Keywords
biomolecular condensate, RNA processing, FLC, COOLAIR, noncoding RNA 15
Abstract
16
The Arabidopsis RNA binding protein FCA is found in liquid-like nuclear condensates and promotes 17
proximal polyadenylation of specific nascent transcripts. To understand the in vivo interactions required 18
for these condensates we used single-particle tracking experiments on FCA expressed at endogenous 19
levels in live cells. These revealed FCA forms a core tetramer that multimerizes into higher-order 20
particles (~16 to 5 6 FCA molecules ), corresponding to condensates observed using confocal 21
microscopy. The coiled -coil protein FLL2, genetically required for FCA function and condensate 22
formation, showed co-localization primarily to the larger condensates. FCA regulates FLC, however, 23
its in vivo co-localization with an FLC lacO/LacI transgene was found to be infrequent. A missense 24
mutation in the FCA RRM domain showed RNA binding to FCA is necessary for function. This reduced 25
RNA-binding activity, attenuated FCA condensate formation, 3’ RNA processing and FLC repression, 26
however it did not influence the core tetramer. Our work points to a modular structure for FCA 27
condensates centred around a core of four FCA molecules , which multimerize to larger functionally 28
important condensates via associated RNA and FLL2 interaction, with only transient residency at their 29
site of action. 30
31
Introduction
32
Cellular compartmentalization by biomolecular condensates is associated with diverse processes in 33
eukaryotic cells (Banani et al, 2017). While in vitro studies have highlighted their roles in increasing 34
local concentration and residence time of interacting components, the functional characteristics of 35
heterogeneous condensates in vivo remain unclear. Plants are an excellent system in which to study 36
biomolecular condensates (Field et al, 2023). For example, Arabidopsis FLOWERING LOCUS C (FLC), 37
a gene encoding a key flowering repressor, is regulated by co-transcriptional and antisense-mediated 38
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chromatin silencing mechanism s (Fang et al , 2020 ; Xu et al , 2021 ) that involves multiple nuclear 39
biomolecular condensates with very different properties (Zhu et al, 2021; Fiedler et al, 2022; Berry et 40
al, 2017). One of those is a liquid-like condensate that involves an RNA-binding protein called FCA, 41
which directly interacts with FY , a Pfs2p/WDR33 homologue and a central component of the 42
polyadenylation machinery in eukaryotes (Simpson et al , 2003) . FCA contains two RRM (RNA 43
Recognition Motif) domains and a WW domain located between two predicted prion -like domains 44
(Macknight et al , 1997) . It was shown to form nuclear condensates through liquid-liquid phase 45
separation and to recruit RNA 3’ processing factors (Fang et al, 2019). Mutant screening identified a 46
coiled-coil protein, FLL2, required for the liquid-liquid phase separation of FCA nuclear condensates 47
and participation in FLC regulation (Fang et al, 2019). In vitro assays revealed that FCA condensates 48
were enhanced by addition of low amounts of Arabidopsis RNA. However, the immunoprecipitation of 49
COOLAIR nascent transcripts by FCA was not dependent on FLL2 (Fang et al, 2019). 50
51
We have continued our investigations of the properties of FCA liquid-like condensates and exploited a 52
single-molecule imaging technique, using Slimfield microscopy with an oblique illumination angle of 53
60 ± 5°degrees to enhance imaging contrast (Plank et al., 2009). This enables simultaneous tracking of 54
individual molecules within a wide range of biological condensates providing quantitative 55
measurements of molecule number and molecular motion behavior in plant nuclei (Shen et al, 2023). It 56
has been used to study biomolecular condensates in live cells including bacteria, yeast or mammalian 57
cells (Kent et al, 2020; Izeddin et al, 2014; Ladouceur et al, 2020; Biswas et al, 2022) and we adapted 58
it for living plant tissues to specifically study nuclear proteins (Bayle et al, 2021). 59
60
Our findings indicate that FCA condensates consist of multimers of a tetrameric FCA core, with sizes 61
ranging from approximately 16 to 56 molecules. The lower diffusion coefficient of the larger particles, 62
compared to core particles, suggests they correspond to the liquid-like condensates observed using 63
confocal microscopy. Notably, FLL2, essential for FCA function, predominantly co -localizes within 64
the larger condensates. However, sustained co -localization of large FCA condensates with the FLC 65
locus is observed only infrequently. The involvement of RNA in promoting FCA condensation was 66
shown through the identification of a missense mutation in the FCA second RRM domain . This 67
mutation reduced RNA-binding activity in vitro, significantly attenuated FCA condensate formation , 68
lowered RNA 3’ processing efficiency and prevented FLC repression but did not influence the core 69
tetramer. Our work points to a modular structure for FCA and RNA 3’ processing condensates, with a 70
core of four FCA molecules that multimerize via associated RNA and FLL2 interaction to larger 71
functionally important condensates. 72
73
Results
74
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Single-particle tracking reveals physical properties of FCA condensates. 75
Biomolecular condensates are considered to increase local concentration of its components (Banani et 76
al, 2017; Shin & Brangwynne, 2017). To assess the consequence of condensation on FCA function, we 77
generated plants carrying an FCA -mScarlet-I translational fusion. A mScarlet-I coding sequence was 78
inserted into an FCA genomic clone and transgenic plant lines carrying single T-DNA insertion were 79
generated, where the fusion was expressed at similar level as the endogenous FCA gene (Fig EV1A and 80
B). The FCA mScarlet-I fusion formed liquid-like condensates (Fig 1A) and rescued the fca-9 mutant 81
phenotype (Fig EV1B). mScarlet-I is a bright red fluorescent protein known for its characteristics as a 82
rapidly maturing monomer (Bindels et al , 2016) and using this in conjunction with the Slimfield 83
microscope provided the capability to track very small FCA particles dynamically in vivo (Fig 1A). The 84
single-molecule sensitivity of Slim field in vivo, coupled with stepwise photobleaching of fluorescent 85
protein tags (Leake et al, 2006; Reyes-Lamothe et al, 2010), also enabled accurate quantification of the 86
number of molecules (stoichiometry) within the condensate (EV2; Jin et al, 2021). 87
88
Analysis of the single-particle tracking dataset identified a distinct peak representing approximately 4 89
molecules of FCA (Fig 1B) with other peaks in multiples of 4 from approximately 16 to 56 molecules. 90
To investigate whether these regular peaks follow specific patterns, we conducted simulations through 91
kernel density estimation to assess their periodicity (Leake et al, 2008). The estimate of the number of 92
molecules in a repeat unit depends on consistent stoichiometry intervals observed between nearest -93
neighbor peaks in the stoichiometry distribution. The periodicity peaks for FCA particles were found to 94
be approximately 4.2 and 8.7 (Fig 1C). 95
96
Particles can also exhibit different motion behaviour (Shen et al, 2023). We analysed the diffusion 97
coefficient of individual particles and plotted single particles with stoichiometry. Generally, particles 98
with low stoichiometry display variable mobility, while those with high stoichiometry show low 99
mobility (Fig 1D). These results suggest that the core module of an FCA particle is a tetramer with 100
larger condensates forming through the higher-order assembly of these tetrameric cores. 101
102
The co-localization of FCA and FLL2 is primarily observed in the prominent foci in 103
Arabidopsis. 104
105
Our previous study used transient assays suggested that FCA condensates serve as the sites for the 106
interaction between FCA, FLL2 and 3’ -end processing factors (Fang et al , 2019) . However, the 107
condensates formed by FCA and FLL2 exhibited different patterns in low resolution images of 108
Arabidopsis roots (F ang et al, 2019). To investigate the potential co -localization of FCA and FLL2 109
within the same nuclear condensates in vivo, we crossed plants carrying an FCA-mTurquoise2 transgene 110
(Xu et al, 2021) with plants carrying FLL2-eYFP transgene (Fang et al, 2019) and generated double 111
homozygotes. Utilizing 3D imaging and Airyscan confocal microscopy, we found that FCA and FLL2 112
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generally reside in distinct fluorescent foci within the cell nucleus (Fig 2A) but co-localize within a few 113
larger foci (Fig 2B and D). We conducted a comprehensive analysis to determine the size distributions 114
for FCA, FLL2 and FCA/FLL2 -co-localized condensates (Fig 2 C). The data suggest a specific 115
association between FCA and FLL2 within larger condensates. 116
117
To determine if the se prominent FCA/FLL2 condensates directly associate with the FLC locus, we 118
crossed the FCA-mScarlet-I transgene into a line carrying a previously established FLC-lacO/LacI-119
eYFP system that enables spatial localization of the FLC locus in the nucleus (Rosa et al, 2013). FCA 120
condensates did not frequently co-localize with the FLC-lacO/LacI-eYFP marked locus (Fig EV3). 121
Only 2.7% of identified FCA condensates partially co-localized with the FLC-lacO/LacI-eYFP locus 122
suggesting that FCA condensates only transiently associate with the FLC locus. 123
124
FCA condensation is dependent on a functional RRM domain. 125
To further investigate the functional significance of the heterogeneity in FCA condensates we continued 126
a genetic screen for factors essential for FCA function (Liu et al, 2007). This identified a missense 127
mutation on the FCA overexpression transgene at amino acid 304 of the FCA protein , resulting in a 128
leucine to phenylalanine change (Fig EV1C). This alteration is located within the second RRM domain 129
of FCA, a domain conserved across various species (Macknight et al , 1997) . The impact of this 130
missense mutation on the RNA-binding activity was established through in vitro RNA-binding assays 131
(Fig EV1D). That the mutant came out of an FLC mis-expression screen and exhibited late flowering 132
shows the RNA-binding activity is important for FCA function (Fig EV1E). 133
134
To examine whether this RRM mutation affects FCA condensation, we generated transgene constructs 135
expressing an FCA wild-type genomic DNA fragment with (FCArrm) and without (FCAwt) the RRM 136
mutation fused with mScarlet-I and introduce them into fca-9 mutant (Fig EV1A). After selecting for 137
single insertion transgenic plants and homozygotes, we analysed the FCAwt condensates within the 138
nuclei of young roots using Airyscan confocal microscope. Plants containing t he FCArrm transgene 139
limited the size and number of condensates, displaying a more diffuse signal compared to plants 140
carrying FCAwt (Fig 3A and B). 141
142
In order to determine whether the RRM mutant alters the structure of FCA condensates, we also 143
conducted single-particle tracking with the FCArrm lines. We observed an obvious stoichiometry peak 144
of approximately 4 molecules for FCArrm, slightly higher than that for FCAwt (Fig 3C; Appendix Fig 145
S1). However, when focusing on particles with stoichiometries exceeding 8 molecules, the probability 146
density of FCArrm was found to be lower than FCAwt. FCArrm particles with more than 16 molecules 147
were scarce, however, the integrated nuclear intensity of fluorescent signal in FCArrm and FCAwt 148
showed no obvious change ( Appendix Fig S 2). This result suggests that the reduced RNA -binding 149
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activity of FCA proteins decreases their likelihood of forming larger particles with a range of 16 to 56 150
molecules, consistent with the confocal imaging analysis. 151
152
To determine if the RRM mutant changed the physical properties of FCA condensates, w e compared 153
the diffusion coefficient s of individual particles with their stoichiometry (Fig 3 D). The mean 154
stoichiometry of FCArrm is lower than that of FCAwt, while the overall pattern of diffusion coefficients 155
is distributed towards slightly higher values (Fig 3E; Appendix Fig S3). Surprisingly, the periodic unit 156
of FCArrm only experiences a minor reduction compared to FCAwt, which implies that FCA proteins 157
with reduced RNA-binding activity retain the capacity to form the tetrameric core (Fig 3F). Thus, the 158
RNA-binding activity of FCA proteins affects the formation of larger condensates but does not affect 159
core protein assembly. 160
161
The functional RNA-binding domain is required for COOLAIR R-loop resolution and FCA auto-162
regulation. 163
We then used the FCAwt and FCArrm lines to further investigate the functional importance of RNA 164
binding. Compared to the FCAwt transgenic plants, FCArrm plants displayed higher levels of FLC 165
expression and therefore flower ed late (Fig 4 A and B , EV1B ). FCA associate s with COOLAIR, 166
recruiting 3’ processing factors to promote proximal COOLAIR polyadenylation, thus resolving a 167
COOLAIR-formed R-loop (Liu et al, 2010; Xu et al, 2021). The ratio of proximal-to-distal isoforms of 168
COOLAIR transcripts was reduced in the FCArrm lines compared to FCAwt consistent with reduced 169
R-loop resolution when RNA binding is defective (Fig 4 C). S9.6-DNA/RNA immunoprecipitation 170
followed by cDNA conversion (DRIPc)-qPCR analysis also revealed FCArrm has reduced ability to 171
resolve the COOLAIR-induced R-loop (Fig 4D). 172
173
FCA autoregulates itself promoting polyadenylation at the proximal sites in intron3 (Quesada et al, 174
2003), so we conducted Quant-seq analysis to capture polyadenylated FCA transcripts in Col-0, FCAwt, 175
FCArrm and fca-9. In FCArrm and fca-9, the re were significantly fewer reads of transcripts 176
corresponding to proximally polyadenylated FCA transcripts compared to Col-0. Conversely, reads at 177
the distally polyadenylated site of FCA increased (Fig 4E-F), all consistent with reduced FCA function. 178
RNA-binding activity is thus important for FCA condensation and for well-defined FCA functional 179
roles, promotion of proximal COOLAIR termination and R-loop resolution. 180
181
Discussion
182
Our study provides insight on the functional properties of the dynamic liquid-like RNA 3’ processing 183
condensates containing the Arabidopsis nuclear RNA -binding protein FCA. We conducted single -184
particle tracking to determine the molecular stoichiometry and diffusivity of FCA condensates in plant 185
nuclei. This revealed insights into the particle assembly size and association of FCA with its protein 186
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and RNA partners functioning in FLC repression. Our work points to a modular structure for FCA 187
condensates centred around a core of four FCA molecules, which multimerize to larger functionally 188
important condensates via associated RNA and FLL2 interaction, with only transient residency at their 189
site of action. 190
191
The missense mutation in the FCA RRM domain reduced RNA-binding activity, attenuated condensate 192
formation and prevented FLC repression but the stoichiometry of the smaller FCA particles was 193
unaffected. The lack of effect of RNA binding on the core modular structure is similar to previous 194
observations with ELA V , a well-characterized RNA-binding protein with three RRM domains. ELA V 195
multimerizes on its target RNAs and forms a defined complex (Soller & White, 2005). Future analysis 196
should examine how FCA core tetramers multimerize. The FCA prion-like domain (Chakrabortee et al, 197
2016), RRM domain (Macknight et al, 1997), WW domain (Simpson et al, 2003; Henderson et al, 2005) 198
and extended NH2 terminus initiating in a non -methionine start codon (Simpson et al, 2010) may all 199
play a role. In addition, m6A exerts function in the regulatory mechanisms of FLC and COOLAIR (Xu 200
et al, 2021; Wang et al, 2022; Sun et al, 2022; Amara et al, 2023); we need to understand if the dynamic 201
structures are affected by RNA modification and how this tetramer interfaces with its target RNAs . 202
Continued analysis of the role of the first RRM may also be productive as the protein phosphatase 203
SSU72 was found to antagonize FCA’s binding to COOLAIR in a manner dependent on the first RRM 204
motif (Yongke Tlan et al, 2019). 205
206
COOLAIR transcripts form dense ‘clouds’ at each FLC locus as judged by single-molecule fluorescence 207
in situ hybridization, which are enhanced upon cold exposure (Rosa et al., 2016). Whether the FCA 208
condensates associate with these RNA condensates will require RNA live imaging analysis. It is 209
interesting to speculate that COOLAIR molecules might undergo thermo-responsive phase transitions 210
as has been found recently for other RNAs (Wadsworth et al., 2023). Protein partners can tune this 211
phase behavio ur (Ruff et al ., 2020) , so this system has a lot of potential to uncover fundamental 212
principles of condensate functionality in vivo , and if transient association with the FLC locus is 213
sufficient for function. In mammalian cells, Mediator -bound enhancers only sporadically co -localize 214
with their target loci. This variability in co-localization can be attributed to a dynamic kissing model, 215
where a distal Mediator cluster interacts with the gene only at specific timepoints (Cho et al, 2018). 216
217
Our work demonstrates the power of studying biomolecular condensate functionality in genetically 218
tractable systems. Arabidopsis with its extensive genetic resources, ability to make transgenic lines and 219
small, transparent roots is particularly suitable for these studies, as illustrated by our ability to image 220
condensates in living roots with the single-molecule sensitivity of Slim field. Coupled with stepwise 221
photobleaching we could accurately quantify the number of molecules within condensates providing 222
mechanistic insights into the modular structure of FCA condensates , with and without various 223
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functionally important partners. These tools now allow us to explore the role of FCA condensate 224
dynamics in response to various environmental exposures. 225
226
Materials and methods
227
228
Plant materials and growth conditions 229
The wild type Col-0, fca-9 mutant allele, pFCA::FCA-mTurquoise and pFLL2::FLL2-eYFP transgenic 230
plants were described previously (Fang et al , 2020 ; Xu et al , 2021 ). To generate the pFCA::FCA -231
mScarlet-I transgenic plants, FCA genomic DNA fragments was amplified and insert into the pENTRY 232
vector. The mScarlet -I coding sequence was inserted before the stop codon via In -Fusion seamless 233
cloning. The FCA genomic DNA fragment fused mScarlet -I was transferred to pSLJ699I5 vector via 234
gateway cloning. The RRM mutation construct is modified from wild -type FCA genomic DNA 235
constructs via In-Fusion seamless cloning . These constructs were transformed into the fca-9 mutant. 236
Arabidopsis seeds were surface sterilized and sown on standard half-strength Murashige and Skoog (½ 237
MS) medium plate without glucose and stratified at 4 °C for 3 days before transferred to long -day 238
conditions (16-h light at 20 °C, 8-h darkness at 16 °C). 239
240
Confocal microscopy of FCA-mScarlet-I 241
Plants were grown vertically on half strength MS plates for 4-7 days. Confocal images were acquired 242
on a Zeiss LSM 880 upright microscope equipped with an Airyscan detector. Samples were imaged 243
through a C-Apochromat 63x/NA 1.2 water-immersion objective by exciting them at 561 nm and using 244
the Airyscan detector in super resolution mode. The fluorescence emission arrived at the detector after 245
passing through a filter that allowed wavelengths between 495 -550 nm and above 570 nm to pass 246
through. The voxel size was 0.06 × 0.06 × 0.26 µm (xyz) and the pixel dwell time was 1.78 µs. Z-stacks 247
comprised 28 slices and spanned a 7.13 µm range. After Airyscan processing, the image analysis was 248
performed in Arivis Vision4D ver. 4.1.0. (Zeiss) as described below. 249
250
Co-localization analysis of FCA and FLL2 251
Confocal images were acquired either on the Zeiss LSM 880 microscope mentioned above or a Zeiss 252
LSM 980 confocal microscope. For using LSM880, line by line sequential acquisition was employed. 253
Samples were imaged through a C -Apochromat 63x/NA 1.2 water-immersion objective and were 254
excited at 458 (mTurquoise) and 514 nm (eYFP). The fluorescence emission of the samples passed 255
through a filter that only allowed wavelengths in the 465-505 nm range and above 525 nm to reach the 256
Airyscan detector, which was operating in super resolution mode. The voxel size was 0.05 × 0.05 × 257
0.21 µm (xyz) and the pixel dwell time was 0.72 µs. Z-stacks comprised 25 slices spanning a 4.96 µm 258
range. 0.2 mm TetraSpeck microspheres (Thermo Fisher Scientific, UK) were imaged using these same 259
settings and the resulting images were used to correct the sample images for chromatic aberration. The 260
correction was performed in Zen (Zeiss, Germany) using the channel alignment method. 261
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For using Zeiss LSM 980, frame by frame acquisition was employed. Samples were imaged through a 262
C-Apochromat 63x/NA 1.2 water-immersion objective and were excited at 445 (mTurquoise) and 514263
nm (eYFP). The fluorescence emission of eYFP was collected through a filter that only allowed 264
wavelengths in the 530-582 range to reach the Airyscan detector, whereas the fluorescence emission of 265
mTurquoise was collected through a filter that allowed wavelengths in the 422 -497 and 607-735 nm 266
ranges to reach the Airyscan detector. The detector was operating in super resolution mode. The voxel 267
size was 0.05 × 0.05 × 0.20 µm (xyz) and the pixel dwell time was 1.06 µs. Z-stacks comprised 30 slices 268
spanning a 5.8 µm range. 269
270
After Airyscan processing, t he image analysis was performed in Arivis Vision4D ver. 4.1.0. (Zeiss). 271
Firstly, the blob finder algorithm was applied to the mTurquoise2 channel using a diameter value of 272
0.35 mm, a probability threshold of 60%, and a split sensitivity of 50%. Then, the blob finder algorithm 273
was applied to the eYFP channel using a diameter value of 0.30 mm, a probability threshold of 50%, 274
and a split sensitivity of 50%. Blob finder is a segmentation algorithm that excels at finding round or 275
spherical objects in 2D or 3D, respectively. It uses a Gaussian scale to identify seeds for the objects and 276
subsequently applies a watershed algorithm to determine the boundaries of the objects. Afterwards, the 277
intersection between the output of the two blob finder operations was calculated. Finally, metrics such 278
as volume, mean intensity, and total intensity were computed for the objects generated by each of the 279
blob finder operations, as well as for their intersection. 280
281
Slimfield microscopy 282
The customized Slim field microscope was previously described ( Payne-Dwyer and Leake, 2022). 283
Continuous wave lasers (Coherent OBIS) delivered a de -expanded Gaussian beam mode (TEM00) to 284
the back aperture of an NA 1.49 Apo TIRF 100× oil immersion objective lens (Nikon). Single molecule 285
sensitivity was achieved using a fast sCMOS camera (Photometrics Prime95B) which triggered a 286
continuous wave laser for 10 ms exposure per frame at 80 Hz. Excitation and emission filters were 287
tailored to mScarlet-I (594/25 nm) for their respective red channels. The total magnification was 288
approximately 200×, resulting in an oversampled image pixel edge size of 53 nm. Nuclei were identified 289
using brightfield mode to determine the best focus and were subsequently captured for manual 290
segmentation later. Fluorescence acquisition settings in the green and red channels were pre-optimized 291
to prevent initial saturation and to ensure the detection of individual molecular brightness tracks for 292
mScarlet-I. These settings were then locked to prevent systematic variation in the characteristic single 293
molecule brightness. 294
295
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Single-particle tracking and intensity analysis 296
Fluorescent foci were identified from Slimfield image sequences and linked into tracks using 297
ADEMScode software ( Plank et al , 2009 ). Each of these foci were localised to a super -resolved, 298
subpixel precision, typically 40 nm. The random overlap probability was estimated using a nearest 299
neighbour distance approach (Payne-Dwyer et al, 2023). Analysis was spatially restricted to data lying 300
within a region of effectively uniform laser illumination (80% ± 9% s.d. peak intensity ) by cropping 301
images to an area of 240 × 184 pixels (12.7 × 9.8 μm). Fluorescence image sequences were further 302
cropped to specify individual nuclei, using manually segmented masks from brightfield images. 303
The 2D diffusion coefficient of each track ( 𝐷) was computed using the increase of mean-square 304
displacement across time interval according to a random walk model (Leake et al , 2008) . Focus 305
intensity was calculated by summing the pixel value s within a 5-pixel distance and subtracting an 306
averaged background level from the rest of a 17-pixel square (Leake et al , 2008) . The track 307
stoichiometry was found by extrapolating the first 5 foci intensities to account for photobleaching 308
(Syeda et al., 2019), then dividing this initial intensity by the characteristic single molecule brightness 309
(Wollman et al ., 2017) . The characteristic single molecule brightness linked to each reporter was 310
determined as 110 ± 15 (mean ± sem) for mScarlet-I based on the Chung-Kennedy-filtered terminal 311
intensity of tracks in each acquisition (Leake et al, 2003), thus providing an internal calibration for track 312
stoichiometry, periodicity, and nuclear protein copy number. 313
314
To calculate periodicity, the stoichiometries of all tracks within each nucleus were represented as a 315
kernel density distribution (Leake et al , 2014) , employing an empirical standard deviation of 0.6 316
molecules on the characteristic single molecule brightness. Peaks within this distribution were identified 317
using the MATLAB findpeaks function, and the intervals between nearest neighbour peaks were 318
computed (Payne-Dwyer and Leake, 2022). Raw estimations of the total number of molecules in each 319
nucleus were determined using ImageJ macros to integrate the pixel values inside segmented nuclei as 320
in previous work (Wollman and Leake, 2015; Payne-Dwyer and Leake, 2022). The nuclear protein copy 321
number of each reporter dataset was refined to exclude autofluorescence by calculating the difference 322
between mean integrated nuclear intensities of the labelled dataset and an unlabeled control, adjusted 323
proportionally to the ratio of mean nuclear segment areas. 324
325
Expression analysis 326
Total RNA was extracted from plant materials as described previously (Qüesta et al, 2016), treated with 327
TURBO DNase (Ambion) to eliminate DNA contamination, and reverse-transcribed using SuperScript 328
IV Reverse Transcriptase (Invitrogen) with gene -specific reverse primers. Quantitative PCR (qPCR) 329
analysis was conducted on a LightCycler480 II (ROCHE), and the qPCR data were normalized to the 330
Reference
genes UBC and PP2A. To measure the proximal ratio of COOLAIR, the level of the proximal 331
component was normalized to the distal COOLAIR. Primers were listed in Appendix Table S1. 332
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333
DNA−RNA hybrid immunoprecipitation followed by cDNA conversion (DRIPc) 334
The DRIP protocol is as described previously ( Xu et al, 2021) with modifications. In all, 3 g 10-day-335
old seedlings were harvested and grounded into a fine powder. The powder was suspended in 35 mL of 336
Honda buffer (20mM HEPES, 0.44M sucrose, 1.25% Ficoll, 2.5% dextran T40, 10mM MgCl 2, 0.5% 337
Triton x-100, 5 mM DTT, 1x protease inhibitor cocktail (Roche), filtered through one layer of Miracloth, 338
and centrifuged at 3500×g for 15 min. Nuclear pellets were resuspended in 1mL Honda buffer and 339
centrifuged at 8000×g for 1 min. Pellets were then resuspended in the lysis buffer (50mM Tris-HCl pH 340
8.0, 10mM EDTA, 1% SDS) supplied with 0.1 mg/mL proteinase K (AM2546, Invitrogen) and digested 341
at 55 °C overnight with gentle rotation. The mixture was phenol/chloroform extracted, followed by 342
nucleic acid precipitation with NaOAc and ethanol. The nucleic acid pellet was dissolved in water and 343
quantified with Qubit DNA quantification kit (Invitrogen). In general, 1 μg of nucleic acid was digested 344
by restriction enzymes including DdeI, NdeI and XbaI (NEB) overnight. The digested nucleic acid was 345
phenol/chloroform extracted, followed by nucleic acid precipitation with NaOAc and ethanol. Then the 346
nucleic acid was treated with RNAse III (Ambion) and then extracted by phenol/chloroform and ethanol 347
precipitation. The treated nucleic acid was then diluted ten times with dilution buffer (16.7mM Tris pH 348
7.5, 167mM NaCl, 2.2mM EDTA, 0.1% Triton X-100) and 10% was stored at −20 °C as input. In all, 349
5 μg of S9.6 antibody (1:100 dilution, ENH001, Kerafast) was added, then incubated overnight at 4 °C. 350
The next day, 50 μl Protein G Agarose (Invitrogen) was added and incubated for another 2 h. The 351
immunoprecipitants were washed five times with dilution buffer and twice with TE buffer, then were 352
eluted in 100 μl elution buffer (10mM Tris pH 7.5, 2 mM EDTA, 0.2% SDS, 100 ng/μl tRNA) at 55 °C 353
for 2 hours, together with input samples. The nucleic acids were precipitated with NaOAc, isopropanol, 354
and glycogen, dissolved in water. The nucleic acid samples were then treated with treated with TURBO 355
DNase (Ambion) to eliminate DNA contamination, and reverse -transcribed using SuperScript IV 356
Reverse Transcriptase (Invitrogen) with gene-specific reverse primers. All the samples including inputs 357
were subjected to qPCR analysis via LightCycler480 II (Roche). The data were normalized to 1% of 358
input. Primers were listed in Appendix Table S1. 359
360
Quant-seq 361
The Quant -seq protocol is as described previously ( Mateo-Bonmatí et al , 2024 ). The total RNAs 362
prepared for Quant-seq underwent purification using the Qiagen RNeasy miniprep kit (74106). Lexogen 363
GmbH (Austria) conducted the library preparation, sequencing, and data analysis. Sequencing-ready 364
libraries were created from 100 ng of input RNA using a QuantSeq 3 ’ mRNA-Seq Library Prep Kit 365
REV for Illumina (015UG009V0271), following standard procedures. The RNA integrity and quality 366
of indexed libraries were assessed on a Fragment Analyzer device (Agilent Technologies) using a DNF-367
471 RNA Kit and HS -DNA assay, respectively. Library quantification was carried out using a Qubit 368
dsDNA HS assay (Thermo Fisher). 369
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A sequencing-ready pool of indexed libraries was then sequenced on an Illumina NextSeq 2000 with a 370
100-cycle cartridge, using the Custom Sequencing Primer (CSP). Verification of read quality utilized 371
FastQC version v0.11.7, and read adapter trimming employed cutadapt version 1.18 (Martin 2011). 372
Clean reads were mapped to the latest version of the Arabidopsis genome (TAIR10) using the splice -373
aware aligner STAR version 2.6.1a (Dobin et al, 2013). The raw reads have been deposited in the Short 374
Read Archive (SRA) under the reference (PRJNA1087342 and PRJNA1076161). 375
376
Electrophoretic Mobility Shift Assay 377
FCA cDNA with L304F mutation was amplified from the mutant as described in Figure EV1. 378
To generate RNA probes, dsDNA of the corresponding region was amplified through PCR (primers see 379
Appendix Table S1) with the T7/T3 phage polymerase promoter added at the 5’ end of the primer. 380
COOLAIR RNA was then generated by following a protocol provided by the MAXIscript® T7 381
Transcription Kit (Invitrogen). The resulting product was DNA digested, denatured, and separated on 382
5% TBE gel containing 8 M Urea. The band at the right size was cut out, sliced, and eluted in gel 383
extraction buffer (0.5 M NH4Ac, 1 mM EDTA, 0.2% SDS, 1xRNAsecure ™ (Invitrogen)) at 37ºC 384
overnight, followed by precipitation with isopropanol. 10 pm ol purified RNA was 3’biotinylated by 385
following the instructions provided by the RNA 3' End Biotinylation Kit (Pierce). The labelling 386
efficiency was determined to be at least 90%. For the gel shift assay, a 20 μl reaction (25 ng/μl protein, 387
2 nM probe, 250 ng/μl tRNA, 50 ng/μl heparin, 10 mM HEPES (pH 7.3), 120 mM KCL, 1 mM MgCl2, 388
1 mM DTT) was set up on ice. For the competition assay, 2x to 100x of unlabelled probe was included 389
in the reaction. The reaction with only GST was used as a negative control. The mixture was incubated 390
at room temperature for 5 min and resolved on 3.5% native TBE-acrylamide gel and transferred onto a 391
positively charged nylon membrane. The biotinylated RNA on the membrane was detected by 392
chemiluminescence according to a protocol provided with the Chemiluminescent Nucleic Acid 393
Detection Module (Pierce, 89880). Primers to generate probes were listed below. For the binding 394
reaction, 1 μg of different recombinant proteins was incubated with 2 pmol of biotinylated probe in 20 395
μL of 1× buffer containing 20 mM Tris (pH 7. 5), 100 mM NaCl, 1 0 mM MgCl 2, non-specific 396
competitors (1µg/µl heparin and 5µg tRNA) and 0.05% Triton X-100 at room temperature for 10 min. 397
The RNA -protein mixture was resolved on 6% 1× T BE acrylamide gel under 100 V for 50 min, 398
followed by electrophoretic transfer to positively charged nylon membranes (GE Healthcare). The 399
biotinylated RNA on the membrane was UV cross-linked and detected using chemiluminescent nucleic 400
acid detection following the manufacturer’s instructions (Thermo). 401
402
Acknowledgements
403
We thank Shuqin Chen and Tina Zhang for their excellent technical assistance and Hsuan Pai for her 404
artwork assistance. We also thank all members of the Dean and Howard groups. This work was 405
funded by the European Research Council Advanced Grant (EPISWITCH, 833254), Wellcome Trust 406
.CC-BY-NC 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted April 7, 2024. ; https://doi.org/10.1101/2024.04.06.588283doi: bioRxiv preprint
(210654/Z/18/Z), and the Royal Society Professorship (RP\R1\180002) to Caroline Dean, and EPSRC 407
grants (EP/T00214X/1 to C.D. and EP/T002166/1 and EP/W024063/1 to M.L). 408
409
Author contributions 410
G-J.J. and C.D. conceived the study. G -J.J., A.P.-D., R.M., Z. W., F.L. and S.G.L. performed the 411
investigation and analysed the data. G-J.J. and C.D. wrote the manuscript; all authors reviewed and 412
edited the manuscript. M.C.L. and C.D. supervised the study, acquired the funding, and were the project 413
administrators. 414
415
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558
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Figure 1. Super-resolution and single-particle tracking characterize physical properties
of FCA condensates
A SlimVar microscopy of FCA-mScarlet-I (in magenta) in Arabidopsis root cells. Scale bar, 2
µm.
B Distributions of stoichiometry (molecule number) of individual FCA particles.
C Periodicity of FCA particle stoichiometry estimated from the most common spacing
between neighboring peaks in each stoichiometry distribution.
D The diffusion coefficient and stoichiometry of each FCA particles.
The single-particle tracking analysis is from 3 biologically independent experiments. Results
from individual replicate are provided in Appendix Figure S1.
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Figure 2. The co-localization of FCA and FLL2 is primarily observed in a limited
number of prominent foci in Arabidopsis
A Representative 3D images of FCA and FLL2 colocalization. The FCA were identified and
labelled in green and FLL2 labelled in magenta using Vision4D software. White labelling
indicates the co-localization of FCA with FLL2. The enlarged images of co-localized foci
were shown in insets at the bottom right corner. Scale bars, 1 μm.
B Quantification of size of identified FCA, FLL2 and co-localized foci. The lines in the violin
plots indicate the median and quartiles. ns, no significance.
C Size and frequency distribution of FCA, FLL2 and co-localized foci.
D Number of FCA, FLL2 or co-localized foci in each nuclei. The lines in the violin plots
indicate the median and quartiles. Non-parametric Brunner-Munzel test.
The quantitative analysis is based on 18 nuclei from 5 independent samples in 1
representative replicate. The labeled P-value was analyzed using the non-parametric
Brunner-Munzel test.
FCA FLL2
FCA
∩ FLL2
0
10
20
30foci number/nucleus
FCA FLL2
FCA
∩ FLL2
0.00
0.05
0.10
0.15Volume (µm3)
A FLL2-eYFP FCA-mTurquoise
Merge Foci identification
C
B
D
0.0001
0.0009
ns
ns
0.00 0.05 0.10 0.15
0
10
20
30
40
Vollume (µm3)
% Frequency
FCA
FLL2
FCA ∩ FLL2
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Figure 3. The RNA-binding activity of FCA modulates FCA condensates
A Representative Airyscan confocal images of wild type FCA fused mScarlet-I (FCAwt) and
FCA with L304F mutation (FCArrm). Scale bars, 5 μm.
B Quantification of size and number of FCAwt and FCArrm condensates using Vision4D
software. The lines in the violin plots indicate the median and quartiles. The quantitative
analysis is based on 43 FCAwt nuclei and 65 FCArrm nuclei from 3 independent
experiments.
C Distributions of stoichiometry of individual FCAwt (in black) and FCArrm (in red) particles.
D The diffusion coefficient and stoichiometry of each FCAwt (in black) and FCArrm (in red)
particles.
E Statistic analysis of stoichiometry and diffusion coefficient of FCAwt and FCArrm particles.
F Periodicity of FCAwt (in black) and FCArrm (in red) particle stoichiometry.
The single-particle tracking analysis is from 3 biologically independent experiments. The
FCAwt data corresponds to that shown in Figure 1. The labeled P-value was analyzed using
the non-parametric Brunner-Munzel test. Results from individual replicate are provided in
Appendix Figure S1 and S3.
FCAwt FCArrm
0
2
4
6
8
10
foci number/nucleus
0.0342
FCAwt FCArrm
0.0
0.1
0.2
0.3
0.0135
Volume (µm3)
0.0066
0.0026 0.0093
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Leaf number
Col-0FCA
WT
FCA
rrmfca-9
0
10
20
30
40
<0.0001
Col-0FCA
rrm fca-9
0.0
0.5
1.0
1.5
Proximal: distal ratio (/Col-0)
<0.0001
Col-0FCA
WT
FCA
rrmfca-9
0
10
20
30
Relative expression level
(/UBC/Col-0)
0.0006
4000 4500 5000 5500 6000
0
1
2
3
4
5
Distance from FLC TSS (bp)
DRIPc-qPCR (/Input)
Col-0
fca-9
FCAwt
FCArrm
FloweringA B
D
Spliced FLC
FCA
FCAwt
FCArrm
Col-0
fca-9
proximal
E F
distal
A B
C
D
E
C
Quant-seq read number
100
10
1
100
10
1
100
10
1
100
10
1
COOLAIR
proximal: distal ratio
0.0
0.2
0.4
0.6
0.8
1.0Porximal/ total
0.0002
0.0
0.2
0.4
0.6
0.8
1.0Distal/ total
0.0002
Col-0FCAwtFCArrm
fca-9
0
5
10
15Porximal/Distal
0.0057
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Figure 4. The missense mutation in the RRM of FCA only partially complements the
fca-9 mutant phenotype
A Flowering time of indicated plants grown in long-day photoperiod. Data are presented as
mean ± s.d. (n = 10).
B Expression of spliced FLC relative to UBC in the indicated plants. Data are presented as
mean ± s.d. (n = 5).
C The level of proximal isoforms of COOLAIR transcripts in the indicated plants relative to
control (FCAwt). Data are presented as mean ± s.d. (n = 4).
D DRIPc–qPCR analyzing COOLAIR R-loop in indicated plants. Data are mean ± s.d. from
one representative replicate of three biological replicates.
E Quant-seq experiment results from the FCA locus carried out on indicated seedlings. The
vertical pale gray bars highlight proximal and distal polyA sites.
F Quantification of reads corresponding to proximal and distal polyadenylated FCA
transcripts. Data are presented as mean ± s.d. (n = 3).
The labeled P-value was analyzed using the two-tailed t-test.
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