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The Population Genetics of Clonal and Partially Clonal Diploids
François Ballouxa,b, Laurent Lehmannc, and Thierry de Meeûsda I.C.A.P.B., University of Edinburgh, Edinburgh EH9 3JT, Scotland, United Kingdom,
b Department of Genetics, University of Cambridge, Cambridge CB2 3EH, United Kingdom,
c Institute of Ecology (Zoology and Animal Ecology), University of Lausanne, 1015 Lausanne, Switzerland
d Centre d'Etude du Polymorphisme des Microorganismes, Equipe ESS, UMR 9926 CNRS-IRD, BP64501, 34394 Montpellier Cedex 5, France
Corresponding author: François Balloux, University of Cambridge, Downing St., Cambridge CB2 3EH, United Kingdom., fb255{at}mole.bio.cam.ac.uk (E-mail)
Communicating editor: M. K. UYENOYAMA
| ABSTRACT |
|---|
The consequences of variable rates of clonal reproduction on the population genetics of neutral markers are explored in diploid organisms within a subdivided population (island model). We use both analytical and stochastic simulation approaches. High rates of clonal reproduction will positively affect heterozygosity. As a consequence, nearly twice as many alleles per locus can be maintained and population differentiation estimated as FST value is strongly decreased in purely clonal populations as compared to purely sexual ones. With increasing clonal reproduction, effective population size first slowly increases and then points toward extreme values when the reproductive system tends toward strict clonality. This reflects the fact that polymorphism is protected within individuals due to fixed heterozygosity. Contrarily, genotypic diversity smoothly decreases with increasing rates of clonal reproduction. Asexual populations thus maintain higher genetic diversity at each single locus but a lower number of different genotypes. Mixed clonal/sexual reproduction is nearly indistinguishable from strict sexual reproduction as long as the proportion of clonal reproduction is not strongly predominant for all quantities investigated, except for genotypic diversities (both at individual loci and over multiple loci).
THE essential feature of sexual reproduction is that genetic material from different ancestors is brought together in a single individual. If sexual reproduction is dominant in eukaryotic organisms (e.g., ![]()
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Here we present both analytical and stochastic simulation results for the population genetics of clonally and partially clonally reproducing populations. We focus on a simple population subdivision model (island model) and restrict our work to neutral mutations. We derive the identities by descent, F-statistics, and mean coalescence times of alleles and genotypes for variable rates of clonal reproduction. We also investigate the allelic and genotypic diversities maintained under different rates of clonal reproduction.
| MODEL ASSUMPTIONS AND GENETIC IDENTITIES |
|---|
We consider a subdivided monoecious population of diploid individuals, which reproduce clonally with probability c, with sexual reproduction occurring at the complementary probability (1 - c). Sexual reproduction in the model follows random union of gametes, self-fertilization occurs at a rate s, and a subpopulation is composed of N number of adults. In our model, individuals, rather than gametes, migrate following an island model (![]()
- Adult reproduction and subsequent death
- Juvenile dispersal
- Regulation of juveniles, the survivors reaching adulthood
Because of the symmetry of the island model, only the following probabilities of identity by descent are needed to describe the apportionment of genetic variation in a subdivided monoecious population.
- F: The inbreeding coefficient, defining the probability that two alleles drawn at random from a single individual are identical by descent.
: Coancestry of individuals drawn at random from within the same subpopulation, defined as the probability that two randomly sampled alleles from two different individuals within a subpopulation are identical by descent.
: Coancestry of individuals randomly drawn from different populations. This is defined as the probability that two randomly sampled alleles from two individuals in different subpopulations are identical by descent.
The identities may be calculated in juveniles (FJ,
J,
J), or adults (FA,
A,
A), or respectively before or after migration. In a first step, we express identities between adults one generation forward in time (t + 1) as functions of juvenile identities (t + 1/2). Adult identities are affected only by dispersal,
![]() |
(1) |
with qs being the probabilities that two individuals taken at random within the same subpopulation after migration were born in the same deme. The exact expression for qs is relatively cumbersome (see ![]()
![]() |
(2) |
where m represents the migration rate and n the number of subpopulations. Now we can define qd as the probability that two individuals sampled after migration in different subpopulations originated from the same deme:
![]() |
(3) |
We then express juvenile identities as functions of adult identities in the previous generation. Here both mutation and the reproductive system will affect the genetic identities of juveniles. The mutation rate is u for all alleles and therefore the probability of two alleles that are identical by descent before mutation still being identical after mutation will be
(1 - u)2. In the absence of any mutation event, clonal reproduction occurring at rate c will produce offspring identical to its progenitor, so that the inbreeding coefficient of a clonally produced juvenile individual will be identical to its parent's. Selfing occurs with probability s, and in that case the coancestry will be (1 + FA)/2. With a probability 1 - s, nonselfing sexual reproduction occurs, the offspring will have two parents, and its inbreeding will be the parental coancestry (
A). This gives us the following juvenile identities as functions of adult identities:
![]() |
(4) |
Substituting Equation 4 in (1), we obtain the recurrence equations for describing the dynamics of identities among adults:
![]() |
(5) |
The recurrence equations for
A and
A are identical to those given by ![]()
For analytical effectiveness, recurrence equations for identities by descent can be presented in matrix form,
![]() |
(6) |
where Qt is a column vector of the probabilities of identities at generation t + 1. The transition matrix G defines the probabilistic changes of the vector variables, and D is the constant column vector. Solving (6) at equilibrium we obtain the identities from
![]() |
(7) |
with I being the identity matrix.
| INDIVIDUAL-BASED SIMULATIONS |
|---|
To obtain the variances of the quantities of interest, as well as multilocus behavior, we additionally performed stochastic individual-based simulation, as implemented in the software EASYPOP (version 1.7.4; ![]()
| F-STATISTICS |
|---|
Deviations from random mating are generally expressed by means of F-statistics (![]()
![]()
![]() |
(8) |
(![]()
![]()
![]() |
(9) |
(![]()
Within-population deviations from random mating (FIS):
Replacing the solutions of Equation 7 in (8), we get FIS after migration for subdivided populations with a mixed system of clonal and sexual reproduction (selfing set to 1/N) and zygotic migration
![]() |
(10) |
Neglecting mutation (
= 1), but allowing for a mixed system of clonal reproduction with arbitrary selfing rate, we obtain
![]() |
(11) |
The equation shows that FIS is independent of the migration rate but sensitive to the total number of individuals in the population; this occurs because we assumed zygotic rather than gametic migration. Under random mating (s = 1/N) we further obtain
![]() |
(12) |
When reproduction is strictly sexual (c = 0), Equation 12 reduces to the form
![]() |
(13) |
For a strictly clonal population (c = 1), FIS = -1. This reflects the fact that in the absence of sexual reproduction, all individuals are expected to be heterozygous at equilibrium F = 0, while
= 1/2.
In Fig 1, we plot FIS as obtained from Equation 10 against the rate of clonal reproduction. We also give values obtained from individual-based simulations. Analytical and stochastic simulation results are in excellent agreement. From Fig 1, it can be seen that for very high values of clonal reproduction, huge heterozygote excesses are obtained. However, as long as there is a small proportion of sexual reproduction, FIS stays close to what is expected under panmixia; a significant excess of heterozygotes occurs only for extreme rates of asexuality. As long as there is mutation in the system, FIS cannot reach -1 even for strict clonality. If the product of the number of individuals in the complete population (nN) times the mutation rate is high, the FIS value for complete clonality can be very much offset from -1. The reason for this can be seen from Equation 8. Under clonal reproduction all individuals will be heterozygous and this will not be changed by mutation, so F = 0, while
decreases with increasing mutation rate.
|
The FIS estimates from the stochastic simulations in Fig 1 are averaged over loci and replicates and do not reveal anything about the strong influence of the rate of clonal reproduction on the variance over loci. This huge variation among loci, in particular for low rates of sexual reproduction, is illustrated by standard errors in FIS (Fig 2). The lowest variations are obtained with pure clonality and with <95% of clonality.
|
Population differentiation (FST):
Again by replacing the solutions of Equation 7 in (8), we obtain FST for subdivided populations with a mixed system of clonal, selfing, and sexual reproduction after migration:
![]() |
(14) |
Neglecting mutation (
= 1) leads to
![]() |
(15) |
Finally, if only sexual reproduction is allowed (c = 0 and s = 1/N), we get
![]() |
(16) |
In Fig 3, we plot FST as obtained from Equation 14 against the proportion of clonal reproduction, as well as values obtained from the individual-based simulations. The amount of clonal reproduction has a strong effect on population differentiation. Whereas even for very limited proportions of sex, there is no noticeable effect, when reproduction tends toward strict clonality, FST is strongly reduced. Note that in the absence of any mutation, FST would be defined but equal to 0, as all the genetic variance is within individuals and none between individuals and subpopulations. In all simulated cases the between-loci variance of FST strongly increases with the proportion of clonal reproduction (results not shown).
|
| EFFECTIVE POPULATION SIZE |
|---|
Effective population size:
The effective population size (![]()
![]()
![]()
![]() |
(17) |
where
is the expected time it takes for two randomly sampled alleles in a population to coalesce to a common ancestor. For the Wright-Fisher model
, so that the effective size reduces to the actual number of diploid individuals. This definition of effective size allows us to disentangle the allelic effective size (all classical definitions) from the genotypic effective size (see below), and we can further obtain their variance.
There is a strict relationship between identity-by-descent probabilities and coalescence times (![]()
![]()
![]()
![]() |
(18) |
The matrix G is diagonalizable for c
1. We can represent the vector D on the basis of the right eigenvectors of the matrix G as D =
jajrj, where j is the number of columns of G, aj the coefficient determined by the preceding system of equations, and rj
(r1j, ... , rkj)T the jth right eigenvector of G. Using the fact that the jth eigenvalue of the matrix (I -
G)-1 is 1/(1 - 
j), and its associated right eigenvector is rj, where
j is the jth eigenvalue of G, we can express Equation 18 following ![]()
![]() |
(19) |
The second equality is obtained by using the property of geometric series. Then
![]() |
(20) |
is the coalescence probability of alleles at time t at any hierarchical level i (where i stands for F,
, and
). From this, we can obtain the expected coalescence times by classical tools. However, after substituting Equation 20 into Equation 19, a closer look reveals that the vector Q defines the probability-generating functions of coalescence time at each level i. These functions reduce to the calculations of expected coalescence times as
![]() |
(21) |
where
is the expected coalescence time at level i and Qi is the ith row of the equilibrium vector given by Equation 20 and their variances as
![]() |
(22) |
At this point we have all necessary tools to obtain the mean coalescence times of alleles in a subdivided population with arbitrary rates of clonal reproduction. Writing the recurrence Equation 5 under the form given in Equation 18 and using Equation 21 yields the following mean coalescence times,
![]() |
(23) |
where 
is a low migration limit obtained by a first-degree Taylor expansion. The mean coalescence time of two randomly sampled alleles is the expectation of the
i; in the finite-island model this yields
![]() |
(24) |
Substituting Equation 24 into (17), we obtain the coalescence effective population size. Note that this effective size captures the loss of allelic diversity in the population and we refer to it as 2Ne, the allelic effective population size, which is equal to
in our model. In Fig 4, we plot the effective population size as a function of clonal reproduction and selfing rate (the union of gametes within individuals). Increasing the rate of clonal reproduction has no noticeable effect on most of the parameter space. However, when the reproductive system tends toward complete asexual reproduction, the effective population size suddenly tends toward infinite values. This slightly counter-intuitive result simply reflects that the genetic diversity within individuals cannot be lost in clonal organisms. Doubling of Ne compared to random mating is observed approximately when the rate of sexual reproduction is in the order of 10-4 with the simulation parameters used in Fig 4. Contrarily, increased rates of selfing decrease effective population size. This effect is linear and the effective population size ranges between Ne under absence of selfing to Ne/2 for strict selfing.
|
Genotypic and allelic effective population size:
We have shown that increased rates of clonal reproduction will increase the allelic effective population size, and thus clonal populations are expected to maintain more alleles at neutral loci than are sexually reproducing ones. We can go a step further and address the issue of how clonal reproduction will affect the number of different genotypes maintained. The coalescence approach allows us to capture qualitatively these trends by calculating the genotypic effective population size. To obtain this quantity, we need, in addition to F and
,
, the probabilities that three alleles randomly sampled in two different individuals are identical. These three variables are necessary to calculate the probability
that two genotypes are identical. However, these higher-order coefficients are complicated and we therefore limit ourselves to a non-subdivided monoecious population without mutation. We follow the approach of ![]()
![]() |
(25) |
Note that when c = 0, F =
, and the recurrence equations reduce to COCKERHAM's (1971) model. Substituting these equations into a transition matrix G and a column vector of constants D following Equation 18 allows us to obtain the mean coalescence times:
![]() |
(26) |

is the mean coalescence time for genotypes and we refer to it as the genotypic effective size. This quantity is undefined for c = 1 as the matrix G is not diagonalizable in this case. However, we know that when c = 1, the genotypic identity is independent of F,
, and
and thus follows a dynamic similar to haploid genetics, with mean coalescence time N. When c
1, the mean genotypic coalescence time 
takes the form of a relatively complex polynomial (the coefficients are given in Appendix B). Note that in the absence of clonal reproduction, there is a very compact approximation for the genotypic coalescence time 
3N (see Appendix B). Mean coalescence time for alleles in a nonsubdivided population can be obtained as
and thus reads
![]() |
(27) |
Note that we could have obtained the allelic effective size directly from Equation 24 assuming no migration, one subpopulation, and a selfing rate of 1/N. In Fig 5, we give mean coalescence times for both alleles and genotypes. It can be seen that contrarily to what is observed at the allelic level, genotypic effective size decreases with increasing clonality. The decrease is relatively smooth over the complete parameter range of c and reaches N for strict clonality. The intuitive reason behind this is that when there is no segregation at all, the two alleles within a diploid individual behave as a single haploid locus. The rate of clonal reproduction has thus an antagonistic effect on the variability of alleles and genotypes.
|
| GENETIC DIVERSITIES |
|---|
We can now take a closer quantitative look at how genetic diversity is distributed between alleles and genotypes with the stochastic simulations. Allelic diversity can be expressed as the effective number of alleles, ne, corresponding to the number of equally frequent alleles needed to observe a given genetic diversity, which is 1/(
pi2), where pi is the frequency of the ith allele. Similarly, we can express the effective number of genotypes as Ge = 1/(
gi2), where gi is the frequency of the ith genotype. In Fig 6 we plot both the effective number of alleles and genotypes within a subpopulation. The number of alleles maintained is strongly positively affected when the reproductive system tends to be completely asexual. This effect is generated by fixed heterozygosity (i.e., under strict clonal reproduction in diploids the two alleles at each locus are behaving as two haploid loci). In contrast to allelic diversity, clonal reproduction decreases the effective number of genotypes steadily (Fig 6). To summarize, populations of clonal or subclonal organisms can maintain more allelic diversity at each single locus but fewer distinct multilocus genotypes.
|
| DISCUSSION |
|---|
We used both an analytical approach and stochastic individual-based simulations to describe the dynamics of genetic variance in subdivided populations, characterized by various levels of clonal reproduction. Higher rates of asexual reproduction will increase heterozygosity and decrease population differentiation. Diversity at single loci will be higher in clonal organisms than in sexuals, whereas the opposite is true for genotypic diversity. At the exception of genotypic diversity (both at single loci and over multiple loci), which decreases at a constant rate with increasing rates of asexual reproduction, all other quantities investigated are significantly affected only when sexual reproduction becomes rare.
Our results thus suggest that strict clonality may easily be detected in diploid populations due to heterozygote excess. Furthermore, very low levels of sex (cryptic sex) may also be revealed by on average low FIS values with very important variance among loci, though DNA alterations may also lead to a similar pattern in a strictly clonal population. For instance, Candida albicans is known to undergo mitotic recombinations including chromosomal translocation (![]()
![]()
![]()
![]()
![]()
![]()
![]()
Empirical data on genetic variation and its apportionment by means of F-statistics in clonal lineages, as compared to sexually reproducing populations of the same species, are rare. Furthermore, studies using dominant genetic markers (e.g., rapidly amplified polymorphic DNAs) do not properly allow for the disentanglement between genetic variation within loci and within genotypes. Indeed, as can be seen from Fig 6, the absolute genetic diversity (the sum of allelic and genotypic variability) does not provide any clear prediction on the rate of clonal reproduction. Another potential problem stems from the difficulty in ruling out the presence of rare sexual reproduction. However, a recent study by ![]()
![]()
![]()
Indeed our model does not include natural selection, so that our results apply strictly to neutral genetic variability or more generally to relatively weakly selected polymorphisms subject to genetic drift. Genetic drift is the main force driving allele frequencies as long as the selection differential s between alleles is not much above the inverse of effective population size (1/Ne). For higher selection differentials, the effect of genetic drift becomes negligible. However, our predictions should hold even for relatively important selection differentials in clonal and nearly clonal organisms, as the efficacy of selection acting simultaneously at linked sites is considerably reduced (![]()
We assumed identical fitness (in both mean and variance) for clonally and sexually produced offspring. The rate of clonal reproduction is not a heritable trait in our model, as it is a fixed property of the population (clonally produced individuals do not have a higher chance to reproduce clonally themselves). Therefore, different fecundities for sexually or clonally produced offspring would result only in increasing the variance in reproductive success and thus would decrease the effective population size. Our results are thus qualitatively robust to reasonable differences in relative fitness between clonally and sexually produced offspring.
Finally, our model could lead to the development of new approaches to infer the rate of clonal reproduction. Our results show that all estimators based on identities by descent (including linkage disequilibrium approaches) are expected to be rather insensitive to the rate of clonal reproduction as long as it does not become strongly predominant. It is therefore doubtful that such estimators will allow precise inferences on the actual rate of clonal reproduction unless it is very close or equal to 1. As genotypic diversity decreases smoothly with the rate of clonal reproduction, one promising alternative approach would be to build estimators of clonal reproduction as functions of the relative genotypic and allelic identities.
| ACKNOWLEDGMENTS |
|---|
We thank Nathalie Charbonnel, Sylvain Gandon, Jerôme Goudet, Andy Overall, Franck Prugnolle, François Renaud, Max Reuter, Denis Roze, Michel Tibayrenc, and two anonymous referees for very inspiring conversations and comments; François Rousset for having given access to unpublished material; and Sylvain de l'Hérault for his strong support. F.B. was supported by the Biotechnology and Biological Sciences Research Council and by grant 823A-067616 from the Swiss National Science Foundation.
Manuscript received November 6, 2002; Accepted for publication April 11, 2003.
| APPENDIX A |
|---|
GENOTYPIC PROBABILITIES OF IDENTITIES BY DESCENT
We follow the same rationale as ![]()
. When one offspring is produced clonally, his two alleles are not independent. When we sample alleles and look back to their common parent, the two genes of a clone always stem from the same individual. Two clones are randomly sampled with probability c2; the four genes stem either from the same parent or from two different ones. The identity between genotypes and three alleles reads
![]() |
(A1) |
(two from one offspring, the third from the other). When one offspring is produced clonally and one through random mating, the identity among three alleles will differ if two or only one allele stem from the clonal offspring, the former case occurs with probability c(1 - c) and the identity is as in Equation A1. The second case also occurs with probability c(1 - c), and the three genes then all stem from the same parent with probability P3 and share identity
3. The three genes might as well stem from two different parents with probability P21 and then have identity
21; finally, they can stem from three different parents with probability P111 and their identity is
111. The three types of identities can be expressed as
![]() |
(A2.1) |
For the identity between genotypes, we have with probability 2c(1 - c):
![]() |
(A2.2) |
When we sample two offspring issued from random mating with probability (1 - c)2, the identities for
are given by Equation A2.1. The genotypic identity is obtained by summing
4,
22,
31,
211, and
1111, each identity weighted by its corresponding probability P4, P22, P31, P211, and P1111. The five identities are written
![]() |
(A3) |
The different probabilities of gamete origins are given in ![]()
![]() |
(A4) |
| APPENDIX B |
|---|
COEFFICIENT OF Equation 23
![]() |
(B1.1) |
![]() |
(B1.2) |
If c = 0, then the mean coalescence time for two genotypes in the Wright-Fisher setting reduces to
![]() |
(B2) |
Performing a Taylor expansion of first degree under large population size and substituting some close integers yields the approximation for Equation B2:
![]() |
(B3) |
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