO-1, SUMO-2/3, HP1-β and telomere repeats occupy distinct locations in PML-NBs with respect to the PML-Sp100 protein shell
In order to determine the location of other PML-NB protein components with respect to PML and Sp100, a series of two-color immunostaining experiments in conjunction with 4Pi microscopy imaging was conducted (Fig. 4, supplementary material Fig. S1B). The location of SUMO modifications was investigated. The SUMO-1 protein was detected in aggregated spots in the PML-Sp100 protein shell (Fig. 4A). In general, for PML protein and SUMO-1, a partial colocalization was apparent from the line profiles. The SUMO-1 patches were less frequent and appeared more aggregated than those formed by PML protein. Interestingly, staining with an antibody that detects SUMO-2 and SUMO-3 also showed a signal in the interior in about 50% of the PML-NBs (Fig. 4B, supplementary material Fig. S5). This indicates a different distribution of SUMO paralogues in PML-NBs, with SUMO-1 being located in the PML-Sp100 shell whereas SUMO-2/3 was also present in the interior. In the other half of the investigated PML-NBs, there was only very weak SUMO-2/3 staining in the interior, and the modification was found in the shell defined by PML-Sp100-SUMO-1, as shown Fig. 4B (merge 2).
In another set of experiments, the structure of PML-NBs complexed with telomeres was investigated in U2OS cells (supplementary material Fig. S6). These so-called APBs are complexes that appear as unusually large PML-NBs on the images. They are specific for the alternative telomere-lengthening mechanism present in this cell line, and are not found in telomerase-positive cell lines such as HeLa (Jegou et al., 2009; Neumann and Reddel, 2006; Yeager et al., 1999). Under the conditions used here, about 5% of the detected telomere signals were in a complex with a PML-NB in U2OS cells, which have a total of ~77 chromosomes corresponding to ~144 telomeres (Jegou et al., 2009). For the 4Pi image analysis, the telomere repeats were stained by FISH with a Cy3-labeled (CCCTAA)3 peptide nucleic acid probe, and PML was visualized by immunostaining. The PML protein formed a distinct shell around the telomere repeat sequence (supplementary material Fig. S6B,C). For the limited number of APBs studied here (n=14), the PML protein shell was between 120 nm and 140 nm as measured for regular PML-NBs.
Finally, the association of PML-NBs with heterochromatin protein 1 (HP1) was investigated, because a function of PML-NBs in heterochromatin formation via its interaction with HP1 has been reported previously (Luciani et al., 2006). In these experiments, the PML protein was visualized by immunostaining, whereas HP1β was detected by transient transfection with an mRFP1-HP1β construct (supplementary material Fig. S7). The 4Pi images clearly revealed that HP1β was located in the interior of PML-NBs. The PML shell again displayed the same apparent average thickness of ~130 nm (n=11) around the HP1 core that was measured for the other PML-NBs studied here.
During mitosis, Sp100 and SUMO-1 showed a dispersed pattern, and both proteins did not colocalize with PML particles, as was apparent on the CLSM images (supplementary material Fig. S8A). The 4Pi images of PML revealed that the spherical structure of the PML body with a distinct shell of PML and Sp100 protein had transformed into an amorphous aggregated conformation of PML multimers in metaphase (supplementary material Fig. S8B).
In the experiments presented here, 4Pi microscopy was used to reveal details of the three-dimensional PML-NB structure that has not been reported in previous studies for any nuclear bodies. Compared with a conventional confocal microscope a five- to sevenfold improvement to about 110 nm axial resolution was achieved. Although our lateral resolution of 150-170 nm was only moderately better than that of a typical CLSM set-up (200-250 nm), a striking improvement of resolvable details in the x-y plane was apparent on the 4Pi images. The reason for this is the elongated shape of the excitation volume in z-direction of normal CLSM. This leads to a corresponding blurring of the image that obscures the resolution of structural details in the x-y plane. The results of the 4Pi imaging of PML-NBs conducted here reveal the localization of PML protein in a spherical shell. Based on an analysis of the modulation depth of the 4Pi images (Fig. 2E,F) and correlative electron microscopy studies (Fig. 1D, supplementary material Fig. S4), we determined the thickness of this shell to be around 50-100 nm. Moreover, the dimensions of this structure were found to be independent of the PML-NB diameter, as well as the specific type of PML-NB, i.e. ‘canonical’ PML-NBs, APBs or PML-NBs containing HP1β. This points to a self-organizing mechanism for the assembly of PML and Sp100 into a spherical shell of distinct thickness that is similar to the mechanism by which liposomes or micelles form from amphiphilic phospholipids (Kostarelos and Miller, 2005). The use of 4Pi microscopy allowed the high-resolution investigation of the two PML-NB components in the same sample. Although Sp100 was present in the same shell as PML, an enrichment of PML and Sp100 in separate regions was also apparent (Fig. 1C, Fig. 4D). The SUMO-1 protein was organized in patches that showed some intrusions and extrusions from the PML shell (Fig. 3A). This indicates that there are areas of PML protein within the shell that are strongly sumoylated, whereas little sumoylation is present in others. PML, Sp100 and SUMO-1 were confined to the outer shell part of PML-NBs. By contrast, SUMO-2/3 was found also in the interior in about 50% of the PML-NBs studied (Fig. 3B). The telomeric repeat DNA in APBs (supplementary material Fig. S6), as well as HP1 (supplementary material Fig. S7) were excluded from the PML-Sp100 shell and clearly confined to the inside of PML-NBs.
If the results obtained here are considered in the context of the large number of previous studies, several factors can be identified that determine the PML-NB structure. The N-terminal RBCC domain of PML protein has self-assembly properties, and deletions or mutations within this domain prevent PML-NB formation (Borden, 2002; Le et al., 1996). This is demonstrated by the formation of spherical structures of similar size to PML-NBs from a bacterially expressed, non-sumoylated RBCC domain (Kentsis et al., 2002). In addition, Sp100 has been reported to self-associate via its HSR domain into homodimers, which is probably also relevant for the interaction network formed between PML and Sp100 protein (Sternsdorf et al., 1999). Importantly, the structures that form via self-association of PML protein in the absence of sumoylation and Sp100 are clearly different from that of a canonical PML-NB. This can be inferred from inspection of PML bodies in mitotic cells where the PML protein is not sumoylated and is not colocalizing with Sp100 (supplementary material Fig. S8). Under these conditions PML protein formed amorphous aggregates with a homogenous PML density throughout the particle. This is consistent with previous reports showing that sumoylation is essential for the formation of normal PML-NBs in mammalian cells (Ishov et al., 1999; Nacerddine et al., 2005; Zhong et al., 2000), and that PML-NBs are disrupted during mitosis as a result of desumoylation (Everett et al., 1999). The results from the 4Pi imaging obtained here indicate that sumoylation of PML is required for the organization of PML and Sp100 in PML-NBs in a distinct spherical shell.
The FRAP and FCS experiments demonstrate that PML-NBs are accessible for a relatively small particle such as GFP (27 kDa, cylindrically shaped with ~3 nm diameter and ~4 nm height) (Fig. 3). From inspection of the 4Pi and EM images, it appears that the PML shell is a filamentous structure, with some variations in thickness. In a recent comprehensive set of FRAP experiments, it was demonstrated that the PML protein splicing variants I-IV and VI, as well as Sp100 exchange between the PML-NB-bound state and the pool of free PML-Sp100 protein in the nucleoplasm within a time scale of seconds to minutes. By contrast, the PMLV splicing variant remained bound in the PML-NB with an average residence time of 48 minutes (Weidtkamp-Peters et al., 2008). These findings suggest that PMLV provides a stable structural scaffold for the other more mobile components of the PML-Sp100 shell. Given the relatively fast exchange of the other splicing variants I-IV and VI, it can be rationalized that the diffusion of GFP in and out of PML-NBs is only moderately slower than its mobility in the nucleoplasm. Nevertheless, the threefold reduction in diffusion rate as observed in the FCS analysis might be sufficient for an increased probability of a protein to become modified. For instance, PML bodies are implicated as sites for both acetylation and phosphorylation of the tumor suppressor p53 (Louria-Hayon et al., 2003; Pearson et al., 2000).
The results on the PML-NB ultrastructure obtained here, together with a number of findings from previous studies, are cast into the model depicted in Fig. 5. In the absence of sumoylation, PML protein forms unspecific aggregates via the N-terminal RBCC domain of PML. Upon sumoylation of both PML and Sp100 protein, a filamentous network of PML-PML, Sp100-Sp100 and PML-Sp100 interactions is established via the SIM found in both proteins. This interaction network organizes into a spherical shell of 50-100 nm in thickness and variable diameter with patches of PML and Sp100. In the resulting PML-NB structure, SUMO-1 modifications are found preferably within the shell or adjacent to it. By contrast the SUMO-2/3 modifications were not restricted to this region, but extended into the interior for a ~50% fraction of the PML-NBs. In this context, it is noteworthy that SUMO-2/3 has the ability to form polymeric chains, because both SUMO-2 and SUMO-3 contain an internal sumoylation site that is missing in SUMO-1 (Matic et al., 2008). Because the other half of the studied bodies displayed only very little SUMO-2/3 signal in the interior, it seems that two different types of PML-NBs exist (compare merge images in Fig. 4B and supplementary material Fig. S5). This view is supported by the electron microscopy analysis, in which PML-NBs with low and high density of the material inside the PML-Sp100 shell were detected at a ratio of 1:1 (Fig. 1D, supplementary material Fig. S4). This observation might reflect the fact that PML-NBs with SUMO-2/3 in the center appear as the more densely stained bodies in the EM images. Thus, the protein composition in the interior of PML-NBs could be controlled by modulating their SUMO-2/3 content. The dynamic nature of this modification is supported by the finding that sumoylation might occur within PML-NBs (Saitoh et al., 2006) and that the presence of poly-SUMO-2/3 chains is a prerequisite for the ubiquitin-dependent degradation of PML (Lallemand-Breitenbach et al., 2008; Tatham et al., 2008). It is noted that such a mechanisms of targeted PML degradation could serve to release the SUMO-interacting proteins into the nucleoplasm so that they would exert specific activities.
Many proteins that associate with PML-NBs are sumoylated or contain a SUMO-interacting motif. This is also relevant for the complexes of PML with telomeres (supplementary material Fig. S6) and HP1 investigated here (supplementary material Fig. S7). The interaction of telomeric repeats with the PML-NBs in APBs is critically dependent on the sumoylation of telomere-binding proteins such as TRF1, TRF2, TIN2 and RAP1 by the MMS21 SUMO ligase. It was shown that APBs did not form in the absence of TRF1 or TRF2 sumoylation (Potts and Yu, 2007). The recruitment of HP1 into PML-NBs is also related to sumoylation processes, because it has been reported that the interaction of HP1 with other proteins can be enhanced by SUMO modifications of the HP1 interaction partner (Seeler et al., 2001; Uchimura et al., 2006). Accordingly, a number of models for the PML-NB structure were proposed previously that are based on a network of SUMO-SIM interactions (Lin et al., 2006; Shen et al., 2006), albeit without the structural details on the organization of PML-NBs provided from our analysis. The clear discrimination between an inner part and an outer shell of PML-NBs obtained in this study supports the view that PML-NBs can assemble around a distinct core structure such as telomeric DNA (supplementary material Fig. S6), as shown recently in live-cell-imaging experiments (Jegou et al., 2009). The presence of a chromatin core has also been observed for the giant PML-NBs in cells from patients suffering from ICF syndrome (Luciani et al., 2006), as well as the assembly of PML-NBs around HSV-1 viral nucleoprotein complexes (Everett and Murray, 2005). Because HP1 was located in the inner part of PML-NBs (Fig. S7), it appears that the presence of HP1 could increase the propensity of a genomic locus to serve as the nucleation site for PML-NB assembly. In agreement with this view, ICF-associated PML-NBs or APBs form at heterochromatic loci such as telomeres or microsatellite DNA enriched in HP1 (Luciani et al., 2006; Yeager et al., 1999). This might contribute to the creation of a distinct nuclear subcompartment to confine associated activities to these sites.
We conclude that the ultrastructure of PML-NBs revealed here reflects the self-organizing properties of PML and Sp100 proteins in the environment of the nucleus, which are steered by sumoylation and the interaction with SIMs present in both proteins. In this context, it is also noteworthy that the SUMO modification of Sp100 is significantly decreased in the absence of PML (Everett et al., 2006). Thus, the PML-Sp100-SUMO interaction network could be established and maintained in PML-NBs in a feedback-loop manner in the presence of desumoylation activities outside this nuclear subcompartment. Such a mechanism would be further enhanced by the putative SUMO ligase activity of PML (Quimby et al., 2006; Shen et al., 2006). The resulting PML-Sp100 shell structure appears conceptually similar to the organization of a liposome. It is dynamic and allows for an exchange of proteins in and out of the PML-Sp100 shell on the second-to-minute time scale, as inferred from our studies of GFP mobility. Via a protein interaction network that makes use of SUMO-mediated binding to the SIMs of the various ‘cargo’ proteins, specific biological activities can be concentrated in the PML-NB subcompartment. This process could serve to promote modifications of nuclear components that require a high concentration of these factors not available in their freely mobile state in the nucleoplasm. Alternatively, PML-NBs could represent sites of storage or confinement for certain nuclear factors that would exert their biological function only upon release from the PML-NB by removal of SUMO residues.
Materials and Methods
Cell culture and sample preparation
Human cell lines HeLa (REF) and U2OS (HTB-96) were grown in DMEM (Invitrogen) containing 10% FCS (PAA, Austria). Immunostaining and PNA FISH were conducted as described previously (Jegou et al., 2009). The primary antibodies against PML and SUMO-1 from Santa Cruz Biotechnology and against Sp100 from Chemicon (Millipore) were used. The anti-mouse Alexa Fluor 568 and anti-mouse/anti-rabbit Alexa Fluor 647 secondary antibody were purchased from Invitrogen and the anti-mouse and anti-rabbit Atto 647N were from ATTO-TEC (Siegen, Germany). Cells for 4Pi microscopy were grown on coverslips ~150 μm thick. After staining, the samples were embedded in a solution containing 97% (v/v) TDE (2,2′-thiodiethanol, Sigma) and 3% (v/v) phosphate buffered saline (PBS) to yield a refractive index of 1.515 (Staudt et al., 2007). This minimizes spherical aberration and minimizes the side lobes. To avoid structural changes, the buffer was replaced with the embedding medium via a dilution series (step-wise 10, 20, 40, 60, 80 and three times 97% TDE was applied for 10 minutes each). This coverslip was mounted on a second coverslip (with a quarter mirror for the phase setting of the 4Pi set-up) of equal thickness and sealed with nail polish. For standard CLSM, the coverslips were dipped briefly into H2O, incubated for 1 minute in ethanol, then air-dried and finally mounted in Vectashield containing DAPI (Vector Laboratories). For analysis of autofluorescent mRFP1-PML-III and GFP-PML-III constructs, cells were transfected with Effectene (Qiagen, Hilden, Germany) incubated for about 17 hours with the transfection reagent before fixation, as described previously (Jegou et al., 2009). Complexes of PML and HP1β were visualized by transient transfection with an mRFP1-HP1β construct (Müller et al., 2009).
4Pi microscopy imaging was conducted with a custom-made module attached to a conventional confocal microscope (TCS SP2, Leica Microsystems, Mannheim) as described in detail elsewhere (Gugel et al., 2004). The 4Pi module was equipped with two high numerical aperture oil-immersion objectives (HCX PL APO CS 100× 1.46 NA Oil, Leica Microsystems, Germany). These yield a narrow central maximum of an axial full-width at half-maximum (FWHM) of ~100 nm and low side maxima. 4Pi imaging was conducted with an Ar-Kr-Laser (one-photon excitation) or a Ti:Sapphire laser (two-photon excitation; Mai Tai, Newport-Spectra-Physics, Mountain View, CA). As described previously (Lang et al., 2007a), 4Pi microscopy with one-photon excitation yielded a higher signal intensity compared with 2-photon excitation at the cost of higher side maxima (supplementary material Fig. S2). Detection of the fluorescence emission was with avalanche photodiodes (PerkinElmer Optoelectronics, Fremont, CA). The 3D data stacks were recorded with a voxel size of 37×28×55 nm in the x-z-y direction. After image acquisition, the 4Pi raw data were processed to remove the side maxima. To this end, the 4Pi raw data were smoothed and a five-point deconvolution was applied (Nagorni and Hell, 2001). Subsequently, an offset of 10% was subtracted. No further deconvolution of the image was conducted. Standard confocal microscopy was performed with a Leica TCS SP2. Z-axis picture stacks with 0.3-μm spacing were acquired and were displayed as maximum intensity projection in the overview images. FRAP experiments were carried out on a Zeiss LSM 510Meta confocal microscope (Carl Zeiss, Jena, Germany) as described (Schmiedeberg et al., 2004). Five to ten images were taken before the bleach pulse and 50-200 images after bleaching of ‘regions of interest’. FCS measurements were performed at 37°C on a LSM 510 Meta/ConfoCor2 system using a C-Apochromat infinity-corrected 40× 1.2 NA water objective (Carl Zeiss, Jena, Germany) as described in detail previously (Schmiedeberg et al., 2004; Weidtkamp-Peters et al., 2008; Weidtkamp-Peters et al., 2009). For the measurements, 10×30 time-series of 10 seconds each were recorded with a time resolution of 1 μsecond and then superimposed for fitting to an anomalous diffusion model in three dimensions with triplet function using the Origin Software. The diffusion coefficients and anomaly parameters were extracted from fitted curves as previously described (Weidtkamp-Peters et al., 2009). FRAP and FCS studies were conducted with the GFP-PML IV splicing variant.
Correlative electron microscopy
Cells transfected with GFP-tagged PML and grown on gridded coverslips (Cellocate, Eppendorf, Germany) were processed for correlative fluorescence and electron microscopy, as previously described (Richter et al., 2005). Briefly, cells were fixed in 4% formaldehyde, 1% glutaraldehyde (EM-grade, Sigma) in 100 mM sodium phosphate buffer, rinsed with buffer and mounted with Vectashield (Vector laboratories) for observation by confocal laser scanning microscopy (TCS-SP II, Leica Microsystems, Germany). CLSM data of cell nuclei of interest comprised 3D-image stacks of GFP-PML at 74 nm pixel size using a 100× 1.4 NA oil objective, and a differential interference contrast image to assist relocation after preparation for EM. Following CLSM investigation, the coverslips were post-fixed in 1% buffered OsO4, dehydrated in graded steps of ethanol and embedded in epoxy resin (Polysciences, Eppelheim, Germany). The coverslips were removed under liquid nitrogen, depicting the negative imprint of the grid on the remaining block faces. Ultrathin sections at nominal thickness of 70 nm were prepared from the grid-region of interest, stained in aqueous lead citrate and uranyl acetate and observed in a Philips 410 transmission electron microscope.
We are grateful to David Baddeley, Malte Wachsmuth and Joel Beaudoin for help and discussions. The work was funded by the Deutsche Forschungsgemeinschaft (Ri 1283/5-3) in the SPP 1128 program (K.R.) and within the project ‘Neue 4Pi-Kontraste zur Abbildung lebender Zellen’ of the Landesstiftung Baden-Württemberg (S.W.H.).