2.1. Cations Promote the Assembly of FUS into Higher-Order Structures in the Presence of PAR-PARP1
Although the mechanism that drives PAR-dependent FUS condensation is well-studied [
7,
14,
26,
27,
28], little is known regarding the effects of PAR-PARP1 on phase behavior of FUS. Earlier, by AFM, FUS has been shown to interact with PAR-PARP1, thereby leading to the formation of supramolecular complexes or multimolecular compartments containing FUS, PAR-PARP1, and damaged DNA [
15]. A recent study has revealed that FUS stabilizes PARP1–DNA condensates, which otherwise dissociate after PARP1 PARylation [
29]. In the cell, PAR mainly exists as a polymer covalently attached to proteins, mainly to PARP1 [
37], and protein-free PAR can arise transiently via hydrolysis of PAR attached to proteins [
38]. Therefore, to assess biological relevance of this phenomenon, here we tested the propensity of FUS for liquid-like assembly under the conditions where negatively charged poly(ADP-ribose) is completely attached to PARP1, i.e., using PAR-PARP1. For this purpose, we employed DLS to monitor changes in hydrodynamic size of FUS in the presence of various concentrations of PAR-PARP1. For these experiments, we used FUS concentrations of 5–10 μM and PARP1 at ~2 μM, which are close to their physiological concentrations [
7,
39], and try to found the PAR-PARP1 concentration that promotes FUS higher-order assembly (
Figure 1). We observed that PAR-PARP1 was not able to induce the assembly of FUS into higher-order structures or protein-rich microphases even at a high FUS-to-PARP1 molar ratio, i.e., when the FUS concentration was one to two orders of magnitude higher than the PAR-PARP1 concentration (
Figure 1).
Only small particles with a hydrodynamic radius of 12–19 nm were detectable under such conditions (
Figure 1). The size of these particles was close to the size of PAR-PARP1 (
Figure 1).
In our previous work, we noticed that aggregates containing FUS, PAR-PARP1, and damaged DNA arise in the presence of Mg
2+ [
15]; moreover, FUS is reported to stabilize PAR-PARP1–DNA condensates also in the presence of Mg
2+ [
29]. Therefore, we hypothesized that PAR-PARP1 could seed FUS liquid-like assembly in the presence of Mg
2+. Given that the cations at low concentration do not trigger the self-assembly of PAR-PARP1 [
36], FUS titration with increasing concentration of PAR-PARP1 was performed at submillimolar concentration of Mg
2+ or other biologically relevant cations such as Ca
2+, Mn
2+, Spd
3+, or Spn
4+ (
Figure 2a–e). Indeed, the automodified PARP1 promoted liquid-like assembly of FUS in the presence of the cations, as evidenced by the emergence of large particles with a radius of 540–834 nm (
Figure 2 and
Figure S1a–e).
The titration of FUS indicated that FUS higher-order assemblies arose at FUS/PAR-PARP1 molar ratios in the range of 200:1 to 50:1 (
Figure 2a–e). Thus, only substoichiometric levels of PAR-PARP1 (at concentration 200- or 50-fold below that of FUS) promoted the protein assembly, because after the increase of PAR-PARP1 concentration, the assembly disappeared (
Figure 2 and
Figure S1a–e). Similar re-entrant phase behavior of FUS with protein-free PAR, but not with PAR-PARP1, has been reported elsewhere [
26,
27]. Although FUS–PAR condensates are stable within a certain concentration range of PAR, they dissolve at a high PAR concentration [
26,
27]. Accordingly, the formation of relatively stable PAR-PARP1-FUS supramolecular assemblies was detectable at a high FUS-to-PAR-PARP1 molar ratio and after the addition of cations.
Both FUS and PARP1 are abundant cellular proteins, and their intracellular concentration has been estimated as 2–8 μM for FUS and 2.0 μM for PARP1
in HeLa cells [7,39]. In our system, we also tested whether the presence of divalent cations was sufficient to induce FUS assembly when PARP1 was added at a micromolar concentration similar to that of FUS, which was within the concentrations found in the cells. By DLS measurements, we analyzed the phase behavior of the proteins within a low FUS-to-PAR-PARP1 molar range (3:1 to 1:1) and after increasing concentrations of Mg
2+, Ca
2+, Mn
2+, Spn
4+, or Spd
3+ (
Figure 3 and
Figure S2). The DLS data suggested that the cations at millimolar concentration promoted the FUS assembly even when PAR-PARP1 concentration was close to that of FUS (
Figure 3). Addition of EDTA, which chelates divalent cations Mg
2+, Ca
2+, and Mn
2+ [
40], to the FUS–PAR-PARP1 mixture resulted in assembly dissolution.
These data strongly support the idea that intermolecular interactions of FUS and PAR-PARP1 are stabilized by cations, even at a low FUS-to-PAR-PARP1 molar ratio that promotes disruption of FUS assemblies (
Figure 2 and
Figure 3). Consequently, we supposed that neutralization of negative charges on the PAR phosphate backbone by cations is key to FUS phase separation in the presence of PAR-PARP1.
Because these cations may promote the self-assembly of PAR-PARP1 even in the absence of FUS [
36], two types of assembly may ensue: PAR-PARP1 or PAR-PARP1–FUS. Therefore, we tested by fluorescence microscopy whether FUS coassembles with PAR-PARP1. To this end, we utilized Alexa Fluor 488 (AF488)-labeled FUS and Cyanine 3 (Cy3)-labeled PARP1 and analyzed the formation of condensates at a low FUS-to-PARP1 molar ratio (4:1) to visualize both the labeled PARP1 and FUS (
Figure 4). An optimal concentration of Mg
2+ was selected to promote the phase separation (15 mM). Starting with the mixture of FUS and PARP1 at micromolar concentration (
Figure 3a), we added NAD
+, which resulted in the formation of small droplets after 30 min incubation of the protein mixture (
Figure 3b). Subsequent incubation of the mixture gave rise to larger assemblies, as evidenced by fluorescence microcopy (
Figure 3c). For instance, the microscopy of the PARylated Cy3-PARP1 and AF488-FUS showed overlapping green (AF488) and red (Cy3) fluorescence signals, indicating simultaneous presence of the two proteins in the assemblies, i.e., FUS–PAR-PARP1 coassembly in vitro (
Figure 3b,c).
Overall, these experiments suggested that FUS coassembly with PAR-PARP1 can be influenced by divalent cations or polyamines. Therefore, we were able to vary phase separation of FUS either by decreasing PAR-PARP1 concentration or by adding cations that stabilize the condensates (
Figure 2 and
Figure 3). On the basis of these results, we next studied the impact of PAR structure on the assembly formation in the PAR-PARP1–FUS system.
2.2. Frequency of Branching of PAR Influences the Assembly of FUS into Higher-Order Structures in the Presence of PAR-PARP1
PAR produced by PARP1 is a polymer with branching structure and may contain up to 200 ADP-ribose units with branch points (~1%) occurring approximately every 20–50 units [
17,
41,
42]. Taking into account that protein-free PAR’s length influences FUS condensation [
26], we hypothesized that the changing of PAR structure, namely, formation of short, long, and/or hyperbranched polymers—when the polymer is covalently attached to PARP1—may also modulate FUS phase separation. To clarify the influence of PAR structure on FUS’s phase behavior, we used point mutants of PARP1 that are a less active than the wild-type enzyme and synthesize short (PARP1
Y986S) or short hyperbranched (PARP1
Y986H) PAR that causes alterations in the morphology of PAR-PARP1 molecules [
42,
43,
44]. Under our experimental conditions, the PARP1
Y986S mutant manifested 15% residual activity relative to PARP1
WT, whereas the PARP1
Y986H mutant showed 50% activity (
Figure S3).
On the one hand, it has been found that protein-free PAR contributes to phase separation of FUS by acting as a molecular “seed” that promotes protein assembly [
7,
14,
26,
27]. On the other hand, PAR readily disrupts FUS assemblies when present in a large molar excess over FUS [
26,
27]. Accordingly, a FUS–PAR system involves phase transition of FUS from one phase to two phases and back to one phase in response to an increase of PAR concentration. This observation suggested that the less effective PAR synthesis by the PARP1 mutants may contribute to the stability of higher-order assembly of FUS in the presence of PAR-PARP1. Therefore, we tested FUS assembly in the presence of PAR- PARP1
Y986H or PAR-PARP1
Y986S. As in the case of PARP1
WT (
Figure 1), PARylation of either PARP1
Y986H or PARP1
Y986S did not trigger their self-assembly (
Figure S4). Then, we again employed DLS to monitor changes in the hydrodynamic size of FUS at a high FUS-to-PAR-PARP1
Y986H (or FUS-to-PAR-PARP1
Y986S) molar ratio and submillimolar concentration of Mg
2+ (
Figure 5a,b and
Figure S5a,b).
In the case of PARP
Y986S (producing short PAR), higher-order assemblies were observed at a high FUS-to-PAR-PARP1
Y986S molar ratio (145:1 to 75:1) (
Figure 5a and
Figure S5a). Thus, the FUS–PARP1
Y986S assembly was stable within a molar ratio that was close to the ratio observed with PARP1
WT (
Figure 2a and
Figure 5a). The results indicated that the less extensive PARP1 autoPARylation and biosynthesis of shorter PAR only slightly affect the FUS-to-PARP1 molar ratio that favors higher-order assembly of FUS with PAR-PARP1.
At the same time, FUS possesses a strong ability to form higher-order assemblies (R
h > 200 nm) with PAR-PARP1
Y986H, which produces a hyperbranched polymer (
Figure 5b and
Figure S5b). In fact, FUS retained the capacity for microphase separation in a broad range of protein-to-PAR-PARP1
Y986H molar ratios (200:1 to 10:1), whereas in the cases of PAR-PARP1
WT and PAR-PARP1
Y986S, large particles were detected in a narrower range of the FUS-to-PARP1 molar ratio (200:1.0 to 50:1.00) (
Figure 2b and
Figure 5b). Our results also revealed that the PAR-PARP1
Y986H mutant (synthesizing hyperbranched PAR) is able to induce FUS assembly even in the absence of cations (
Figure 5c and
Figure S5c).
Similar to PARP1
WT, these mutants could also promote FUS higher-order assembly at a low FUS-to-PARP1 molar ratio in the presence of Mg
2+ when large particles with R
h (~267 nm) and R
h (~103 nm) were detectable (
Figure 5d and
Figure S5d). Consequently, FUS’s microphase-separated state strongly depends on the FUS-to-PAR-PARP1 molar ratio, which differed between the PARP1 mutants producing PAR of different lengths and branching modes. Nevertheless, cations (Mg
2+) were still needed to induce the assembly at a low FUS-to-PAR-PARP1
Y986H molar ratio (
Figure 5d and
Figure S5d).
To confirm that the PAR-PARP1–FUS assembly is affected by the structure of PAR, we tested whether the cation concentration (in particular Mg
2+) needed to induce FUS microphase separation differed between PARP
WT, PARP1
Y986S, and PARP1
Y986H (
Figure 6,
Figures S6 and S7). For this purpose, we compared the assembly of FUS with PAR-PARP1
WT or its mutant in the presence of different concentrations of Mg
2+ by measuring turbidity, which correlates with protein phase separation [
45] (
Figure 6,
Figures S6 and S7). It was observed that at a low FUS/PAR-PARP1 molar ratio (~1:1), already 9 mM Mg
2+ can promote microphase separation after mixing of FUS and (highly branched PAR)-PARP1
Y986H (
Figure 6). In contrast to PARP1
Y986H, Mg
2+ concentration higher than 11.3 mM was required for inducing FUS microphase separation in the presence of either PAR-PARP
WT or PAR-PARP1
Y986S (
Figure 6). Thus, the biosynthesis of highly branching PAR during PARP1 automodification required lower Mg
2+ concentrations to promote FUS phase separation. We also tested the effect of 1,6-hexanediol: a compound widely used to disrupt weak protein–protein hydrophobic interactions underlying FUS LLPS [
46].
A significant decrease in the turbidity was observed after the addition of 1,6-hexanediol to a PAR-PARP1–FUS solution, suggesting that nonionic interactions play an important part in this Mg
2+-dependent assembly of FUS and PAR-PARP1 molecules. For a FUS–PARP1
Y986H mixture, addition of 2.8% of 1,6-hexanediol diminished the turbidity twofold, suggesting that 1,6-hexanediol is efficient in disrupting the microphases (
Figure 6). On the other hand, addition of 1,6-hexanediol up to 15% to a FUS-and-PAR-PARP1
WT or FUS-and-PAR-PARP1
Y986S solution respectively gave only a 17% and 13% reduction in turbidity (
Figure 6).
Therefore, in contrast to FUS–PAR-PARP1WT or FUS–PAR-PARP1Y986S, the FUS–PAR-PARP1Y896H assembly has higher susceptibility to dissolution by 1,6-hexanediol, indicating that this microphase-separated state depends to a lesser extent on the presence of a cation decreasing the involvement of electrostatic interactions. Accordingly, hydrophobic interactions notably contribute to FUS–PAR-PARP1Y896H microphase separation. Although a noticeable reduction in turbidity by 13–50% for PAR-PARP1WT and its mutants was registered at concentrations of 2.8% to 15% 1,6-hexanediol, the reagent was not able to completely disrupt FUS–PAR-PARP1 assemblies coming into being in the presence of Mg2+.
Only the addition of EDTA readily disrupted the assemblies, and the turbidity of the solution returned to a value similar to that of the solution with 4 mM Mg
2+ (
Figure 6).
These results indicated that the assembly of FUS with PAR-PARP1 is indeed a mainly cation-regulated process; however, hydrophobic interactions sensitive to 1,6-hexanediol treatment also help to stabilize the condensates.
As reported elsewhere, mutations Y986S or Y986H in PARP1 alter both overall protein activity and PAR chain structure [
42,
43,
44]. Consequently, these mutations could influence the size of PAR-PARP1–FUS assemblies. To clarify this issue, we visualized a mixture of either PAR-PARP1
WT or PARP1
Y986H with FUS by AFM (
Figure 7). To evaluate the size of PAR-PARP1–FUS assemblies in the presence of Mg
2+, first, AFM imaging of PARP1
WT and PARP1
Y986H was undertaken after incubation with a gapped pBR322 (pBR) plasmid in the presence of NAD
+ (
Figure 7).
As for PARP1
WT, the PARylated molecules had a size (diameter) up to 52 nm, whereas in the case of PARP1
Y986H, the size was only ≤40 nm (
Figure 7b). Consistently with our previous AFM data [
44], modified molecules of PARP1
Y986H synthesizing hyperbranched PAR were found to carry highly packed polymer chains in contrast to PARP1
WT (
Figure 7). The activation of PARP1
WT and its mutants as detected by AFM enabled us to measure the average size of the assemblies engendered by PARylated proteins after the addition of FUS (
Figure 7). We noticed that a decrease in the size of PAR-PARP1
Y986H was accompanied by a diminishing size of the assemblies that were formed by FUS in the presence of PAR-PARP1
Y986H (
Figure 7).
Consequently, the structure of PAR, mainly its branching frequency, is an important factor for FUS higher-order assembly with PAR-PARP1 and influences the size of assemblies and the cation concentration required for the stabilization of the FUS microphase separation process.