single-cell-level measurements of transcription heterogeneity of...
TRANSCRIPT
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Single-cell-level measurements of
transcription heterogeneity of highly mobile identical genes
Enrico Gratton and Paolo Annibale
Laboratory for Florescence Dynamics
University of California, Irvine
AAPM 57th Annual Meeting, Anaheim, 2015
Art by Liz Hinde
• Motivation: Spatial dynamics of proteins in the nucleus of cells
• Approach: Orbital tracking method
• System:
• Tracking a gene on the chromatin
• Detection and localization of gene dynamics
• Discussion/conclusions
Outline of the presentation
Some open questions about chromatin
The elongation rate of Polymerase II (PolII) in eukaryotes varies largely across different cell types and genes There is not yet a consensus whether intrinsic factors such as the position, local mobility or the engagement by an active molecular mechanism of a genetic locus could be the determinants of the observed heterogeneity
Approach Employing high-speed 3D fluorescence nanoimaging we resolve at the single cell level multiple, distinct regions of mRNA synthesis within a labeled transgene array This approach allows measuring the transcription kinetics as a function of time with millisecond resolution for total times of thousands of seconds We can also determine the motion of the transcribed gene and correlate the motion with transcription and with the motion of nearby genes
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3-D particle tracking in the nucleus The orbital tracking method
Valeria Levi
Valeria Levi, Qiaoqiao Ruan, Matthew Plutz, Andrew S Belmont, and Enrico Gratton. Biophys J. 2005; 89(6): 4275-85.
Department of Biological Chemistry, School of Sciences University of Buenos Aires (UBA),
Instrument setup
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angle particle
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laser orbit
Principle of particle tracking using the orbital scanner
• Localization precision depends on the photons collected along the orbit • Temporal resolution depends on the sampling time of the intensity along the orbit • 3D orbits in space allow 3D tracking at very high speed
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DNA
lac operator repeat
(32)
= lac repressor-EGFP
Chromatin labeling in vivo (CHO-K1)
C6-14
2 mm
Belmont et al.
cell nucleus
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High contrast
No photobleaching
Contrast ratio 3-10
on N=39
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In a fixed cell position
is determined with a
standard deviation of
about 20 nm
Dynamics of the fluorescent spot in the context
of structures in the cell and nucleus
association with nucleolus (54%) or nuclear envelope (32%) (N=59)
corralled motion
jumps between regions of confined motion (N=30/59)
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Motion of the whole cell/nucleus ?
Bar, 2 m
DHFR-BAC cell line
multiple insertions of Lac-operator repeat
simultaneous tracking of
two particles
laser orbit
particle 1
particle 2
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jumps in 36% of the cells (N=80)
Motion of the whole cell/nucleus ?
Statistical tests: Analysis of direction/velocity
αd
d
vector
vector
J
a = 1 if g ≤ 20o (for at least 5 contiguous points) = 0 if g > 20o
g
High values of J the sequence is moving fast and in a linear path
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time (s)
random motion
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C6-14 cell
Cumulative J probability identifies correlated
movements at two locations in the same
chromosome
Uncorrelated jumps Correlated jumps
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Observation: the trajectory is not due to a “pure” diffusion process.
The MSD is not Gaussian (Levy’s statistics)
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random diffusion
MSD t
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MS
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active transport
MSD t
Local random diffusion and jumps
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jump size (nm)
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residence time (min)
Statistics of jump size and residence time
Distribution maximum is 120nm Distribution maximum is 40s
Statistical tests: Analysis of instantaneous
velocity (not MSD!)
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87 % of points in jumps are blue (N=23)
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velocity (nm/s)
threshold
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Jumps in the trajectories are ATP dependent
the jumps are ATP and
temperature dependent
during the steps the DNA
sequence moves “linearly”
Experimental tests
Strategy
Statistical tests
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control azide + deoxy-glucose
No jumps (N = 30)
ATP depletion
Open questions about chromatin
Variability of elongation of Polymerase II (PolII) across different cell types and genes Intrinsic factors such as the position, local mobility or the engagement by an active molecular mechanism of a genetic locus could be the determinants of the observed variability
Approach High-speed 3D fluorescence nanoimaging can resolve at the single cell level multiple, distinct regions of mRNA synthesis within a transgene array We can measure kinetics of transcription with millisecond resolution for total times of thousands of seconds We can also observe the motion of the transcribed gene and correlate the motion with transcription and with the motion of nearby genes
terminator 1 kb
3D Tracking of a DNA Locus During Transcription
910 nm excitation 488 nm and 561 nm excitation
mRNA (MS2-EGFP)
CFP reporter 1 kb 24x MS2 repeats 1.3 kb
PolII
promoter
256x Lac op 10 kb
U2OS 2-6-3 Cell line is a courtesy of Dr. Robert Singer (Albert Einstein College, New York) and Dr. Xavier Darzacq (ENS,Paris)
Adapted from Janicki et al., Cell 2004
Lac repressor mCherry
MS2-EGFP
orbit
Paolo Annibale
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3D Motion of the center of mass of the gene
The resolution of the gene location in 3D is 10 nm, enough to establish distances among genes
Time evolution of the fluorescence intensity in the green channel (MS2) along the orbit
Each loci has a different dynamics even if the same transcript is being produced at the same time. Some loci are persistently more active than others during times of 1600s
Photobleaching recovery of one individual loci of gene expression
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tau = 5.8 ± 0.4 s
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+Dox +Dox
+Actinomycin D
Cell with a single gene
Induction of expression with different treatments and at different time
The loci respond to
expression regulators
A cell line with a single copy
of the gene has very similar
behavior than the cell with
many genes
one loop= 60 bp = 60 steps with kstep
24 stem loops = 24 steps with keff
kstep
keff
kinit
krelease
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F th
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kpause
Darzacq 2007 Larson 2011
Comparison of experimental and theoretical expectations according to proposed models
Elongation rate statistics from different loci and different cells
Cell variance of average elongation rate
Petal variance of elongation rate
Effect of activators and inhibitors of transcription
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Elongation rate is loci dependent
Color coded average rate of elongation for different petals Black dashed lines: experimental MSD of the petals. Orange line: average of experimental MSD. Red line: simulated MSD for a wormlike chromatin fiber at equilibrium. Most MSD traces display crossover between a t0.75 rigid rod regime for time scales <5-10 s (dotted orange line) to t0.25-0.5 (dashed-dotted blue and green lines) regime characteristic of entangled fibers between approximately 10-100 s. Scatter plot of confinement radius Rmax .
Simulated trace of intensity fluctuations and angular displacement of a petal A peak in the cross-correlation function is present only if there is a predominant directional motion. Binary map of cross-correlation of the fluorescence intensity and the angular displacement of the petals, calculated in 128 s time bins. Each line corresponds to a different experiment, and the sign of the cross-correlation amplitude is arranged in order to display negative values first.
Correlation between angle and intensity
Spatial pair cross-correlation at points along the orbit using a tri-fold trajectory
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Model of transcription and mRNA export from multimer copies of the same locus within a transgene array
Conclusions
•We followed a loci of gene transcription with nanometer spatial resolution and millisecond time resolution for 1000’s of seconds
•In a large transgene array only few sites of elongation occur
•A gene with active RNA synthesis has a spatial dynamics correlated to the RNA elongation and release
•The specific rate of transcription varies between identical genes in the same cell and at the same time
•RNA transcripts follow specific trajectories after release which imply the presence of topological barriers
•Our observations point out to a loci dependent regulation of gene expression
Thank you
Valeria Levi Paolo Annibale
lfd
NIH-P41-GM103540 NIH-P50-GM076516 LH