Abstract
Pioneer transcription factors have the ability to access DNA in compacted chromatin1. Multiple transcription factors can bind together to a regulatory element in a cooperative way, and cooperation between the pioneer transcription factors OCT4 (also known as POU5F1) and SOX2 is important for pluripotency and reprogramming2–4. However, the molecular mechanisms by which pioneer transcription factors function and cooperate on chromatin remain unclear. Here we present cryo-electron microscopy structures of human OCT4 bound to a nucleosome containing human LIN28B or nMATN1 DNA sequences, both of which bear multiple binding sites for OCT4. Our structural and biochemistry data reveal that binding of OCT4 induces changes to the nucleosome structure, repositions the nucleosomal DNA and facilitates cooperative binding of additional OCT4 and of SOX2 to their internal binding sites. The flexible activation domain of OCT4 contacts the N-terminal tail of histone H4, altering its conformation and thus promoting chromatin decompaction. Moreover, the DNA-binding domain of OCT4 engages with the N-terminal tail of histone H3, and post-translational modifications at H3K27 modulate DNA positioning and affect transcription factor cooperativity. Thus, our findings suggest that the epigenetic landscape could regulate OCT4 activity to ensure proper cell programming.
Subject terms: Cryoelectron microscopy, Nucleosomes, Transcriptional regulatory elements
Binding of the human pioneer transcription factor OCT4 to nucleosomes containing endogenous DNA sequences causes changes to the nucleosome structure and facilitates the cooperative assembly of multiple pioneer transcription factors, a property that can be affected by histone modifications.
Main
DNA-binding transcription factors (TFs) target distinct DNA sequences at gene regulatory regions, thus ensuring specificity in transcription machinery assembly1,5. DNA packaging into nucleosomes can hinder TF binding to target sequences6, but a small set of so-called pioneer TFs can access DNA even within compacted chromatin3,7–10. Once bound to their target sites, pioneer TFs can facilitate the recruitment of other TFs by creating accessible chromatin, a property that underlies their function as master regulators in embryo development, cell differentiation and reprogramming. In fact, overexpression of four pioneer TFs — OCT4, SOX2, KLF4 and MYC — promotes the reprogramming of cells to pluripotency2, with OCT4 expression being necessary and sufficient to reprogram cells4,11. In vitro SOX2, KLF4 and MYC bind to nucleosomes more efficiently in the presence of OCT4 (ref. 8), and cooperativity between OCT4 and SOX2 is critical for early development and reprogramming12–18, but the molecular mechanisms involved remain unclear.
OCT4 has two DNA-binding domains: OCT4-POUS and OCT4-POUHD. Previous X-ray structures showed the two domains wrapping around naked DNA, but such a binding mode would be incompatible with the nucleosome architecture19,20. In recent cryo-electron microscopy (cryo-EM) work21, OCT4-POUS and the DNA-binding domain of SOX2 were seen unwrapping a nucleosome containing binding sites for those TFs inserted into the DNA positioning sequence 601 (ref. 22). The inserts were placed to promote optimal binding and stability of the complex, but the 601 sequence is known to suppress the nucleosome dynamics that are typical of biologically relevant sequences22. In recent efforts to capture OCT4 bound to a nucleosome with an endogenous DNA sequence, the density for OCT4 could not be observed23,24. Hence, a structure of OCT4 in complex with a nucleosome containing a physiologically relevant DNA sequence remained elusive, limiting our mechanistic understanding of pioneer TF function. For instance, although OCT4 and other TFs bind to nucleosomes, it remains unclear whether they interact with histones and whether epigenetic marks would affect that interaction. Previous crosslinking and mass spectrometry analyses of the reconstituted OCT4–nucleosome complex with endogenous DNA have shown that OCT4 binds near to the N-terminal tail of histone H3 (ref. 24), which would require proper positioning of the DNA-binding site on the nucleosome. Moreover, chromatin occupancy by OCT4 correlates with histone marks found in enhancers, such as H3K27ac and H3K4me1, but silent marks such as H3K27me3 are also found at OCT4-binding sites25–30; it remains to be determined whether and how those modifications regulate OCT4 binding.
To address these gaps, we present cryo-EM structures of human OCT4 bound to nucleosomes containing DNA sequences from human LIN28B or near the matrilin 1 gene (nMATN1) loci, along with biochemistry assays. The LIN28B sequence has three binding sites for OCT4, as well as binding sites for SOX2, KLF4 and MYC8, whereas nMATN1 has multiple OCT4-binding sites. Both sequences are thus an ideal platform to study cooperative assembly of multiple pioneer TFs.
OCT4 binding to the LIN28B nucleosome
To investigate the mechanism for cooperativity between the pioneer TFs OCT4 and SOX2, we assembled a complex containing full-length human OCT4 and SOX2 and a nucleosome with DNA from the human LIN28B locus31–33. This DNA fragment contains three binding sites for OCT4 (OBS1–3) and one for SOX2 (ref. 8). Using native gel electrophoresis assays, we observed an association of OCT4 and SOX2 with nucleosomes assembled with LIN28B DNA fragments that were 162-bp or 182-bp long (Extended Data Fig. 1a). However, using cryo-EM analyses, we could only visualize the proteins bound to the 182-bp nucleosome, which indicates that the complex on the nucleosome with shorter DNA is less stable24. Hence, for the remainder of this work, we exclusively used the 182-bp nucleosome.
The initial cryo-EM reconstructions showed a density bound to the linker DNA (Extended Data Table 1 and Extended Data Fig. 1b–h), but the resolution was limited because of flexibility of the complex. To improve the resolution, we used focused classification followed by local search refinements and obtained maps with resolutions of 2.8 Å in the nucleosome portion (Extended Data Fig. 1g–i) and of 3.9 Å for a 30-kDa region of OCT4 bound to linker DNA (Extended Data Fig. 2a–g). We did not observe clear density for SOX2, which suggests that it might have dissociated during sample preparation. The two maps had sufficient overlapping densities to allow assembly of a composite map and model (Fig. 1a, Extended Data Table 1 and Extended Data Fig. 2h). In the structure, OCT4 is bound to the linker DNA near the nucleosome entry–exit site (Fig. 1a and Extended Data Fig. 2h), in agreement with previous crosslinking mapping of reconstituted complexes24. Of note, the DNA bases are well resolved along the nucleosome-wrapped region, indicating minimal movement of the LIN28B sequence in complex with OCT4 (Extended Data Fig. 1i). The high resolution of the nucleosomal DNA allowed us to precisely position the sequence, with OBS1 placed at the exact location of the OCT4 density (Fig. 1a and Extended Data Figs. 1i and 2i).
Extended Data Table 1.
To determine whether OCT4 stabilizes DNA positioning on the LIN28B nucleosome, we determined a cryo-EM structure of that same nucleosome in the absence of any TFs (Extended Data Table 1). This structure had an overall resolution of 3.1 Å, similar to the OCT4-bound nucleosome, but the DNA bases were not well resolved and hence the DNA position could not be determined (Extended Data Fig. 3a–f). We also observed that in some particle classes, the linker DNA protrudes from both sides of the histone octamer (Extended Data Fig. 3g), whereas in the OCT4-bound structure, it protrudes from only one side. Together, these observations indicate that the LIN28B DNA could adopt several positions on the free nucleosome (Extended Data Fig. 3g), in contrast to its well-defined positioning in the OCT4-bound nucleosome (Fig. 1a). These findings are consistent with in vivo data showing that the nucleosome at the LIN28B locus is ‘fuzzy’ and occupies approximately 200 bp (ref. 34). Thus, the naturally occurring LIN28B sequence is able to move along the histone octamer, transiently exposing OBS1. Once OCT4 binds to OBS1, it traps the DNA in that position and stabilizes the otherwise flexible linker DNA into a more defined conformation (Fig. 1b and Extended Data Fig. 4a). Of note, we observed that hexasomes are threefold more abundant in OCT4-bound samples than in the free LIN28B nucleosomes (Extended Data Figs. 1g and 3f).
In the structure, both DNA-binding domains of OCT4 engage with the LIN28B nucleosome: OCT4-POUS is bound to the linker DNA, close to the nucleosome dyad, whereas OCT4-POUHD is located distally from the nucleosome (Fig. 1a and Extended Data Fig. 2h). These observations are consistent with the requirement for both OCT4 DNA-binding domains to efficiently bind to chromatin in vivo21 (Fig. 1a,c). The OCT4 interactions with DNA in our structure are overall similar to those observed in the crystal structure of OCT4 bound to naked DNA19, but we observed that OCT4-POUHD introduces a kink in the linker DNA, due to arginine residues widening the DNA major groove (Fig. 1c and Extended Data Figs. 2g and 4b,c); such DNA distortion could disrupt local chromatin organization and affect binding of other proteins. Overall, the OCT4–DNA interactions in our structure differ considerably from those seen in the cryo-EM structure of OCT4 bound to a 601-based nucleosome, in which only OCT4-POUS was observed to interact with the nucleosome21.
OCT4 modifies H4 tail conformation
Having shown that OCT4 binding stabilizes the positioning of nucleosomal DNA, we examined whether it induced other changes to the nucleosome structure. We observed in our cryo-EM data that the H4 N-terminal tail on the OCT4 proximal side of the nucleosome adopts multiple conformations, whereas the H4 tail on the opposite side is predominately found in the canonical conformation, following the DNA path at SHL2 (refs. 35,36) (Extended Data Fig. 4d). Further image classification revealed two major conformations for the H4 tail on the OCT4 proximal side of the nucleosome: the first one resembles the canonical conformation, whereas in the second one, the H4 tail is rotated 90° towards SHL1 and an additional density can be seen interacting with the H4 tail and α2 helix (Fig. 2a and Extended Data Fig. 4d–f). This density was not observed on the LIN28B nucleosome or on the OCT4 distal side of the OCT4-bound nucleosome, and we hypothesized that it could originate from the OCT4 activation domain, which consists of flexible N-terminal and C-terminal regions. The density alters the conformation of Asp24 at the beginning of the H4 tail, which in turn changes the conformation of the whole H4 tail (Fig. 2a), moving residues that are essential for chromatin compaction by more than 30 Å and potentially disrupting interactions between nucleosomes.
These observations suggest that OCT4 binding affects the interactions between two nucleosomes. To examine this effect further, we induced nucleosome compaction with Mg2+ (refs. 37,38) and found that the presence of OCT4 substantially reduced association between mononucleosomes as assessed by native gel electrophoresis (Fig. 2b and Extended Data Fig. 5a). We also assembled chromatin arrays using a longer 1,022-bp DNA fragment from the LIN28B locus and examined their compaction with Mg2+ by negative-stain EM imaging. We found that the nucleosome arrays are more open in the presence of OCT4 (Fig. 2c and Extended Data Fig. 5b,c).
Finally, we tested the roles of the N-terminal and C-terminal flexible regions of OCT4 on chromatin decompaction by deleting them individually. Neither deletion reduced the interaction of OCT4 with the LIN28B nucleosome (Extended Data Fig. 5d). However, OCT4 lacking the N-terminal region lost the ability to reduce nucleosome compaction and internucleosome interactions, whereas deletion of the C-terminal tail did not affect those properties (Fig. 2b,c and Extended Data Fig. 5e). Together, our structural and biochemical data suggest that the N-terminal region of OCT4 remodels the H4 tail and contributes to chromatin decompaction.
H3K27ac increases OCT4 cooperativity
In our structure of the OCT4-bound nucleosome, both the OCT4-binding sites OBS2 and OBS3 have partial internal motifs exposed, which would allow binding of OCT4-POUHD to OBS2 and OCT4-POUS to OBS3 (Fig. 3a). Binding to partial DNA motifs has been previously proposed8 and our data suggest that DNA positioning induced by binding of OCT4 to OBS1 facilitates binding of additional OCT4 molecules to their internal sites.
To test this hypothesis, we mutated each of the OCT4-binding sites in the LIN28B sequence and examined binding of OCT4 to nucleosomes by native gel electrophoresis. This setup allows us to distinguish nucleosomes with one or more OCT4 bound (Extended Data Fig. 5f). With the wild-type LIN28B nucleosome, we detected strong binding of one OCT4 but also a second and weaker binding of the third OCT4 (Extended Data Fig. 5f,g). Mutation of either OBS2 or OBS3 did not affect the formation of a complex with one OCT4 bound, indicating that the first OCT4 binds to OBS1 as in the wild-type LIN28B nucleosome, whereas a second OCT4 binds to either OBS2 or OBS3 (Extended Data Fig. 5h,i). By contrast, when we mutated OBS1 to generate the LIN28B-1M nucleosome, OCT4 binding to OBS2/3 was considerably reduced compared with the wild-type LIN28B nucleosome (Fig. 3b). Thus, OCT4 binding to OBS2/3 is stimulated when a first OCT4 is bound to OBS1, which is in agreement with our structural data showing that binding of OCT4 to OBS1 stabilizes nucleosomal DNA and exposes partial motifs in internal OBS2/3 sites.
We turned our attention back to OCT4 DNA-binding domains bound to OBS1 and observed interactions between OCT4-POUS and histones H3 and H2A. The tip of helix 1 (residues 159–163) contacts the C-terminal tail of histone H2A and the N-terminal tail of histone H3; the latter is also contacted by small helix 5 (residues 213–222) (Fig. 3c and Extended Data Fig. 5j). The dipole moment of helix 1 and negatively charged helix 5 together form an acidic patch on OCT4 that faces the nucleosomal dyad and interacts with positively charged histone tails there, mediating additional interaction between the OCT4 DNA-binding domain and the nucleosome (Fig. 3d).
In our structure of the OCT4-bound nucleosome, histone H3K27 is in close proximity to the acidic patch of OCT4, specifically to the tip of helix 1, suggesting a potential electrostatic interaction between positively charged H3K27 and the negative dipole moment of helix 1 (Fig. 3c,d). This observation prompted us to examine whether H3K27 modifications would affect OCT4 binding to the nucleosome. H3K27ac is an active mark associated with enhancers that was found to colocalize with OCT4 on chromatin26–28. Acetylation of H3K27 would neutralize the positive charge of the Lys residue and would be expected to affect the interaction between the histone H3 tail and the OCT4 acidic patch. To test this possibility, we assembled nucleosomes with H3K27ac-modified histone H3 and examined binding of OCT4 by native gel electrophoresis (Fig. 3e and Extended Data Fig. 6a). The H3K27ac modification showed only a small effect on binding of the first OCT4, which directly interacts with the H3K27 residue, indicating that this interaction is not required for stability of the OCT4–nucleosome complex (Fig. 3e). However, binding of the second and third OCT4 was increased with H3K27ac nucleosomes compared with unmodified nucleosomes (Fig. 3e). Deacetylation of H3K27ac abrogated the increased binding of the second and third OCT4, resulting in levels comparable with the unmodified nucleosome (Extended Data Fig. 6b,c). Thus, cooperative OCT4 binding to OBS2/3 is increased by H3K27ac.
This finding prompted us to examine whether the interactions of OCT4 with histone H3 contribute to DNA positioning by OCT4 in the LIN28B nucleosome. We first developed an assay to directly assess DNA positioning, taking advantage of an endogenous Mnl I restriction site between OBS1 and OBS2 (Fig. 1b); this site should be accessible to Mnl I when the LIN28B DNA is positioned as in our OCT4-bound nucleosome structure (Fig. 3c). Using LIN28B nucleosomes, we only observed partial digestion by Mnl I (Fig. 3f and Extended Data Fig. 6d), which is consistent with LIN28B DNA adopting multiple conformations on the nucleosome. By contrast, the Mnl I restriction site was fully accessible in OCT4-bound nucleosomes, indicating that OCT4 binding stabilizes the nucleosomal DNA in a conformation in which the Mnl I site is exposed (Fig. 3f and Extended Data Fig. 6d). H3K27ac did not alter the sensitivity of nucleosomes alone to Mnl I digestion (Fig. 3f and Extended Data Fig. 6d); however, OCT4-bound H3K27ac nucleosomes showed higher protection from Mnl I digestion than OCT4-bound unmodified nucleosomes (Fig. 3f and Extended Data Fig. 6d). These results suggest that OCT4 induces an inward movement of the DNA on the H3K27ac nucleosome compared with the unmodified nucleosome. Such movement might be induced by the loss of electrostatic interaction between the H3K27 residue and the OCT4 acidic patch, and it would probably have limited range, until OCT4 gets close to the nucleosome; further DNA movement would require DNA unwrapping or OCT4 dissociation. The DNA movement would increase exposure of OBS2/3, leading to higher binding of second and third OCT4 (Fig. 3a). To test this hypothesis, we digested OCT4-bound nucleosomes with MNase and sequenced the protected DNA (Extended Data Fig. 6e). We found that 70% of OCT4-bound unmodified nucleosomes were in a defined position, in agreement with our structural and biochemical data (Fig. 3g). By contrast, OCT4-bound H3K27ac nucleosomes were less well positioned, with a major species (20%) shifted by 1 bp inwards (Fig. 3g and Extended Data Fig. 6f).
To mimic the changes in the DNA positioning caused by OCT4 on H3K27ac nucleosomes, we moved OBS2/3 by 1 bp (LIN28B-OSO+1) or 2 bp (LIN28B-OSO+2) relative to OBS1. Modelling revealed that inward sliding of DNA for 1 bp would expose the binding site for OCT4-POUS at both OBS2 and OBS3, thus changing the interaction at OBS2 from OCT4-POUHD to OCT4-POUS (Extended Data Fig. 6g). We used unmodified nucleosomes bearing those constructs to test OCT4 binding and observed increased binding to OBS2/3 with the LIN28B-OSO+1 construct compared with LIN28B (Extended Data Fig. 6h). The LIN28B-OSO+2 construct showed binding of OCT4 comparable with LIN28B (Extended Data Fig. 6i). These data show that OCT4 binds to LIN28B-OSO+1 in a manner similar to its binding to the H3K27ac LIN28B nucleosome and support our conclusion that DNA movement of approximately 1 bp on OCT4-bound H3K27ac nucleosomes increases binding to internal sites. To test this model further, we examined the binding of OCT4 to H3K27ac LIN28B-OSO+1 nucleosomes, which would mimic a +2 bp movement (Extended Data Fig. 6j), and observed that acetylation of H3K27 in the LIN28B-OSO+1 nucleosome abrogated the increased binding of OCT4 to LIN28B-OSO+1 relative to the LIN28B nucleosome.
H3K27 methylation is a silent mark that would increase the bulkiness of the Lys residue, which could affect the interaction between the histone H3 tail and the OCT4 acidic patch. To test whether H3K27 methylation modulates OCT4 binding, we assembled nucleosomes with H3K27me3 and examined binding of OCT4 by native gel electrophoresis. We found that H3K27me3 did not significantly change OCT4 binding (Extended Data Fig. 7a). Consistent with that observation, we did not observe change in DNA positioning of OCT4-bound H3K27me3 nucleosomes by Mnl I digestion and MNase sequencing compared with unmodified nucleosomes (Extended Data Figs. 6e and 7b,c).
H3K27ac enhances OCT4–SOX2 cooperativity
In the LIN28B sequence, the SOX2-binding site is located between OBS2 and OBS3, forming a composite site with the latter. In our OCT4-bound nucleosome structure, the SOX2-binding site faces outwards, and modelling showed that SOX2 could bind to that site, with minor clashes with H2A (Extended Data Fig. 7d). Thus, OCT4 binding to the LIN28B nucleosome should facilitate SOX2 binding, by stabilizing the exposure of its binding site. We tested this hypothesis using native gel electrophoresis and observed that SOX2 could bind more efficiently to the OCT4-bound LIN28B nucleosome than to the LIN28B nucleosome alone (Extended Data Fig. 7e–g).
The inward DNA movement caused by OCT4 binding to the H3K27ac nucleosome would further increase exposure of the SOX2 site and alleviate the small clash between SOX2 and histone H2A (Extended Data Fig. 7d). Indeed, we found that SOX2 was able to bind better to OCT4-bound H3K27ac nucleosomes than to OCT4-bound unmodified nucleosomes (Fig. 4a). To validate our finding, we moved the SOX2-binding site to be 5 bp closer to OBS2, which would reduce its exposure in OCT4-bound nucleosomes but not in unbound nucleosomes that can slide. We observed that this shifting of the SOX2-binding site strongly reduced binding of SOX2 to OCT4-bound H3K27ac nucleosomes, indicating that OCT4 binding to OBS1 determines DNA positioning and OCT4–SOX2 cooperativity (Fig. 4b). Of note, SOX2 binding to free H3K27ac nucleosomes was not affected when its binding site was shifted by 5 bp, showing that DNA slides on free nucleosome, transiently exposing the SOX2-binding site and allowing its binding. By contrast, when OCT4 is bound to the H3K27ac nucleosomes, DNA is positioned and cooperative binding with SOX2 is determined by the distance between OBS1 and the SOX2-binding site.
OCT4 binding to the nMATN1 nucleosome
To investigate whether our findings with the LIN28B nucleosome apply to other human DNA sequences, we assembled nucleosomes with a 186-bp-long DNA from the regulatory region nMATN1 (ref. 3) (Extended Data Fig. 8a), which contains multiple OCT4-binding motifs. The initial cryo-EM reconstructions of the nMATN1 nucleosome in complex with OCT4 showed a density near the linker DNA, similar to the density of OCT4 bound to LIN28B DNA (Extended Data Fig. 8b–g and Supplementary Table 1). Focused classification and refinements improved the resolution to 2.3 Å in the nucleosome portion (Extended Data Fig. 8c–f) and to 8.1 Å for an approximately 20-kDa OCT4 region bound to the linker DNA (Extended Data Fig. 9a–d). We performed MNase sequencing to determine the position of the nMATN1 DNA on the OCT4-bound nucleosome and combined that information with the cryo-EM map to build a model for OCT4 bound to the nMATN1 nucleosome (Extended Data Fig. 9d–g).
Our structural and MNase sequencing data revealed that, despite the presence of multiple OCT4 motifs in the nMATN1 DNA, OCT4 predominantly binds to one binding site in the linker DNA, near the nucleosome entry–exit site (mOBS1) (Fig. 5a and Extended Data Fig. 9h), a position overall similar to that in the LIN28B nucleosome structure. Both DNA-binding domains of OCT4 engage the nMATN1 nucleosome; whereas OCT4-POUHD is bound close to the nucleosome dyad, OCT4-POUS is located distally from the nucleosome (Fig. 5a,b). This arrangement differs from that with the LIN28B nucleosome, in which OCT4-POUS was bound to the linker DNA, close to the nucleosome dyad, whereas OCT4-POUHD was located distally from the nucleosome (Fig. 1a and Extended Data Fig. 2h). Nevertheless, despite its distal position relative to the nMATN1 nucleosome, OCT4-POUS interacts with the histone H3 tail via a smaller acidic patch of OCT4 formed by the side chains of helices 4 and 5 (Fig. 5a,b and Extended Data Fig. 9i). Of note, the H3 tail from the entry–exit site opposite to the OCT4-binding side interacts with OCT4 (Fig. 5a,b and Extended Data Fig. 9i), in contrast to the LIN28B nucleosome.
OCT4 interaction with the H3 tail in the nMATN1 nucleosome prompted us to test whether H3K27 modifications also modulate histone cooperativity on this human sequence, as it does for the LIN28B sequence. We found that both H3K27ac and H3K27me3 modifications increased binding of the second and especially the third OCT4 (Fig. 5c,d).
Together, our biochemical and structural data reveal the mechanism for cooperativity of OCT4 and SOX2. OCT4 binding to OBS1 on LIN28B or nMATN1 nucleosomes stabilizes the positioning of nucleosomal DNA, to expose internal TF-binding sites, thereby facilitating binding of additional OCT4 and of SOX2. The internal binding sites are distant from OBS1 (Fig 3a and Extended Data Fig. 7d), pointing to an allosteric mechanism for TF cooperative binding, mediated by DNA positioning on the nucleosome. Moreover, H3K27 modifications can modulate cooperativity of OCT4 and downstream factors, such as other OCT4 molecules or SOX2, by altering the interaction between the OCT4 acidic patch and the H3 tail, which in turn affects the positioning of the nucleosomal DNA and exposure of internal binding sites for downstream factors.
Discussion
Our cryo-EM structures captured OCT4 bound to nucleosomes assembled with endogenous LIN28B and nMATN1 DNA and unveiled previously unknown OCT4 interactions with histones. A previous structure of OCT4 bound to engineered nucleosomes did not reveal interactions with histones21, but those nucleosomes contained the strong 601 positioning sequence39 with the OCT4-binding site inserted in a position that could have prevented interactions with H3 and H2A tails. Our data indicate that proper positioning of the DNA-binding site for TFs on the nucleosome is required for specific interactions and for the formation of a stable OCT4–nucleosome complex. Our findings support a model in which initial binding of OCT4 to a partially exposed motif on the nucleosomal DNA leads to transient complexes that undergo DNA sliding to achieve stable OCT4 binding via its two DNA-binding domains (Extended Data Fig. 9j,k). This model is consistent with recent in vivo data showing that pioneer TFs bind preferentially next to nucleosomes40.
Our findings show that a pioneer TF can directly alter the chromatin environment by stabilizing DNA on the nucleosome. DNA sliding on the nucleosome can occur spontaneously or be facilitated by chromatin remodelling complexes. In fact, OCT4 and other TFs can recruit chromatin remodelling complexes41–45, which might facilitate nucleosome sliding to properly position DNA-binding motifs. The chromatin remodeller BRG1 is required for OCT4 binding to a subset of gene regulatory elements in cells13, and inhibition of the catalytic activity of BRG1 reduces the amount of already bound OCT4 at these elements in vivo25, implying that chromatin remodellers support OCT4 by properly positioning nucleosomes at those specific locations. Our findings suggest that at other sites, OCT4 binding itself could directly position nucleosomal DNA and alter the accessibility of sites for downstream factors.
Of note, we observed that OCT4 alters the conformation of the N-terminal tail of histone H4, affecting internucleosome interactions and promoting chromatin decompaction. Recently, the SOX11 DNA-binding domain was proposed to affect the H4 tail position46, but such mode of H4 regulation would limit TF binding to restricted regions on the nucleosome, where the DNA-binding domain would directly clash with the H4 tail. By contrast, our data reveal that the interaction between OCT4 and the histone H4 tail involves the disordered activation domain of OCT4 and takes place 70 Å away from the site where its DNA-binding domains interact with the nucleosome, indicating that interaction with the H4 tail does not depend on the location of the OCT4-binding site. In agreement with our findings on OCT4, recent work has suggested that the activation domain of FOXA1 binds to histones and that this is required for FOXA1 to open chromatin, although the mechanism remains elusive47.
Perhaps our most consequential finding is that TF binding and cooperativity can be regulated by histone modifications. Of note, our data show that H3K27 modifications did not affect the binding of the first OCT4 to the LIN28B or nMATN1 nucleosome, but it altered the cooperative binding of additional OCT4 or of SOX2 to nucleosomal internal sites. These findings are consistent with previous in vivo data correlating OCT4-binding sites with H3K27ac26,27,29. However, positive correlation with histone marks has not been observed for FOXA2 and GATA4 (ref. 27), suggesting that not all TFs might be affected by epigenetic marks. In conclusion, our findings suggest that the pre-existing epigenetic landscape could tune pioneer TF activity.
Methods
Protein expression, mutagenesis and purification
Xenopus laevis histones for nucleosome assembly were overexpressed in the Escherichia coli BL21(DE3) pLysS strain and purified from inclusion body as previously described48.
The cells were grown in LB medium at 37 °C and induced with 1 mM IPTG when OD600 reached 0.6. After 3 h of expression, the cells were pelleted down, resuspended in lysis buffer (50 mM Tris-HCl (pH 7.5), 150 mM NaCl, 1 mM EDTA, 1 mM DTT and 0.1 mM PMSF) and frozen. Later, the frozen cells were thawed and sonicated. The pellet containing inclusion bodies was recovered by centrifugation at 5,000 rpm for 20 min at 4 °C. The inclusion body pellet was washed three times with lysis buffer containing 1% Triton X-100, followed by two washes with lysis buffer without Triton X-100.
Each histone protein was extracted from the purified inclusion body pellet in a buffer containing 50 mM Tris (pH 7.5), 2 M NaCl, 6 M guanidine hydrochloride and 1 mM DTT for overnight at room temperature. Any insoluble components were removed by centrifugation. Proteins making histone pairs (H2A–H2B and H3–H4) were combined in equimolar ratios and dialysed two times in 1 l of refolding buffer (25 mM HEPES/NaOH (pH 7.5), 2 M NaCl and 1 mM DTT) at 4 °C. Any precipitate was removed by centrifugation for 20 min at 13,000 rpm at 4 °C. The soluble histone pairs were further purified via cation-exchange chromatography in batch (SP Sepharose Fast Flow resin). The samples were diluted fourfold with buffer without salt (25 mM HEPES/NaOH (pH 7.5) and 1 mM DTT) and bound to the resin for 30 min. The resin was extensively washed with 500 mM salt buffer in batch (25 mM HEPES/NaOH (pH 7.5), 500 mM NaCl and 1 mM DTT) and loaded onto a disposable column. On the column, the resin was washed, and pure proteins were eluted with 25 mM HEPES/NaOH (pH 7.5), 2 M NaCl and 1 mM DTT. Soluble histone pairs were concentrated and purified on a Superdex S200 size-exclusion column (GE) equilibrated in 25 mM HEPES/NaOH (pH 7.5), 2 M NaCl and 1 mM DTT. Clean protein fractions were pooled, concentrated and flash frozen.
For cryo-EM grid freezing of ‘assembly 1’ (see below), commercially available OCT4 from Abcam (ab 134876) was used. The protein (approximately 52 kDa) was fused with the herpes simplex virus VP16 transactivation domain at the N terminus and a 11R tag at the C terminus. For the ‘assembly 2’ for cryo-EM and all the other assays, His-tagged OCT4 (approximately 39 kDa) was expressed in a pET28 vector and purified under denaturing conditions from inclusion body using Talon affinity resins. To refold the OCT4 protein, the first overnight dialysis was carried out in 2 M urea, 50 mM HEPES (pH 7.5), 250 mM NaCl, 50 mM l-arginine and 2 mM DTT. Then, the second and third dialyses were carried out for 1 h in a buffer containing 50 mM HEPES (pH 7.5), 100 mM NaCl and 1 mM DTT.
All the OCT4 variants were generated using the inverse PCR strategy. Oligo primers used for mutagenesis were purchased from Integrated DNA Technology and are listed in the Supplementary Table 1. The inverse PCRs were set up in a total volume of 25 μl. After amplification, 10 μl of purified PCR product was incubated with 5 U of T4 PNK in 20 μl of 1× T4 DNA ligase buffer for 1 h at 37 °C. Of T4 DNA ligase, 200 U was added to the reaction and incubated for 1 h at room temperature. Finally, 10 U of Dpn I was added to the reaction and incubated for 1 h at 37 °C. From this mixture, 5 μl was used to transform the competent XL1-Blue E. coli cells. The clones were selected on kanamycin plates and were subsequently confirmed by sequencing.
Histone octamer assembly and purification
Histone octamer purification was done using the standard protocol48,49. In brief, a 2.5-fold molar excess of the H2A–H2B dimer was mixed with the H3–H4 tetramer in the presence of buffer containing 2 M NaCl (25 mM HEPES (pH 7.5), 2 M NaCl and 1 mM DTT). After overnight incubation at 4 °C, the assembled octamer was separated from excess dimer using a Superdex S200 Increase 10/300 GL column on an AKTA FPLC system. The fractions were analysed on SDS–PAGE, pooled and concentrated for final nucleosome assembly.
LIN28B 182-bp DNA amplification
A custom synthesized (Integrated DNA Technology) 162-bp LIN28 genomic DNA8 was cloned into the pDuet plasmid. To make the longer 182-bp LIN28B DNA fragment by PCR, two primers were designed so that each contained an extra 10 bases from the flanking genomic region of the canonical 162-bp LIN28 fragment used in previous studies8. The DNA sequence for the 182-bp extended DNA used in this study is shown in Supplementary Table 1.
Mutant LIN28B DNA
Custom synthesized 182-bp LIN28B DNA was purchased from Integrated DNA Technology with the following mutations in the three OCT4-binding sites:
LIN28B-1M: ATT AAC AT - GCGTCGAT
LIN28B-2M: ATT AAC AT - GCG GCT AT
LIN28B-3M: ATG CTG AAT - GCG GGT AA
The fragments were later PCR amplified to generate DNA for nucleosome assemblies.
OCT4-binding DNA sequences from the human genome
The 186-bp nMATN1 sequence was selected from the human genome (https://www.ncbi.nlm.nih.gov/genome/gdv) from the position GRCh38:1:30216402:30217024:1 on chromosome 1 (ref. 3). The DNA fragment was selected based on the presence of the following OCT4 motifs: ATGCTAAT, ATTAGCAT, ATTAACAT or ATGTTAAT. The 186-bp nMATN1 sequence is shown in Supplementary Table 1.
Nucleosome assembly
Nucleosome assembly was carried out using a ‘double bag’ dialysis method as previously described50,51. The histone octamer and nucleosomal DNA fragment were mixed in equimolar ratios in a buffer containing 50 mM HEPES (pH 7.5), 2 M NaCl and 2 mM DTT. The mixture was placed into a dialysis button made with a membrane with a cut-off of 3.5 kDa. The dialysis button was placed inside a dialysis bag (6–8-kDa cut-off membrane) filled with 50 ml of buffer containing 25 mM HEPES (pH 7.5), 2 M NaCl and 1 mM DTT. The dialysis bag was immersed into 1 l of buffer containing 25 mM HEPES (pH 7.5), 1 M NaCl and 1 mM DTT, and dialyzed overnight at 4 °C. The next day, the buffer was changed to 1 l of a buffer with 25 mM HEPES (pH 7.5) and 1 mM DTT, and dialysis was continued for 6–8 h. In the last step, the dialysis button was removed from the dialysis bag and dialysed overnight into a fresh buffer without any salt (50 mM HEPES (pH 7.5) and 1 mM DTT). The nucleosome assemblies were assessed on a 6% native PAGE using SYBR Gold staining.
Assembly of modified nucleosomes
H3K27ac nucleosomes were assembled using the LIN28B DNA (unlabelled or Cy5-labelled) and histone octamer with H3K27ac modification (custom purchased from Epicypher). For H3K27me3 nucleosomes, the H3K27C-mutant histone was generated using site-directed mutagenesis and later expressed and purified from E. coli. The H3K27C-mutant histone thus obtained was trimethylated using the MLA protocol52 and was purified using a PD10 column. This trimethylated H3 was used with other histones for octamer assembly. The purified H3K27me3 octamer was mixed with LIN28B and nMATN1 DNA for the assembly of H3K27me3 nucleosomes.
Nucleosome array assembly
A 1,022-bp genomic region from the LIN28 genomic site was synthesized by DNA synthesis (Codex, Protein Technology Center, St Jude Children’s Research Hospital). For nucleosome array reconstitution, the DNA fragment was amplified to a larger scale by PCR. For the assembly, the DNA and histone octamer were mixed in a 1:5 ratio.
Nucleosome array reconstitution was carried out using the double bag dialysis salt dilution method described above (see ‘Nucleosome assembly’).
The synthesized genomic DNA sequence used for array assembly (the LIN28B 182-bp region shown in bold) is shown in Supplementary Table 1.
Assembly of the nucleosome–OCT4 complex for cryo-EM grid freezing
The LIN28B complex
Equimolar mixture of histone octamer and LIN28B DNA (2 µM each) were mixed with 1 µM of OCT4 (ab134876, Abcam) and 3 µM of SOX2 (50 mM HEPES (pH 7.5), 2 M NaCl, 20% glycerol and 5 mM DTT). The assembly was carried out with four steps of buffer changes over 72 h. The buffer changes were carried out to dilute out the salt concentration from 2 M starting concentration to a final solvent condition of no salt. The three buffers, used for the assembly dialysis, contained 50 mM HEPES (pH 7.5), 2 mM DTT and varying NaCl concentrations of 2 M, 1 M and 0, respectively. After the assembly, the samples were centrifuged at 13,000 rpm for 10 min at 4 °C to remove any precipitates. Following this, the sample was concentrated using a 10 kDa Centricon to the concentrations needed for cryo-EM grid freezing (0.5–1 µg µl−1).
The assemblies were checked on 6% native gels followed by native western blot analysis. For the detection of nucleosomes, OCT4 and SOX2, anti-H3, anti-OCT4 and anti-His antibodies were used, respectively (see the section ‘Western blot detection’ below).
The nMATN1 complex
For the OCT4 bound to the nMATN1 nucleosome, 1 µM of pre-assembled nucleosomes were mixed with 2 µM of His-tagged OCT4 (see above) and incubated at room temperature for 30 min. The sample was then transferred to ice until grid freezing.
Restriction enzyme Mnl I digestion assays
For digestion of LIN28B nucleosomes, different dilutions of Mnl I (NEB) were made in the 1× CutSmart buffer (NEB). The digestion was carried out for 30 min at 25 °C. For the experiments involving OCT4 and OCT4 variants, the protein was incubated with nucleosomes at 25 °C for 5 min before the addition of Mnl I. After the addition of Mnl I, the samples were kept at 25 °C for 30 min. After the digestion, the samples were run on a 6% polyacrylamide gel to separate all the products and then imaged by SYBR Gold staining on a Typhoon scanner.
Magnesium precipitation assay
LIN28B nucleosome samples were incubated in varying MgCl2 concentrations for 10 min at 25 °C. The precipitated nucleosomes were separated from soluble nucleosomes by spinning at 10,000 rpm for 10 min at 25 °C. The same procedure was followed for nucleosome samples containing wild-type OCT4 and other variants. However, for the experiments done in the presence of OCT4 and OCT4 variants, the nucleosomes were first mixed with fivefold molar excess of OCT4 (or OCT variants) and kept at 25 °C for 5 min before any MgCl2 addition.
Binding assays
The binding assays with OCT4 were performed at 25 °C in 50 mM HEPES (pH 7.5), 200 mM KCl, 1 mM DTT and 0.005% NP-40. The binding assays involving both OCT4 and SOX2 were performed in 50 mM HEPES (pH 7.5) and 1 mM DTT. Typically, 20–40 nM of nucleosome was incubated with different amounts of proteins (OCT4, OCT4 variants and SOX2). For the OCT4-binding experiments, the reaction was incubated for 10 min. For binding involving both OCT4 and SOX2, the reaction was incubated for 10 min after the addition of OCT4, following which SOX2 was added and kept for an additional 5 min. The bound and unbound species were separated on a 5% or 6% native polyacrylamide gel and imaged for Cy5 fluorescence using a Typhoon scanner. In experiments with nucleosomes without Cy5 label, SYBR Gold staining was used to visualize the gels.
Analysis of gels
All the gels were analysed using Quantity One Basic version (Bio-Rad). The data were exported and analysed or plotted using Open Office Calc. All the bands were selected using boxes of the same size: 24 mm2 for input nucleosome and 8 mm2 for all other bands. The background correction was done separately for bands from each lane using boxes of identical size in the same lane.
Analysis of Mnl I digestion of nucleosomes
In the nucleosome-only experiment, after background correction, the signal from the nucleosome band from each concentration point was normalized to the signal from the nucleosome lane in the 0 Mnl I lane. For Mnl I digestion in the presence of OCT4 or its variants, the signal of the OCT4-bound band from each of the Mnl I concentration was background corrected and then normalized to the signal of the OCT4-bound band from the 0 Mnl I lane.
Analysis of the Mg2+ precipitation assays
The relative compaction was calculated as the fraction of the precipitated nucleosomes. For this, the following formula was used: relative compaction = S0 – Sobs. S0 is the signal of the nucleosome band at the 0 Mg2+ concentration normalized to 1, and Sobs is the signal of all the soluble nucleosome bands normalized to the signal of nucleosomes at the 0 Mg2+ concentration. For precipitation experiments in the presence of OCT4 or its variants, the signals from both the bound and the unbound nucleosomal species were summed to calculate the soluble nucleosomes.
Analysis of OCT4 binding to wild-type LIN28B versus the LIN28B-1M mutant
For binding to wild-type LIN28B nucleosomes, all bands were normalized to input nucleosome. For comparison, we used the following equation: binding to OBS2/3 = ‘2-OCT4’/(‘1-OCT4’ + ‘2-OCT4’), where ‘2-OCT4’ represents a nucleosome with two OCT4 bound (OBS1 + OBS2/3), and ‘1-OCT4’ is a nucleosome with one OCT4 bound (OBS1). ‘1-OCT4’ + ‘2-OCT4’ represents input OCT4 bound to OBS1 nucleosomes, which are substrates for binding of the second OCT4. For binding to LIN28B-1M nucleosomes, we used the following equation: binding to OBS2/3 = ‘1-OCT4’/nucleosome, where nucleosome represents input nucleosomes.
Analysis of SOX2 binding to wild-type LIN28B
Binding of SOX2 to OCT-bound nucleosome was calculated as the fraction of SOX2 bound to the OCT4-bound LIN28B nucleosome: SOX2 = ‘1-OCT4–SOX2’/(‘OCT4’ + ‘1-OCT4–SOX2’), where ‘1-OCT4–SOX2’ represent nucleosomes with both OCT4 and SOX2 bound, and OCT4 represents OCT4-bound nucleosomes. ‘1-OCT4’ + ‘1-OCT4–SOX2’ represents input OCT4-bound nucleosomes, which are substrates for binding of the SOX2 to OCT4-bound nucleosomes. Binding of SOX2 to the LIN28B nucleosome is shown as a fraction of free LIN28B nucleosomes: SOX2 = SOX2/nucleosome), where SOX2 represents SOX2-bound nucleosomes and nucleosome represents input nucleosomes.
Analysis of OCT4 binding to unmodified, H3K27ac and H3K27me3 nucleosomes
For binding to modified nucleosomes, we used the following equations: 1st OCT4 = (‘1-OCT4’ + ‘2-OCT4’ + ‘3-OCT4’)/input nucleosome; 2nd OCT4 = (‘2-OCT4’ + ‘3-OCT4’)/(input nucleosome); and 3rd OCT4 = ‘3-OCT4’/(input nucleosome), where 1st, 2nd or 3rd OCT4 indicates binding of the 1st, 2nd or 3rd molecule of OCT4, respectively, ‘1-OCT4’ is a nucleosome with one OCT4 bound, ‘2-OCT4’ is a nucleosome with two OCT4 bound, and ‘3-OCT4’ is a nucleosome with three OCT4 bound. The quantification is shown as a ratio of modified nucleosomes to unmodified nucleosomes (1st OCT4 modified/1st OCT4 unmodified).
Analysis of SOX2 binding to H3K27ac nucleosomes
For binding to modified nucleosomes, we used the following equation: ‘SOX2–OCT4’ = ‘1-OCT4–SOX2’/(‘1-OCT4–SOX2’ + ‘1-OCT4’), where ‘SOX2–OCT4’ represents SOX2 binding to nucleosome with one OCT4 bound, ‘1-OCT4’ represents a nucleosome with one OCT4 bound, and ‘1-OCT4–SOX2’ is a nucleosome with OCT4 and SOX2 bound. The quantification is shown as a ratio of modified nucleosomes to unmodified nucleosomes (‘SOX2–OCT4’ modified/‘SOX2–OCT4’ unmodified).
Western blot detection
SDS–PAGE gels or native PAGE gels were transferred to a PVDF membrane and blocked in TBST (50 mM Tris/HCl (pH 7.5), 150 mM NaCl and 0.1% Tween-20) containing 5% milk for 1 h. Membranes were then incubated in primary antibody in TBST containing 5% milk for 1 h at room temperature. The membranes were washed three times for 5 min with TBST and incubated in secondary antibody for 1 h at room temperature. Membranes were washed three times (approximately 5 min each) with TBST before chemiluminescent detection. The following antibodies were used: anti-OCT4 antibody (1:2,000 dilution; ab109183, Abcam), horseradish peroxidase-conjugated anti-His antibody (1:3,000 dilution; R931-25, Invitrogen–Thermo Fisher), anti-H3 antibody (1:3,000 dilution; ab1791, Abcam) and anti-SOX2 antibody (1:2,000 dilution; ab92494, Abcam), horseradish peroxidase-conjugated anti-rabbit secondary antibody (1:2,000 dilution; 170-6515, Bio-Rad).
MNase-seq
OCT4 was bound to unmodified, H3K27ac or H3K27me3 nucleosomes with LIN28B or nMATN1 DNA (20 mM HEPES (pH 7.5), 50 mM KCl, 2.5 mM MgCl2 and 5 mM CaCl2) and digested by MNase (NEB) for 5 min at 25 °C. MNase digestion was terminated by 50 mM EDTA. Cleaved nucleosome was subjected to phenol/chloroform extraction followed by ethanol precipitation of nuclesomal DNA and used for library preparation. The sequencing library was prepared using the NEBNext Ultra II DNA Library Prep Kit following the manufacturer’s manual. Amplification of the library for Illumina sequencing was performed by PCR using NEBNext Multiplex Oligos for the Illumina kit. Sequencing was pair ended with 100-bp length. Paired reads were merged and filtered by the length of reads between 144 bp and 146 bp and mapped to the LIN28B or nMATN1 sequence with Qiagen CLC genomics Workbench 20 software.
MiDAC purification
MiDAC was purified from 1.25 l of adherent Flp-In 293 T-REx (R78007, Thermo Fisher Scientific) cell lines stably transformed with the Flp-In expression vector carrying FLAG-ELMSAN1/MIDEAS. The cells were grown in DMEM media (Gibco) supplemented with 10% FBS, 100 µg ml−1 hygromycin and induced for 24 h with 1 µg ml−1 doxycycline (Thermo Fisher Scientific). Cells were harvested and lysed using the classical Dignam protocol53. The complex was isolated from the nuclear fraction using anti-FLAG M2 beads from Sigma-Aldrich. The nuclear fraction was mixed with washed FLAG M2 beads and incubated overnight at 4 °C. The next day, the beads were washed with wash buffer (20 mM HEPES (pH 7.9), 300 mM NaCl, 1.5 mM MgCl2, 10% glycerol, 0.5 mM DTT and protease inhibitors (Sigma)) four times. The complex was eluted from the beads in the elution buffer (20 mM HEPES (pH 7.9), 100 mM NaCl, 1.5 mM MgCl2, 0.5 mM DTT and protease inhibitors (Sigma)) after 30 min of incubation at 4 °C. This complex was flash frozen in liquid nitrogen and stored at −80 °C.
Deacetylation of H3K27ac nucleosomes
H3K27ac nucleosomes were deacetylated by the human MiDAC deacetylase complex. The deacetylation reaction was carried out for 18 h at 25 °C in the following buffer: 50 mM HEPES (pH 7.5), 100 mM KCl and 0.2 mg ml−1 BSA. A control parallel reaction containing H3K27ac nucleosomes, but no MiDAC, was also carried out under identical conditions. The extent of deacetylation was confirmed by western blot using anti-H3K27ac antibody.
Negative-stain EM
For the experiment looking at array compaction, 20 nM of the LIN28 array was mixed with MgCl2 to a final [Mg2+] of 3 mM. For analysis of the effect of wild-type and ΔN OCT4 proteins, 70 nM (wild type) and 100 nM (ΔN) proteins were used with the mixture of array and MgCl2.
After approximately 10–15 min of incubation at 25 °C, 3 µl of the sample was added to Lassey carbon or quantifoil grids for 1 min, blotted dry and stained. For staining, four separate drops (approximately 40 µl) of uranyl acetate or uranyl formate were added to a parafilm strip. The grid was briefly brought into contact with the stain for the first three drops before quick blotting. The last drop of stain was kept in contact with the grid for 1 min before the final blot drying.
The dried grids were imaged on a Talos L 120C microscope (Thermo Fisher Scientific) at the cryo-EM facility at St Jude Children’s Research Hospital. Several images were acquired at ×73,000–92,000 magnification from regions showing good particle distribution. Specifically, a magnification of ×73,000 was used for experiments involving Mg2+ compacted arrays in the absence or presence of OCT4; for the experiment with the ΔN variant of OCT4, a magnification of ×92,000 was used. The pixel size was 1.94 Å (73,000) to 1.54 Å (92,000) per pixel on the object scale. The images were later analysed using the ImageJ software after matching the scale from the EM images.
Negative-stain image analysis
Several particles were picked using RELION (n = 450 for arrays in 3 mM MgCl2, n = 262 for arrays in 3 mM MgCl2 with OCT4 and n = 307 for arrays in 3 mM MgCl2 with the ΔN variant of OCT4). For particle picking, the images from the microscope were binned twofold in RELION and saved as 400 pixel × 400 pixel tiff files, which were later analysed using the ImageJ software54. First, the particles were encircled using the free-form selection tool in ImageJ. Later, the ‘set scale’ tool in ImageJ was used to set the size of the pixel in the image to 0.4 nm (pixel size of 0.2 nm at ×73,000 magnification multiplied by 2 for binning in RELION). The particle sizes were measured using the image analyser option in ImageJ and plotted.
Cryo-EM grid preparation and data collection
For cryo-EM of the OCT4-bound LIN28B nucleosome structure, we assembled an OCT4–SOX2–nucleosome complex as described. The sample was concentrated to 0.25 mg ml−1 for the cryo-EM grid. To avoid the extensive aggregation of the complex sample on the cryo-EM grid, OCT4 and SOX2 were mixed with nucleosomes in a 0.5:1 ratio during the assembly. The OCT4-bound nMATN1 nucleosome was assembled as described with a 2:1 ratio of OCT4 to nucleosome. Of the complex sample, 3 μl was applied to a freshly glow-discharged Quantifoil R2/1 holey carbon grid. The humidity in the chamber was kept at 95% and the temperature at +10 °C. After 5 s of blotting time, grids were plunge-frozen in liquid ethane using a FEI Vitrobot automatic plunge freezer.
For the LIN28B nucleosome and the OCT4-bound LIN28B nucleosome, electron micrographs were recorded on FEI Titan Krios at 300 kV with a Gatan Summit K3 electron detector using SerialEM55 (approximately 6,000 and approximately 11,000 micrographs, respectively) at the Cryo-EM facility at St. Jude Childrens’s Research Hospital. Image pixel size was 1.06 Å per pixel on the object scale. Data were collected in a defocus range of 7,000–30,000 Å with a total exposure of 90 e− Å−2. Fifty frames were collected and aligned with the MotionCorr2 software using a dose filter56,57. The contrast transfer function parameters were determined using CTFFIND4 (ref. 58). For the OCT4-bound nMATN1 nucleosome, the data were recorded on the FEI Titan Krios at 300 kV with a Falcon 4 electron detector using EPU (approximately 35,000 micrographs) at the Cryo-EM facility at the Dubochet Center for Imaging (DCI) at EPFL and UNIL. Data were collected in a defocus range of 7,000–25,000 Å. Image pixel size was 0.83 Å per pixel on the object scale.
Several thousand particles were manually picked and used for training and automatic particle picking in Cryolo59. Particles were windowed and 2D class averages were generated with the RELION software package60. Inconsistent class averages were removed from further data analysis. The initial reference was filtered to 40 Å in RELION. C1 symmetry was applied during refinements for all classes. Particles were split into two datasets and refined independently, and the resolution was determined using the 0.143 cut-off (RELION auto-refine option). All maps were filtered to resolution using RELION with a B-factor determined by RELION.
Initial 3D refinement was done with 2,600,000 particles. To improve the resolution of this flexible assembly, we used focused classification followed by focused local search refinements. Nucleosomes were refined to 2.8 Å. Density modification in Phenix improved the map to 2.5 Å (ref. 61). OCT4 bound to DNA (30 kDa) was refined to 4.2 Å using a subset of 65,000 particles after extensive sorting. Using density modification in Phenix, we improved resolution and the appearance of this density to 3.9 Å. The maps have extensive overlapping densities that we used to assemble the composite map and model. The LIN28B nucleosome sample contained 1,000,000 particles, which were refined to 3.1 Å, and improved with density modification to 2.8 Å.
For the second dataset, we collected 1,400 images, yielding 68,000 nucleosomal particles, which refined to 3.7 Å. Classification revealed that approximately 21,000 particles had OCT4 bound, which refined to 4.2 Å.
Molecular models were built using Coot62. The model of the nucleosome (Protein Data Bank (PDB): 6WZ5)63 was refined into the cryo-EM map in PHENIX64. The model of the OCT4 bound to DNA (PDB: 3L1P)19 were rigid-body placed using PHENIX, manually adjusted and rebuilt in Coot and refined in Phenix. Visualization of all cryo-EM maps was done with Chimera65.
Reporting summary
Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article.
Online content
Any methods, additional references, Nature Portfolio reporting summaries, source data, extended data, supplementary information, acknowledgements, peer review information; details of author contributions and competing interests; and statements of data and code availability are available at 10.1038/s41586-023-06112-6.
Supplementary information
Acknowledgements
We thank Cryo-EM Center members at St. Jude Children’s Research Hospital for support with grid screening, especially A. Myasnikov and L. Tang for support with data collection of the LIN28B nucleosome and the OCT4-bound LIN28B nucleosome; A Myasnikov and B. Beckert from the Dubochet Center for Imaging (DCI) at EPFL and UNIL for data collection of OCT4 bound to the nMATN1 nucleosome; H.-M. Herz and Y. Sedkov for FLAG–ELMSAN1 HEK293T cell line and support with MiDAC purifications; I. Chen for critical reading and comments; and Z. Luo for help with making Extended Data Fig. 9j,k. Work in the Halic laboratory is funded by St. Jude Children’s Research Hospital, the American Lebanese Syrian Associated Charities and the US NIH awards 1R01GM135599-01 and 1R01GM141694-01.
Extended data figures and tables
Author contributions
K.K.S. and M.H. designed the experiments. K.K.S. performed the biochemical experiments and electron microscopy. S.B. built the models. Y.D. performed the MNase-seq experiments. D.M. purified the MiDAC complex. K.K.S., S.B., Y.D. and M.H. analysed the data. K.K.S., S.B. and M.H. wrote the paper.
Peer review
Peer review information
Nature thanks the anonymous reviewers for their contribution to the peer review of this work. Peer reviewer reports are available.
Data availability
EM density maps and models have been deposited in the Electron Microscopy Data Bank and PDB under the following accession codes: for OCT4 bound to the LIN28B nucleosome, PDB 8G8G was built using maps EMD-29855 (all particles), EMD-29850 (H3 tail subset), EMD-29852 (H2A tail subset), EMD-29854 (H4 tail A subset), EMD-29854 (H4 tail B subset) and EMD-29846 (OCT4 focus; PDB 8G8E). For OCT4 bound to the nMATN1 nucleosome, EMD-29837 and PDB 8G86 (nucleosome focus); EMD-29841 and PDB 8G87 (OCT4 focus); EMD-29843 and PDB 8G88 (conformation 1); and EMD-29845 and PDB 8G8B (conformation 2). All other data supporting the findings of this study are available within the article and its Supplementary information files.
Competing interests
The authors declare no competing interests.
Footnotes
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Extended data
is available for this paper at 10.1038/s41586-023-06112-6.
Supplementary information
The online version contains supplementary material available at 10.1038/s41586-023-06112-6.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Data Availability Statement
EM density maps and models have been deposited in the Electron Microscopy Data Bank and PDB under the following accession codes: for OCT4 bound to the LIN28B nucleosome, PDB 8G8G was built using maps EMD-29855 (all particles), EMD-29850 (H3 tail subset), EMD-29852 (H2A tail subset), EMD-29854 (H4 tail A subset), EMD-29854 (H4 tail B subset) and EMD-29846 (OCT4 focus; PDB 8G8E). For OCT4 bound to the nMATN1 nucleosome, EMD-29837 and PDB 8G86 (nucleosome focus); EMD-29841 and PDB 8G87 (OCT4 focus); EMD-29843 and PDB 8G88 (conformation 1); and EMD-29845 and PDB 8G8B (conformation 2). All other data supporting the findings of this study are available within the article and its Supplementary information files.