Inheritable cell-states shape drug-persister correlations and1
population dynamics in cancer cells2
Anton Iyer1, Adri´ an E. Granada2 and Shaon Chakrabarti 1,*
1Simons Centre for the Study of Living Machines, National Centre for
Biological Sciences, Bangalore
2 Charit´ e Comprehensive Cancer Center, Berlin
*Email for correspondence:
[email protected]
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Abstract4
Drug tolerant persisters (DTPs) drive cancer therapy resistance by temporarily evading drug action,5
allowing multiple routes to eventual permanent resistance. Despite clear evidence for DTPs, the6
timing of their emergence, proliferative nature, and how their population dynamics arise from mea-7
sured single-cell kinetics remain poorly understood. Here we use time-lapse microscopy data from8
two cancer cell lines, integrating single-cell and population measurements, to develop a quantitative9
description of drug persistence. Contrary to the expectation that increasing levels of genotoxic stress10
should lead to slower times to division and faster times to death, we observe minor changes in the11
single-cell intermitotic and death time distributions upon increasing cisplatin concentration. Yet,12
population decay rates increase 3-fold, suggesting a surprising independence of the overall dynamics13
from the measured birth and death rates. To explain this phenomenon, we argue that the observed14
lineage correlations and concentration-dependent decay rates imply cell-state dependent fate choices15
made both pre and post-cisplatin as opposed to just post-drug birth/death rate-based competitive16
fate choices. We demonstrate that these cell-states, present in the ancestors of DTP and sensi-17
tive cells, exhibit no difference in cycling speed and are inherited across 2-3 cellular generations. A18
stochastic model implementing these rules simultaneously recapitulates the observed decay rates and19
cell-fate correlations, also explaining how pre-drug fate decisions are consistent with barcoding ex-20
periments where barcode diversity remains unchanged after drug administration. Our results provide21
a powerful perspective on drug tolerance based on general arguments, without requiring knowledge22
of the underlying molecular architecture of the heterogeneous cell states.23
Introduction24
Non-genetic heterogeneity amongst isogenic cells gives rise to drug-tolerant persisters or “DTP”s –25
cells that temporarily survive drug treatment, often providing a reservoir for future genetic changes26
driving permanent resistance [1, 2, 3, 4, 5, 6, 7, 8]. Originally discovered in the context of bacterial-27
cell survival in the presence of antibiotics [9], the existence of persisters was later suggested for cancer28
as well, where a fractional-killing effect was demonstrated to limit curability in leukemia [10]. A large29
body of literature has since accumulated, suggesting interesting parallels between the phenomenon30
of persistence in bacterial and cancer cells, including a characteristic bi-phasic exponential decay in31
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the population dynamics after drug administration and the origin of persisters from a small fraction32
of quiescent or slow-cycling cells in drug-naive conditions [8, 11, 12, 13, 14]. Furthermore, there33
seems to be no unique non-genetic cell-state that gives rise to persistence either in bacteria or in34
cancer cells – a wide range of regulatory networks such as metabolic, extra-cellular matrix and EMT35
pathways are likely involved depending on the specifics of the cell-type, the drug being administered36
and cellular interactions with the micro-environment.37
While there have been a lot of recent advances in characterizing DTP’s and their origins, many38
questions remain unresolved and debated, particularly in the context of cancer drug tolerance [15].39
For instance, the timing of cellular decisions leading to DTPs remains unclear. Based on end-fate40
(survival or death) correlations on lineages, some previous studies concluded that heterogeneous41
cell states existing before drug administration (“pre-DTPs”) pre-determine cell fate outcomes post42
drug treatment [2, 16, 17, 18]. Conceptually similar conclusions were later drawn from elegant43
barcoding techniques that additionally gave insights into the gene expression states that might44
determine these pre-DTP states [19, 20, 21]. It was also demonstrated using theoretical models of45
transcriptional bursting that it is indeed possible to generate rare cell-states where fluctuations in46
gene expression persist for a few generations, leading to cell survival in the face of drug treatment [22].47
However, other studies have argued that fate decisions are drug-induced by combining mathematical48
modeling of cancer population dynamics, modified Luria-Delbruck fluctuation tests and barcoding49
approaches [23, 7, 24]. Similarly, the question of whether persister cells always arise from lineages50
with intrinsically slower division kinetics remains debated. Original studies in bacteria attributed51
persisters to the presence of slowly cycling sub-populations in drug naive conditions[12, 13]. Most52
studies in cancer cells have also suggested the same phenomenon, resulting in the terms “cancer53
persisters” and “quiescence/dormant” being used almost interchangeably [25, 26]. These studies54
suggest the presence of a fitness cost to non-genetic persistence in the same vein as is often ascribed55
to genetic resistance mechanisms [27]. However, emerging evidence suggests that the ancestors of56
cancer persisters before drug treatment might also be proficient in cell-division, therefore challenging57
the wide-spread notion that drug tolerant persisters necessarily emerge from quiescent subpopulations58
of cancer cells[20, 28, 29].59
In this study we explore the nature, timing and kinetics of these cell fate decisions by investigating60
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how the observed population dynamics of cancer cells quantitatively emerges from the measured61
single-cell kinetics. Integrating single-cell and population dynamics measurements from time-lapse62
microscopy datasets, we first demonstrate the surprising result that increasing cisplatin concentration63
does not affect cellular birth or death rates, unlike what is widely assumed [30, 31, 32, 33, 34, 35]. As64
a consequence, the ubiquitous exponential growth models which assume stochastic competition of cell65
fates (birth-death process and age-structured population models), fail to explain experimental data66
from two cisplatin-treated cell types, HCT116 and U2OS. Instead, we argue based on observed lineage67
correlations that pre-existing cell states largely determine fate decisions, and are inherited across68
multiple cellular generations before drug addition. However, some degree of fate determination must69
also occur during the time of drug administration, which is necessary to explain drug concentration-70
dependent effects on the population dynamics. Furthermore, we demonstrate that cells in states that71
are primed for death or survival do not have fitness differences, and are both inherited across 2-372
generations before the drug is administered. Finally, we show how early fate decisions are consistent73
with recent barcoding experiments where no change in barcode diversity was observed after drug74
administration. Our arguments are based on general principles independent of the molecular details75
of the underlying cellular states, providing a powerful approach to deciphering the dynamics of drug76
persistence in cancer.77
Methods78
Mixture models to investigate the presence of multiple cellular popula-79
tions before cisplatin, with different cycling kinetics.80
While full lineages were tracked in the HCT116 dataset [18], only one cell per sister-pair was tracked81
in the U2OS dataset [36]. Hence for the latter, we resorted to using a mixture model to check whether82
multiple subpopulations with distinct proliferation rates could be identified from the pre-cisplatin83
cells. Since previous work has identified the Exponentially Modified Gaussian (EMG) as a good84
model of the IMT distribution [18], we used a mixture of EMGs for this purpose. The EMG is a85
convolution of an exponential and Gaussian distributions, the former parameterized by λ and the86
latter by µ and σ. We used a mixture of two EMGs to fit the IMT distribution data and compared87
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with the fit to a single EMG using the Akaike Information Criterion (AIC). Details of the likelihood88
function and inferred parameters can be found in SI Section 3.89
Predicting population dynamics from single-cell measurements.90
Age structured population growth models link the net proliferation rate of the population to single-91
cell division and death time distributions [37, 38, 39, 40]. They relate the exponential proliferation92
rate of the population to the age dependent division and death rates (hazards) via the Euler-Lotka93
equation:94
1 =
ˆ ∞
0
ϕ(x)e−γxdx, (1)
where ϕ(x) = b(x)e−
´ x
0 hnet(y)dy, hnet(y) = b(y) + µ(y) is the net hazard, and b(y) and µ(y) are95
the age dependent birth and death hazards respectively. γ is the unique root to Equation 1 that96
gives the population growth rate. The hazard functions are time-dependent generalizations of the97
rate parameter in exponential distributions. The parameters of the birth and death hazards can be98
inferred from the experimentally measured single-cell inter-mitotic time (IMT) and apoptosis time99
(AT) distributions respectively. These can then be used to solve the integral Equation 1 to obtain100
the population growth/decay rate γ. Detailed descriptions of parameter inference and calculation of101
the hazard and proliferation rates are provided in SI section 8.102
Stochastic simulations of age-structured population dynamics – Model103
M0.104
Model M0 corresponds to the conventional age-structured model of population dynamics which105
generalizes constant division and death rates to age-dependent rates, giving rise to exponential106
growth at long times. Stochastic simulations of this model were performed in R for both pre-drug107
(only division) and post-drug (division and death) scenarios[38]. Single-cell distributions of division108
and death times were taken from the experimental datasets and converted to age-dependent birth109
and death rates (hazards; see SI section 8 for details). Each new cell in a lineage was assigned an age110
0 at birth and for each following time-step, the probabilities of dividing versus nothing happening (or111
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dividing, dying or nothing happening after drug) were computed based on the birth and death rates.112
This tracking was done for each extant cell. At each division event, two new cells were stored as113
nodes in the extant cells list and the graph that was uniquely defined for each lineage tree. Attributes114
like ‘birth time’, ‘state’, ‘fate’, etc. were stored in these newly created nodes for future reference.115
Further details can be found in SI Section 9.116
Competing risks analysis of exponentially distributed division and death117
time distributions.118
Since cells exposed to cisplatin can undergo either division or death, these events are mutually119
exclusive and hence give rise to ‘competing risks’ for each cell. A well known problem in statistics,120
the competing risks effect leads to significant biases in the experimentally measured times to division121
and death after cisplatin addition [18]. Since only the event with a shorter time will ultimately122
be observed for any single-cell, all the measured division and death times will be biased towards123
lower values, thereby hiding the actual underlying distributions of division and death times. These124
underlying distributions therefore are not directly measurable, but need to be inferred from the125
measured biased division and death times. A simple analytical calculation using exponential waiting126
times for the birth and death events illustrates the competing risks problem, and demonstrates how127
inference of the underlying distributions can be carried out (see SI Section 7 for details).128
A Markov Chain Monte Carlo approach to competing risks analysis for129
HCT116 and U2OS cells.130
While exponential distributions allow for an analytical solution of the competing risks inference prob-131
lem, non-exponential distributions along with the pre and post-drug scenarios in the HCT116/U2OS132
experiments complicate the inference problem and preclude analytic solutions. For the post-drug133
scenario we needed to find the underlying distributions of IMT and AT as mentioned in the com-134
peting risks section, which are modeled as EMGs having three parameters each ( µ, σ and λ). We135
performed the inference of these distributions from the biased IMT and AT values obtained from136
the experiment using a Metropolis-Hastings Markov Chain Monte Carlo approach. In this method137
we sampled a total of 8 parameters from their posteriors. Six of these parameters describe the two138
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distributions, IMT and AT (µ, σ and λ for each distribution). The remaining 2 parameters describe139
the probability of the cell to enter a quiescent stage and the delay time for the drug to act. To find140
the posteriors of these parameters, we formulated likelihoods for all the division and death events141
that are possible post-drug and assumed a uniform prior to obtain the posterior using Metropolis142
Hastings MCMC. Details of the inference method are provided in SI section 8 .143
Beyond age-structured populations: stochastic simulations of Models144
M1, M2 and M3.145
Model M1 : In Model M1, we defined the cells to exist in one of two states, one being more susceptible146
to die (sensitive, S’) while the other is more likely to persist (pre-DTP, P’) in the face of drug147
treatment. The cells were allowed to interconvert between these states in drug naive conditions.148
Post cisplatin, sensitive cells and pre-DTP cells were assigned fates to die and divide respectively.149
The times taken for the division or death events were sampled from the respective distributions150
measured in the experiments. This model could recapitulate the experimentally observed lineage151
correlations, but not the drug-concentration dependent decay rates.152
Model M2 : In this model, the cells possessed no ‘states’ before cisplatin so that on its administration,153
the cells were randomly assigned fates with probabilities that depended on drug concentration. While154
this model could explain the population decay rates observed in the experiment, it failed in explaining155
the correlations seen in the final post-cisplatin fates of lineage related cells.156
Model M3 : This model is essentially a combination of Models M1 and M2, where we simulated cells157
in two states S’ (sensitive) and P’ (pre-DTP) prior to drug addition with inter-state transitions.158
After the drug, the cells were assigned fates from 3 possibilities – death, survival or division, with159
probabilities conditioned on their state at the time of drug treatment. The state-dependent fate160
probabilities were chosen from a fate-matrix F. If a cell was assigned ‘division’ as the fate, the two161
resultant daughters maintained the original state of the mother cell at time of drug addition, and162
the fate assignment process was repeated using the same matrix F. This model could quantitatively163
recapitulate both the lineage correlations as well as the drug concentration dependent decay rates164
measured in the experiments. Further details are provided in SI Sections 9 and 10.165
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Results166
Subpopulations with distinct proliferation rates cannot be detected in167
HCT116 or U2OS cells.168
To obtain accurate single-cell intermitotic times (IMTs), apoptosis times (ATs) and cell lineages, we169
obtained datasets from two previous studies on colon cancer HCT116 [18] (Fig. 1a-c) and osteosar-170
coma U2OS [36] (Fig. 1d-f) cell lines. These studies performed five days of single-cell time lapse171
microscopy, tracking cells in two days of drug-free medium followed by three days of cisplatin treat-172
ment, with snapshots taken every 30 mins. While HCT116 were exposed to a single concentration of173
cisplatin approximately near its IC50 value [18], U2OS cells were treated with four concentrations of174
cisplatin, 0, 7, 10 and 13 µM corresponding to Control, Low, Medium and High labels [36]. Besides175
measurements of IMT and AT of single cells, these datasets allow simultaneous extraction of the176
population dynamics by counting the number of surviving cells in each time frame. Furthermore,177
the HCT116 dataset also provides information on lineage relationships between the various single178
cells. In both datasets there were a small fraction of cells which never divided from the beginning of179
tracking, and which did not show any bias towards end fate (survival or death post cisplatin). We180
excluded these cells from all further analysis. SI Section 1 provides further details of both datasets,181
number of cells included/excluded and the fraction of end-fates observed.182
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Figure 1: Pre-cisplatin heterogeneity in inter-mitotic times arises from a single population of cycling
cells. (a) HCT116 tracking records the trajectories of all lineages. The dashed vertical line shows
time of administration of cisplatin. Blue lines track back to ancestors of surviving (persister) cells
while the red lines track back to ancestors of cells that die (sensitive cells). (b) log of population
versus time for HCT116 cells show a distinct bi-phasic exponential decay after cisplatin (denoted
by the vertical line). (c) Boxplot comparing IMTs of distinct drug naive ancestor cells belonging to
lineages of persister or sensitive phenotypes. (d) U2OS tracking records the trajectories of a randomly
chosen daughter cell (forward lineages). (e) log of population versus time for U2OS cells with three
different cisplatin concentrations. The biphasic decay observed in panel (b) is not observed here.
(f) Pre-cisplatin single-cell IMT distribution is better explained with a single EMG (Exponentially
Modified Gaussian) model than a mixture of 2 EMGs as verified by comparing AIC values for the
two models.
We first asked whether distinct sub-populations of slowly dividing cells could be detected in the183
drug naive HCT116 and U2OS cells. The HCT116 dataset had both the daughter cells of dividing184
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cells tracked (Fig. 1a) allowing extraction of single-cell times and cell fates for all the cells in185
the population. To find the population-time curve (Fig. 1b), we summed the number of cells186
in each time frame. Starting with a population of 65 cells, the semi-log plot of the curve shows187
characteristic exponential growth before the addition of the drug (vertical line in Fig. 1b) and a188
bi-phasic exponential decay after cisplatin exposure. The first larger decay rate switches to a plateau189
after the 100th hour of the experiment, driven by the drug tolerant persisters in the population. We190
identified persisters as those cells surviving till the end of the experiment (resulting in the second191
phase of exponential population decay) and extracted the IMTs of their drug-naive ancestors by192
tracking back in time along their lineages (Fig. 1a, blue line). We compared these drug-naive193
ancestor IMTs to those of the sensitive cells that died after cisplatin treatment (Fig. 1a, red line),194
and could not detect any statistically significant difference between these two distributions (Fig. 1c;195
see SI section 3 for details).196
The U2OS dataset was generated by tracking a single randomly chosen daughter after each cell197
division (Fig. 1d; starting population ∼7 cells per field of view). The population-time curves,198
calculated by averaging over the number of cells across 51 fields of view per time frame, showed a199
characteristic exponential growth before cisplatin addition and concentration-dependent exponential200
decay post cisplatin exposure (Fig. 1e). However, five days of tracking was not sufficient to observe201
the second slower exponential decay unlike in the HCT116 cells. Therefore to investigate whether202
multiple sub-populations with distinct IMT distributions exist pre-cisplatin, we resorted to fitting the203
data with a mixture model (see SI section 3 for details). We thus compared the ability of single and204
two-component Exponentially Modified Gaussian (EMG) models to explain the IMT distribution205
of drug naive cells, using the Akaike Information Criterion (AIC). We found that the single EMG206
(AIC = 3687.4) fared better than the mixture model (AIC = 4137.649). Also, the two models207
generated best fit distributions that were essentially indistinguishable, suggesting the absence of208
multiple sub-populations with distinct proliferation rates within the U2OS population as well (Fig.209
1f).210
In summary, our analysis demonstrates that in both HCT116 and U2OS cell types, the heterogeneity211
in cell cycle times before addition of cisplatin is best explained by a single population of cycling cells,212
not by multiple sub-populations with distinctly different cycling kinetics. This suggests that if a pre-213
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DTP state exists amongst these cells before drug administration, it does not have any fitness cost214
as compared to the sensitive cell state.215
Proliferation rate of cancer cells can be predicted from single-cell division216
times.217
Having established that a single IMT distribution best explains the datasets before cisplatin treat-218
ment, we next asked how accurately this IMT distribution can predict the population growth rates.219
For exponentially proliferating cells, the population growth rate is approximately given by the inverse220
of the mean of the IMT distribution. While this is the most popular model used to describe expo-221
nential cellular growth, the underlying assumption here is that the IMT distribution is exponential.222
However, this is clearly not true in our datasets (Fig. 1f) and hence a more general approach is223
required. An age-structured population model (Model M0 ; see Methods and SI section 9 for details)224
is a generalization of the simple exponential growth models, that allows for non-exponential IMT225
distributions, and connects the population growth rate to the full IMT distribution via the Euler-226
Lotka equation (see Methods and SI section 4 for more details)[38, 41, 37, 40]. From the measured227
single-cell IMTs we estimated the predicted population growth rates from both the inverse of the228
mean as well as the Euler-Lotka equation, and compared them with the true growth rate – the linear229
regression slope of the semi log plot of number of cells as a function of time (Table 1).230
For the HCT116 cells, we found that the inverse of the mean gave an error of around 62%, while the231
Euler-Lotka estimate gave a much reduced error of 13% (Table 1 and Fig. 2a). The large error in the232
former model was not surprising as the measured IMT distribution was neither exponential nor very233
narrow to be effectively represented by the mean. For the latter result, we further investigated the234
potential origins of the 13% error. To check whether this error could arise simply due to the small235
number of cells in our experiments, we performed stochastic simulations taking the measured IMT236
distribution as input to generate in silico proliferation trajectories with similar cell numbers.237
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Figure 2: An age-structured model accurately predicts population growth rates from single-cell IMT
distributions. (a)-(c) are plots for HCT116, (d)-(f) are for U2OS. (a) Semi-log plot of population
versus time curve of HCT116 cells before cisplatin administration. Predicted growth rate using
inverse of the mean (pink line; error = 62%) and the Euler-Lotka equation (blue line; error = 13%)
are compared with the experimental data shown as black dots. (b) Maximum Likelihood inference of
the age distribution of ancestor cells immediately after seeding. (c) Distribution of errors in Euler-
Lotka predictions of growth rate, obtained by running 500 iterations of an age-structured population
simulation with initial age distribution taken from panel (b). Vertical dashed line represents the
Euler-Lotka prediction error in experimental data (corresponding to error of the blue line in panel
(a)). (d) Semi-log plot of population versus time curve of U2OS cells before cisplatin, with colours
as in panel (a). Predicted growth rate using inverse of the mean (pink line; error = 73%) and the
Euler-Lotka equation (blue line; error = 22%) are compared to the experimental data shown in
black dots. (e) Inferred age distribution of seeded population of U2OS cells, as in panel (b). (f)
Distribution of errors in Euler-Lotka estimates, obtained by running 500 iterations of simulations as
in panel (c). Initial age distribution was taken from panel (e) for these simulations. Vertical dashed
line represents Euler-Lotka prediction error in experimental data (corresponding to error of the blue
line in panel (d)).
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For each simulation run we calculated the growth rate prediction errors using both the growth238
rate estimates, mimicking the procedure we carried out on the experimental data. Since the age239
distribution of the cells at the initial time is an input to the simulations, and it is known that this240
distribution can affect the emergent population dynamics [38], we estimated the age distribution241
of the initial cells directly from the experimental data (Fig. 2b). Based on the IMT distribution242
of the full pre-cisplatin population, we inferred the starting ages of the initially plated cells in the243
experiment using a Maximum Likelihood approach (Fig. 2b; details in SI). We then repeated the244
simulations using the inferred initial age distribution and measured IMT distributions and found245
that the Euler-Lotka errors peaked around 2% (Fig. 2c). We carried out a similar analysis for the246
U2OS dataset, where we once again found a large error of around 73% from the inverse of the mean247
prediction, and a much reduced error of 23% from the Euler-Lotka equation (Fig. 2d). We found248
that the inferred initial age distribution of the starting U2OS cells was broader than that of the249
HCT116 cells (Fig. 2e), and when used in the simulations, could account for about 4% error in the250
growth rate prediction (Fig. 2f). The unexplained errors of about 10 − 20% for HCT116 and U2OS251
cells could be due to artefacts of the image analysis pipeline, or from other unaccounted biological252
sources such as cell-size control of the cell cycle.253
Model for growth rate prediction HCT116 U2OS
Inverse of mean IMT 62% 73%
Euler-Lotka 13% 23%
Expected Errors (Simulations) ∼ 2% ∼ 4%
Table 1: An age structured model (Euler-Lotka equation) accurately predicts population growth
rates of both HCT116 and U2OS cells before cisplatin treatment. Shown here are deviations (in %)
of growth rates predicted by either the Euler-Lotka equation or the inverse of the mean IMT, from
the experimentally measured growth rate (obtained via linear regression of the cell-population versus
time curve in Fig. 2a,d). The growth rate prediction by the Euler-Lotka equation for HCT116 cells
is within ∼ 11% of the error expected from age-structured population simulations with the inferred
starting age-distributions. For the U2OS cells, the predictions are off by about ∼ 20%.
Our results in this section demonstrate that in the absence of cisplatin, the age-structured model254
predictions of population growth rate using a single IMT distribution is accurate to within 10 − 20%255
in both HCT116 and U2OS cell types. This provides a benchmark for the expected error level when256
trying to predict population dynamics from our single-cell datasets. Additionally, the fact that a257
single IMT distribution is sufficient to predict the population growth rate is consistent with results258
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from the previous section, which suggested the absence of sub-populations of cells with different259
cycling kinetics.260
First exponential decay of drug treated cancer cells is not established261
by single-cell division and death times262
Since the age-structured model (Model M0 ) could predict pre-cisplatin population growth rates from263
the measured cell division times within 20% error, we next asked if a similar prediction accuracy264
can be achieved in the post-cisplatin scenario, where an added dimension is cell death causing the265
populations to decay instead of grow. Throughout this section, we will be focusing only on the266
first phase of exponential decay after cisplatin treatment (for the U2OS cells the experiments were267
not long enough to observe the second exponential phase). To find the IMT and AT distributions268
for both HCT116 and U2OS cells, we extracted the times from cells that were either born before269
drug exposure but divided or died after drug exposure, or cells that were both born and reached a270
fate after drug exposure (Fig. 3a-d). For the HCT116 cells there was data from only one cisplatin271
concentration (Fig. 3a, b), but three different concentrations for U2OS cells allowed us to explore272
concentration effects on the population dynamics (Fig. 3c, d).273
Though the U2OS population decay rates were distinctly different between high (−25x10 −3h−1)274
, medium (−11.4x10 −3h−1) and low ( −7.2x10−3h−1) cisplatin, surprisingly there were negligible275
differences in the IMT and AT distributions across the three cisplatin concentrations (Figs. 3c and276
3d respectively). This directly showed, in a model-independent manner, that times to division or277
death post cisplatin (and consequently the division and death rates) do not determine the population278
decay rates. This result contradicts the widely used assumption that the effect of drugs can be well279
described either as increasing the cellular death rate or reducing the division rate [30, 31, 32, 33,280
34, 35]. To rigorously confirm that the minor differences in the measured IMT and AT distributions281
cannot explain the large differences in decay rates across cisplatin concentrations, we calculated the282
predicted rates using both inverse of the mean and Model M0 (see SI section 9 for details). The283
IMT and AT distributions were not sufficient to accurately predict the concentration-dependent284
decay rates of the U2OS cells, producing errors greater than 100% (‘Measured’ columns in Table285
2). Indeed, even for HCT116 cells where we had data from one drug concentration, the error in286
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predicted287
Figure 3: Inferring the underlying post-drug IMT and AT distributions from the experimentally
measured, biased distributions. (a)-(d) are plots of measured IMT and AT distributions of HCT116
and U2OS cells while (e)-(h) are the competing-risks corrected distributions inferred using a Markov
Chain Monte Carlo approach (see Methods and SI section 8 for details). (a)-(b) IMT and AT distri-
butions of HCT116 cells. All cells that divided or died during the treatment period were tracked and
measured, including cells that were born before and after cisplatin addition. (c)-(d) Forward lineage
distributions for U2OS cells that have division and death events that occurred during the treatment
period. The three distributions in both panels (c) and (d) are almost identical, demonstrating that
increasing drug concentration does not affect division or death rates post cisplatin. (e) Inferred IMT
distribution of HCT116 cells. Compared to panel (a), the long tail is evident demonstrating the
significant bias in the measured distribution. (f) Inferred AT distribution of HCT116 cells, which
is similar to the measured distribution in panel (b). (g) Inferred IMT distributions for U2OS cells
reveal increasingly long tails for increasing cisplatin concentrations. (h) Similar to panel (f), the
inferred AT distributions for U2OS cells is almost identical to the measured AT distributions.
population decay rates was greater than 100% (‘Measured’ column in Table 2). Taken together, these288
findings were remarkably surprising in light of our previous section results as well as the vast body289
of literature modeling population growth/decay as the difference in birth and death rates.290
We therefore wondered if our analysis using the measured IMT and AT distributions suffered from a291
competing-risks bias, a statistical effect that prevents direct measurement of the correct underlying292
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distributions when the events are mutually exclusive. We have previously demonstrated that this293
effect leads to strong biases in the IMT and AT distributions measured after drug treatment [18],294
and hence can potentially lead to erroneous population growth rate predictions. A simple analytic295
calculation for exponentially distributed IMT and AT is presented in SI section 7 that provides296
intuition for this competing risks effect, and how it can be corrected using inference techniques.297
In the more complex case of non-exponentially distributed IMT and AT as is the case with the298
HCT116 and U2OS datasets, we used a Markov Chain Monte Carlo (MCMC) approach to infer299
the parameters of the unobserved distributions (see SI section 8 for details). The inferred IMT300
distributions of HCT116 cells (Fig. 3e) showed a significant right skew (slower division times)301
compared to the measured IMT distribution, which was not observed for the AT distribution (Fig.302
3f). For the U2OS cells, the degree of right skewness in the inferred IMT distributions increased with303
higher drug concentrations (Fig. 3g) while once again the inferred AT distributions (Fig. 3h) had304
no significant skew compared to the measured AT. Using these inferred IMT and AT distributions305
we then recalculated the predicted decay rates using the mean inverse and the Eula-Lotka equation.306
While the errors significantly reduced (‘Inferred’ columns in Table 2), they were still very high with307
the smallest error around 40% in both HCT116 and U2OS and the largest error greater than 100%308
for low and medium cisplatin doses in U2OS.309
HCT116 U2OS
Measured Inferred Measured Inferred
Model Low Med High Low Med High
Mean Inverse > 100% 51.8% > 100% > 100% > 100% > 100% 85% 60.2%
Euler-Lotka > 100% 40.3% > 100% > 100% > 100% > 100% > 100% 40.3%
Table 2: Age structured models fail to predict population decay rates for cells treated with cis-
platin. Shown here are deviations (in %) of the predicted decay rates from the measured decay rates
(obtained via linear regression of post-cisplatin experimental data in Fig. 1b,e). Predictions were
made using IMT and AT distributions obtained directly from the experiment (‘Measured’) and from
competing risks-corrected unbiased distributions (‘Inferred’).
In summary, we found that estimates of population decay rate using measured single-cell times to310
division and death post cisplatin treatment were erroneous by over 100%, predicting positive growth311
instead of decay. Even after correcting for competing risk biases, the population decay rates could312
be predicted at best with an error of 40%, often with errors as high as 100%. These counter-intuitive313
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results suggest that measured single-cell IMT and AT are not sufficient to estimate population decay314
rates post addition of cisplatin. In turn these results suggest that post-drug stochastic competition315
of cell fates inherent to these exponential growth models (Model M0 ), is likely to be an incorrect316
model of cell-fate decisions in the development of cancer drug persistence.317
Cell-state inheritance along with fate decisions before and during drug318
treatment control cancer population dynamics.319
We next asked if the nature and timing of fate decisions can be determined by developing a series320
of models with varying assumptions and checking for compatibility with experimental data. The321
deviations from Model M0 predictions of decay rates suggest that the cell fates are likely decided322
either during or before drug addition, largely independent of the single-cell times. Therefore we323
developed three alternate models of the fate decision process, Models M1, M2 and M3 (Fig. 4a).324
In these models, cell fates are either (i) determined based on 2 cell-states before drug – a pre-DTP325
state P’ that is more likely to survive and generate persisters, and a sensitive state S’ that is more326
likely to lead to cell death after drug administration (M1 ), (ii) decided randomly at the time of drug327
addition with probabilities that depend on the drug concentration (M2 ), or (iii) a combination of328
both M1 and M2 where pre-existing cell-states determine the end fate with large probability while329
the drug concentration modulates this probability to some extent ( M3 ). Inter-conversion between330
states S’ and P’ in Models M1 and M3 is modeled using a Markov Chain described by a transition331
matrix T while the drug concentration-dependent fate probabilities in Model M3 are imposed using332
a fate matrix F. Further details and parameterizations of each model are provided in Methods and333
SI Sections 9 and 10.334
Interestingly, we found that though Models M1 and M2 could recapitulate certain aspects of the335
experimental datasets (see SI section 9 for details), only Model M3 could quantitatively explain all336
three major observations simultaneously: (1) decay rate for a fixed drug concentration,337
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Figure 4: A two state Markov model with state-dependent fates (Model M3 ) quantitatively ex-
plains the experimentally measured decay rate and correlations in lineage related HCT116 cells. (a)
Schematics of models M0 to M3. Cells in gray indicate no role of cell-states in determination of fate.
Coloured cells indicate pre-existing cell-states that pre-determine final fates to a large extent. The
dice indicates probabilistic fate assignment at the time of drug administration. (b) Lineage corre-
lations in fates of HCT116 cells measured from time lapse experiments. Correlations exist for first
and second cousins (FC and SC), while third cousins (TC) are similar to randomly selected pairs of
non-lineage related cells (horizontal dashed line). (c) An example run of Model M3 showing the rel-
ative populations of the two states as a function of time before drug administration. (d) Population
versus time trajectories from simulations of Model M3 using identical IMT and AT distributions, a
fixed Transition matrix T, but different Fate matrices. Each colour corresponds to simulations with
a different F. (e) Same as panel (d), but with different Transition matrices for a fixed Fate matrix F.
(f) Distribution of decay rates from the simulations (red histogram). The vertical dashed line is the
decay rate obtained from the HCT116 experimental dataset. (g) Comparison of lineage correlations
obtained from the HCT116 experiment (red) with simulations of Model M3 (blue). Transition rates
used in the simulation were symmetric for transition between the two states, 9 × 10−3 per hour. The
fate probabilities for cells to die, divide and stay alive for the two states were: Sensitive state S’ =
(0.9125, 0.05, 0.0375); pre-DTP state P’ = (0.35, 0.1, 0.55).
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(2) lineage correlations in end-fate and (3) drug concentration dependence of the population decay338
rates. On simulating M3, we noticed that a broad spectrum of effective decay rates could be obtained339
after cisplatin exposure even with the IMT and AT distributions fixed. This arises either due340
to different Fate matrices for a given Transition matrix (Fig. 4d) or due to different Transition341
matrices for a given Fate matrix (Fig. 4e). This explains the surprising results from Fig. 3c-342
d where the IMT and AT distributions were found to be insensitive to drug concentration – the343
IMT and AT distributions have little contribution towards establishing the decay rate. Rather,344
the population dynamics is dominated by the relative proportion of the two states at time of drug345
exposure (determined by T), and the entries of F. Importantly, we found that for certain physically346
realistic values of the T and F matrices, we could approximately recapitulate the experimentally347
measured decay rates (Fig. 4f) as well as the lineage correlations (Fig. 4g) while maintaining the348
same IMT and AT distributions as measured in the HCT116 experiment.349
Our analysis in this section quantitatively explains why the birth and death rates (and more generally350
the single-cell IMT, AT distributions) do not determine the decay rates of drug treated cells at351
the population level. We demonstrate that the transition rates between cell states before drug352
treatment, the ability of these states to be passed down across cellular generations, and the cisplatin353
concentration-dependent propensity of these states to result in death or survival largely determine354
the population dynamics and lineage correlations of cells after drug treatment.355
Change in barcode diversity before and after drug cannot establish timing356
of fate decisions in the presence of cell-state switching.357
Our analyses thus far demonstrated the importance of pre-existing cellular states in the population358
that leads to persistence of cells in the face of cisplatin treatment. This conclusion was true for both359
colorectal cancer as well as osteosarcoma cell types. However, a recent study on colorectal cancer360
cells concluded that the persister fate arose after the addition of cisplatin, based upon analysis of361
a high-complexity barcode library that had been transduced into the cancer cells [24]. In short,362
this study found that the barcode diversity (measured by the Shannon Diversity Index) showed no363
reduction upon cisplatin treatment, which suggested that the persister fate choice was likely made364
post drug treatment. Since these results are conceptually different from our findings,365
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Figure 5: Maintenance of barcode diversity before and after drug cannot be interpreted as a signa-
ture of drug-induced cell fates. (a) Current barcoding methods relate fate determination to pre-drug
cell-states if the barcode diversity, shown here by the presence of distinct barcodes (colored circles),
significantly reduces after drug (i). However, if the diversity does not reduce then fate determina-
tion is assumed to be in response to drug exposure (ii). Our model however, suggests that both
the conditions (i & ii) can be obtained with fates largely determined before drug administration.
Simulation results show that in conditions when the cell-states before drug transition on time scales
much slower than the cell division time, barcode diversity shrinks significantly post drug treatment
(iii). However, if the transition rates are of the order of a few cell cycles or faster, more sensitive cells
transition to a pre-DTP state, resulting in insignificant change in barcode diversity post-drug (iv).
(b) Barcode abundance plot post drug treatment obtained from simulations of Model M3. Circle
fill colors represent distinct barcodes while their sizes show barcode frequency counts. Results of 3
simulations are compared. ‘Control’: simulations with cell-state independent fate assignment of cells;
‘No Trans’: simulations with cell-fate assignment conditional on cell-states that do not inter-convert;
‘SimExpt’: simulations with state dependent fate assignment with cell-state transitions allowed be-
fore drug addition. (c) Diversity of barcodes can be measured by the Shannon Diversity Index. The
boxplot here shows change in Shannon Diversity Index for the corresponding simulations described
in panel (b).
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Figure 5: (d) Variance over Mean Ratio (VMR) of persister cell counts as measured in the experiment
(Expt) and the simulation matching experimental results (SimExpt). The horizontal dashed line
shows the VMR for a Poisson distribution. (e) Comparison of Cumulative Distribution Function
(CDF) for perister cell counts obtained at the end of simulation (green) and experiment (red).
‘Poisson fit’ (blue line) is the CDF expected from a Poisson distribution of persister cell counts.
we next investigated potential reasons that may explain the apparently contradictory results.366
The barcoding approach to determine the timing of persister fate choice relies on comparing the367
barcode diversity, or abundance of unique barcodes, before and after drug exposure in many cellular368
replicates. A reduction in barcode diversity after drug treatment is interpreted as selection of a small369
set of pre-existing persister cells (Fig. 5a i). Maintenance of barcode diversity on the other hand370
suggests a scenario where persister cells arise randomly in cells after drug treatment, thereby leading371
to many surviving barcodes (Fig. 5a ii). However, these interpretations were originally derived in372
the context of genetic mutations [42] where reversal of mutations is rare. The same assumptions do373
not hold in case of non-genetic cell states (the pre-DTP state P ′ or sensitive state S′ in our case),374
and we argued in the previous sections that transitions between the two states is a fundamental375
aspect of the dynamics in both HCT116 and U2OS cell types.376
To quantitatively explore how cell-state switching before drug addition could affect interpretations377
of barcode diversity, we used Model M3 with the same parameters from the previous section, with378
the additional information of barcodes (Fig. 5a iii-iv; see SI sections 11-12 for details). In brief,379
each starting cell was given a barcode ID that was inherited by all descendants across cell divisions380
and maintained over cell-state changes. The fates were conditioned on cell-state as described before381
for Model M3. The results of the simulation are shown as an abundance bubble plot (Fig. 5b)382
for qualitative visualisation and as a Shannon Diversity Index (SDI) plot (Fig. 5c) for quantitative383
assessment of barcode enrichment or diversity. The drop in Shannon Diversity Index post drug was384
observed only when the simulation did not allow for state transitions before drug treatment, which385
is equivalent to very slow transitions compared to a typical cell cycle time (Fig. 5b-c, ‘No Trans’).386
However, if the transitions were allowed with rates that gave rise to the experimentally measured387
lineage correlations (Fig. 4g), it resulted in no change in the SDI value (Fig. 5b-c, ‘SimExpt’). This388
short analysis confirmed that the timing of development of pre-DTP states cannot be inferred using389
current barcode analysis techniques and might require development of novel methods to account for390
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cell-state transitions.391
Finally, we used an orthogonal approach to analyse the timing of fate decisions for the HCT116392
cells – a Luria-Delbruck (LD) fluctuation test. This method is based on quantifying the persister393
count distribution after cisplatin, with a Poisson distribution suggesting drug-induced persistence,394
while a super-Poisson distribution implying pre-existence of a pre-DTP state before drug addition395
[43]. The comparison is made either by calculating the Index of Dispersion (variance over mean) or396
obtaining the cumulative distribution function of the persister cell counts. We calculated the Index397
of Dispersion for HCT116 data by comparing the persister cell counts across lineage trees and found398
it to be around 4.5, which meant that the distribution of persisters was not Poissonian and that399
the persister fate originated before drug addition (see SI section 13 for details). Note that for the400
U2OS cells this analysis was not possible since the second exponential decay phase was not observed,401
precluding identification of persisters (Fig. 1e). Finally, we also checked if our simulation results402
that matched the decay rates (within 5% error; Fig. 4f) and lineage correlations (Fig. 4g) seen in the403
experiment, would give similar results. Indeed, the simulation results also showed non-Poissonian404
distributions (Fig. 5d). By comparing the CDF of the persister counts in simulation and experiment,405
we further confirmed the distribution to be non-Poissonian (Fig. 5e).406
In summary, the results in this section show that change in barcode diversity before and after drug407
treatment is not always sufficient to establish the timing of fate decisions. This is true when fates408
are related to non-genetic cell-states which inter-convert between each other on time scales similar409
to the cell-cycle time. Maintenance of barcode diversity after drug treatment is therefore consistent410
with a pre-DTP state existing before drug treatment and driving fate outcomes, as our analyses411
demonstrates using both lineage correlations as well as the Luria-Delbruck fluctuation test.412
Discussion413
In this work we demonstrate how general principles underlying the dynamics of drug persistence can414
be discovered in the process of connecting measured single-cell kinetics to the emergent population415
dynamics of cancer cells. Quite unexpectedly, the single-cell measurements directly show that in-416
creasing drug concentration does not affect the birth or death rates (Fig. 3c-d), unlike the widespread417
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assumption in the field [30, 32, 33, 34, 35]. These results suggest that stochastic competition be-418
tween fates based on drug-induced cellular birth and death rates is not the mode of decision-making419
underlying the emergence of non-genetic drug tolerance. Rather, we demonstrate that non-genetic420
cell-states existing before drug treatment largely bias the eventual fates towards drug-tolerance or421
susceptibility. These biases are further modulated at the time of addition of the drug, leading to a422
quantitative explanation of both the population dynamics as well as the lineage correlations observed423
in experimental datasets of HCT116 and U2OS cells (Fig. 4f-g). While earlier studies have discussed424
the role of pre-existent cell-state switching in cancer drug tolerance, they typically use markers of425
specific cell-states to demonstrate state-switching and emergence of drug tolerant persisters [3, 44,426
45, 46, 47]. Our work however is based on more general arguments for the existence of non-genetic427
states and transitions between them, requiring no a priori knowledge of the molecular architecture of428
the underlying states. This is particularly powerful since the molecular details of these states remain429
unknown in all generality, and are likely to comprise transcriptional, post-transcriptional as well as430
epigenetic elements. Additionally, to the best of our knowledge this work is the first to quantitatively431
explain the connection between measured single-cell kinetics and the emergent population dynamics432
of drug-treated cancer cells.433
In the widely used exponential growth models and their generalizations, the fraction of cells that die434
(establishing the first decay rate) depend entirely upon the parameters of the post-drug IMT and435
AT distributions. However, in the presence of non-genetic cellular states that pre-determine fate436
outcomes (sensitive and pre-DTP states), the fraction of cells that die no longer depends exclusively437
on the IMT and AT distributions, but also on the transition rates of these pre-existing cell states.438
Though this idea has been suggested in many previous theoretical works that typically analyze439
FACS datasets [3, 48, 49, 50, 51, 35, 52], it has not been directly demonstrated from single-cell440
measurements linking IMT and AT distributions to the population dynamics. Additionally, the idea441
that single-cell division and death kinetics may not be sufficient to predict drug-treated population442
dynamics has been suggested before in the context of lung cancer cells [53]. However, this study did443
not incorporate distributions of time to death or correct for competing-risks biases, thereby making444
it challenging to interpret the results.445
Furthermore, the implications of cell-fate lineage correlations have been poorly appreciated in the446
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context of non-genetic heterogeneity and the timing of emergence of pre-DTP states. While early447
studies on TRAIL-induced apoptosis had already suggested that lineage correlations imply early fate448
decisions[2, 17], a careful study later explored the detailed implications of correlations in apoptosis449
and their decay across sisters, cousins and higher order lineage-related cells [16]. Based on careful450
time-lapse microscopy experiments, this study separated out the effects of spatial correlations po-451
tentially arising from inter-cellular signalling from correlations arising from inheritance of cell-states,452
to argue for decisions of apoptosis taken well before addition of the drug [16]. Recently we demon-453
strated that correlations also exist in the dynamics of signaling pathways that get upregulated only454
after drug treatment (rate of p53 increase in response to cisplatin), suggesting that even if cellu-455
lar states change upon drug addition, the propensity for these changes are largely pre-programmed456
into upstream regulatory networks of the ancestor cells existing before drug addition [18]. Taken457
together with our current study, the emerging evidence points towards a scenario where cell-states458
existing well before drug addition largely determine eventual cell fates after addition of drugs. In-459
terestingly, recent tour-de-force studies using clever combinations of high-complexity barcoding and460
single-molecule FISH have arrived at broadly similar conclusions. These newer studies have also461
begun to shed light on important and previously unavailable information on the genes whose expres-462
sion states pre-determine the ultimate fate of cancer cells in response to drugs[19, 21], and further463
demonstrate that transcriptional states post long-term drug treatment may be very different from464
those that existed prior to drug exposure [28, 54].465
An intriguing implication of our results is that both the pre-DTP as well as the drug-sensitive states466
exist in cells that are actively proliferating. This suggests that DTPs need not arise exclusively467
from quiescent (also called dormant) or slowly cycling cells (such as cancer stem cells), which is468
primarily the evidence that has been reported in the literature from bacteria, mammalian cell lines,469
primary cells as well as tissues [12, 55, 56, 57, 26, 58, 59]. Importantly, our inability to find multiple470
proliferative sub-populations in either HCT116 or U2OS cells before drug treatment (Fig. 1c,f),471
combined with the fact that we could accurately predict the population growth rates from the472
measured single IMT distribution (Fig. 2c,f), demonstrates that the pre-DTP state does not have473
any fitness cost. This result is intriguing since a fitness cost is typically associated with drug resistance474
arising from genetic mutations [34, 60, 61], and has recently been suggested for non-genetic persister475
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states as well [27]. It is interesting to note however that though the IMT distributions do not476
distinguish the ancestors of persisters versus sensitive cells, the number of divisions undergone can477
be predictive of eventual cell fate after drug treatment [36].478
The use of single-cell time lapse microscopy datasets in this study provides an advantage over other479
barcoding studies in terms of the high resolution at which lineages can be reconstructed. Indeed,480
these results demonstrate the advantage of using single-cell resolved lineage correlations over barcode-481
diversity based methods to infer timing of fate decisions (Fig. 5b-c). However, these experiments482
and hence our accompanying analyses have the major limitation of exploring very short time-scales483
after drug treatment (on the order of a few days). As a result, we cannot comment on effects of484
long-term drug exposure on cell-state switching, or drug induced gradual cell-state reprogramming485
over long time scales [5, 6, 20, 7, 28]. Careful combinations of time-lapse microscopy along with486
barcoding studies will be required to delineate short-term versus long term dynamics and provide a487
full picture of non-genetic drug tolerance that eventually leads to genetic resistance.488
Conclusions489
We quantitatively demonstrate in this study that stochastic choices between survival and death based490
on post-drug division and death rates is not how cancer cells make fate decisions. Rather, the choices491
are largely pre-determined via cell-states that exist at least 2-3 generations before drug treatment,492
and are inherited by successive generations. This is true both for the cell-state that likely leads to493
drug-tolerant persisters as well as the state that makes cells susceptible, thereby suggesting that the494
notion of a fitness cost need not necessarily apply to non-genetic mechanisms driving persistence. To495
a smaller extent the fate decisions are also modulated by the drug, and together with the pre-existing496
cell-states, quantitatively explain the emergence of lineage correlations in end-fate and the population497
dynamics. We argue that the existence of lineage correlations is a better alternative to inferring the498
timing of fate decisions as opposed to barcode diversity analysis, which is hard to interpret in the499
presence of cell-state switching. These arguments do not require knowledge of the specific molecular500
details of the underlying cell-states, and hence provide a general and powerful approach to the study501
of drug-tolerance on short time scales driven by non-genetic heterogeneity.502
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