Abstract
Neutral models, in which genetic change arises through random variation without fitness differences, have proven remarkably successful in describing observed patterns of biodiversity, despite the manifest role of selection in evolution. Here we investigate the effect of barriers on biodiversity by simulating the expansion of a population around a barrier to form a ring species, in which the two ends of the population are reproductively isolated despite ongoing gene flow around the ring. We compare the spatial and genetic properties of a neutral agent-based population model to the greenish warblers’ complex, a well-documented example of an actual ring species in nature. Our results match the distribution of subspecies, the principal components of genetic diversity, and the linear spatial–genetic correlation of the observed data, even though selection is expected to be important for traits of this species. We find that ring species are often unstable to speciation or mixing but can persist for extended times depending on species and landscape features. For the greenish warblers, our analysis implies that the expanded area near the point of secondary contact is important for extending the duration of the ring, and thus, for the opportunity to observe this ring species. Nevertheless it also suggests the ring will break up into multiple species in 10,000 to 50,000 y. These results imply that simulations can be used to accurately describe empirical data for complex spatial–genetic traits of an individual species.
Keywords: geography, topopatric, allopatric, birds, DNA
There is a growing paradox in our understanding of the core issues of speciation and biodiversity. First, the manifest empirical importance of selection in the traits of species appears to be counter to the ability to describe biodiversity by using neutral models of speciation (1–4). Second, geographical heterogeneity, including geographical isolation, is no longer considered necessary to account for the emergence of new species. Traditionally, the emergence of new species has been explained by a period of geographic isolation of subpopulations. In the absence of gene flow, genetic differences accumulate and reproductive isolation eventually arises (5). However, if population ranges are large enough, genetic divergence can lead to speciation despite ongoing gene flow (6), as demonstrated by empirical and theoretical results (7–15). Moreover, it has been shown that existing patterns of diversity are consistent with such speciation with ongoing gene flow and without trait selection or spatial heterogeneity, as long as mating is constrained by spatial and genetic distances (15). Here we show that neutral models of speciation can also account for the genetic diversity of a single species in a context in which geographical barriers play a central role in that diversity. We compare the diversity of a neutral model to empirical findings about a ring species formed when population expansion occurred around a geographical barrier. The genetic patterns are consistent even though selection is expected to be important for traits of this species (11, 16, 17).
Currently, the best documented example of a ring species is that of the greenish warblers, which inhabit a ring around the Tibetan Plateau (11). In the northernmost area of this ring are two Siberian taxa that are reproductively isolated and occupy overlapping geographical regions (18). Gene flow is still possible between them over multiple generations through a chain of reproductively linked taxa around the ring. One noteworthy characteristic is that the Siberian taxa, which occur in the area of secondary contact (i.e., ring closure) of the expanding population, have much larger distribution ranges than do other subspecies. The correlation between range size and latitude is a strong pattern found in many terrestrial groups of the Old World (19).
We simulated the formation of a ring species (Fig. 1) (20), explicitly including the ring topography and allowing a small initial population to grow as it expands and differentiates around a geographical barrier (Fig. S1). We used an individual-based model based on neutral replacement with local mating, migration, and mutation (Methods). Reproductive isolation is modeled by a multilocus generalization of the Bateson–Dobzhansky–Muller model whereby the population evolves through nearly constant fitness ridges (21, 22). The initial population is set within a starting area, and the individuals whose local mating area is underpopulated generate two rather than one offspring before dying. This enables the population to grow and spread up to the carrying capacity of the entire available space.
Results and Discussion
The genetic variation plot (Fig. 1 C and D) reveals a gradual genetic change over geographical space (see also Figs. S2 and S3). Simulated and actual warbler populations have a similar decomposition of variance (15.9% vs. 19.4% for the first principal component and 10.8% vs. 5.6% for the second principal component, respectively). The genetic distance between individuals increases linearly with their geographic distance as measured around the ring in both cases (Fig. 1 E and F). Different behaviors are expected for a single mixed species or multiple species (Fig. S4). For the sampling shown in Fig. 1, the average genetic distance within populations—the number of differing loci along their strings—is approximately three and the genetic distance between the populations at the area of secondary contact is approximately seven. This is in agreement with amplified fragment length polymorphism (AFLP) data (11) in which AFLP distances between populations at secondary contact is approximately twice the average distance within populations. The number of genetic differences in the sampled model corresponds to the same proportion of AFLP differences in the sampled experimental observations. This indicates that populations separated by half the ring’s length should already be reproductively isolated. The terminal populations came into contact after ∼2,000 generations (Fig. 2, middle line). The number of generations is consistent with the timing of habitat recovery as a result of tree cover expansion—an important factor in the spread of the greenish warbler. The forest range expanded starting approximately 10,000 y ago and achieved its current area ∼2,000 y later (17). Given the greenish warblers’ annual life cycle and assuming that their range expansion accompanied this forest recovery (19), the rates of population expansion in our simulations coincide, consistent with empirical evidence (17). A sharp boundary between reproductively isolated subspecies in the area of secondary contact is maintained by the difficulty in finding compatible mates when an individual is surrounded by the other type. The spatial and genetic restrictions in mating lead to selection against rare types in favor of common types in the region of overlap. The U-shaped pattern in Fig. 1 C and D and Fig. S3B is a consequence of the gene flow around the ring that couples the otherwise independent expanding fronts. If the fronts begin to mix into a single species, the bending increases and the “U” shape turns into an “O” shape that closes into a single spot.
There seems to be an empirical mismatch between the expected spread of the population around the ring 10,000 y ago and the genetic divergence of types measured by using mitochondrial DNA clocks, which is 2 million years (11). This may be resolved through the observation that asexual replication of mitochondria diverges genetically even without speciation, whereas genetic bounds on reproduction limit the range of the sexual component of the genome. Before ring formation, when the population evolved while located solely in the southernmost area, the diversity of mtDNA would diverge, but would be spatially correlated in local patches reflecting branches of the ancestral tree (23, 24). The spreading of the population from one patch around one arm and another patch around the second arm of the ring would result in large divergences between the mitochondrial DNA of the types that meet after ring closure. The divergence would be characteristic of the time to common ancestor of that DNA, but not of the time of ring formation. This scenario is consistent with simulations (Fig. S5).
Although natural and/or sexual selection appear to be important for greenish warblers’ traits (11, 16, 17) and those of other potential ring species (13, 18, 25–29), our results show that their role in the emergence of reproductive isolation and maintenance of ring species (as suggested in ref. 11) is not yet well understood. Consistent with the importance of neutral divergence in the formation of ring species, for the salamander Ensatina eschscholtzii, a second well-documented ring species (reviewed in ref. 30), divergence in neutral nuclear markers is a better predictor of reproductive isolation than ecological divergence (31).
Our model of ring species formation also provides an opportunity to clarify and analyze the role of geographical barriers. There is a dichotomy that can be readily understood: fast enough differentiation leads to multiple species as a result of isolation by distance (15), whereas slow differentiation leads to a single species (Fig. 2). Our question, however, is whether a third intermediate case of ring species can be robustly formed so they are observed in nature. When a population expands around a spatial barrier that limits its range, the interplay between the velocity of range expansion and genetic differentiation will determine the fate of the terminal populations when they come into secondary contact. Increasing carrying capacity decreases differentiation (32) and increases the velocity. Other features that affect this interplay include population features (e.g., growth rate, mating distance, dispersal rate, and mobility) and landscape features (e.g., corridor width, distance around the barrier). None of these provides stability for a ring species. We tested the robustness of ring species formation to variation in the geographical structure of the ring. We hypothesized that the larger habitable area present near the region of secondary contact enhanced the likelihood of ring species formation. Larger populations of the divergent types inhibit genetic fluctuations that could lead to mating opportunities that would revert the speciation process (33). Simulations confirmed that when the excess area was displaced to a different location in the ring near the point of origin, equivalent to shifting the point of origin from south to north, ring species were less likely to form, even though the time until secondary contact between terminal populations remained the same (Fig. 3). The enlarged regions in the contact area reduce genetic variability over time, and selection against rare types limits the overlap area, reducing the probability of merger.
Fig. 4 shows the occurrence of ring species formation as a function of the dispersal rate and carrying capacity, which are related to the rate of population expansion. The comparison of results in the two different geographical structures highlights the importance of the specific structure of the landscape (not just geographic distance around the ring) in regulating genetic variability in space and thus the outcome of the speciation process.
Even though we find that ring species can form during expansion, given the possibility of speciation without barriers, an important question is whether ring species are ultimately stable to breaking up into multiple species or to consolidation to a single interbreeding population. The extent of their persistence is important for determining their prevalence in nature. To evaluate stability and persistence, we extended simulations that resulted in ring species after 10,000 generations. We performed these simulations for both geographical structures previously identified. In the original scenario in which ring species are more likely to form, we found that they persist for many generations, although eventually most resolve to single mixed or multiple species. The time until 90% of ring species collapsed by speciating or mixing was 130,000 generations. For the simulation shown in Fig. 1, the ring species is expected to break up into multiple species in 10,000 to 50,000 y (Figs. S6 and S7). Thus, most ring species are not stable, but they can persist for a long time and thus be observed. These results counter the idea of ring species instability reported in previous models (9, 34, 35).
Comparisons between closely related taxa that share a history of range expansion around the same barriers could provide empirical insight into the relation between species’ and landscape parameters in ring species formation. Old World leaf warblers, genus Phylloscopus, are forest-dependent species, and the range expansion of their ancestral populations is thought to be associated with forest expansion following warming of the climate after Pleistocene glaciations (19). However, the only case of ring species confirmed so far for this group is the greenish warbler (Phylloscopus trochiloides). The species in Phylloscopus inornatus complex, for example, have been considered separate species based on genetic and song divergence (36). Salamanders in western North America may provide another interesting case. Despite some taxonomic controversy, the E. eschscholtzii complex is still one of the few well-documented ring species (reviewed in ref. 30), and it occurs in sympatry with other salamander genera (27).
The fine-tuning of population, individual, and landscape parameters necessary for ring species formation in our simulations, as well as their ultimate instability, suggest that ring species can be expected to be rare in nature. For a given barrier, only species within a narrow range of mobility are candidates to display rings. More mobile species, e.g., birds, require larger barriers than do reptiles or small mammals. The key genetic evolutionary parameter is the underlying rate of genetic isolation, the mutation rate divided by the genetic isolation distance. Ring species will form if the period of expansion L/v, where L is the ring size and v is the speed of expansion times the rate of genetic isolation w, is approximately one, i.e., if Lw/v ∼ 1. Even under this condition, rings will be more or less likely depending on the details of the geography. Given the wide range of observed results, simulations may be used to characterize the dynamics of range expansion genetics for direct comparison in multiple cases, including single, multiple, and ring species.
Finally, this work also demonstrates that barriers can dramatically increase speciation, even when they do not cause isolation. Many of the simulations that resulted in multiple species in the ring geometry would result in a single species were the barrier not present. Speciation is a result of the increase in effective distance around the ring, as well as the reduction in carrying capacity of the narrow circumferential habitat. This speciation by partial obstruction complements the idea of speciation by partial isolation, i.e., parapatric speciation.
Methods
The simulations use an agent-based population model that consists of haploid and hermaphroditic individuals characterized by a binary string of B loci. Reproduction is restricted by a mating area determined by a spatial distance, S, and a genetic distance, G, beyond which other individuals are not considered potential mates. Reproductive isolation caused by this mechanism can be considered a multilocus generalization of the Bateson–Dobzhansky–Muller model whereby individuals accumulate genetic incompatibilities without the population passing through an adaptive valley (22). Reproductive success depends on the number of genetic differences between the individuals attempting mating, without affecting the fitness of the individuals themselves (21). The genetic distance between two individuals is the number of differing loci along their strings. The geographical space is represented by a 128 × 142 lattice with barriers defined by sites that cannot be occupied by individuals (Fig. S1). The remaining sites can be occupied by multiple individuals. The carrying capacity, K, determines the maximum population size allowed in the entire population. The expected demographic density, ρ, is calculated as the ratio between K and the number of available sites. The initial population consists of genetically identical individuals randomly placed in a fixed area bellow the larger barrier, as shown in Fig. S1. The number of individuals in the initial population is given by ρ times the number of sites in this area.
The population evolves in discrete generations. Each individual seeks potential mates for reproduction once and is replaced by the resulting offspring. However, there is a probability Q that the individual will not reproduce at all. In this case, a neighbor is selected at random to reproduce in its place. In each reproductive event, one individual is selected at random from the list of potential mates (meeting spatial and genetic criteria), and the genetic information of both parents is combined with one genetic crossover for which the breakpoint is randomly selected along the string. There is a mutation rate per locus, µ. Offspring dispersal occurs with probability D; the offspring is placed at one of the 20 neighboring sites, chosen randomly. In addition, if the demographic density in the mating area is lower than 60% of the expected demographic density, ρ, a second offspring is produced. This allows for the spreading of the population toward empty areas, as shown in Fig. 3 and Fig. S2. After the population reaches the carrying capacity, each individual can have only one offspring. If there are fewer than P potential mates for a specific individual, the mating area for that individual is increased by setting S to S + 1. If the number of available mates is still smaller than P, the process is repeated. S may be increased by a maximum of 10 units, in which case, if there are still less than P potential mates, a neighbor is randomly selected to reproduce instead. A highly divergent individual is likely to be replaced by a more common type. This selects against rare types when they coexist with a common type in a geographical region.
For the results reported, B is equal to 125, S is 9, G is 20, µ is 0.0003, Q is 0.3, P is 20, and the geographical barriers occupy 11,796 of 18,176 sites, leaving 6,380 available (Fig. S1).
A species is identified as a group of organisms that are connected by gene flow and separated from all others by the genetic restriction on mating determined by G. This definition does not require all members of a species to be able to mate with each other; two members can be incompatible, as long as they can exchange genes indirectly through other members of the species. As an example, three individuals A, B, and C whose genetic distances satisfy d(A,B) < G, d(B,C) < G, but d(A,C) > G belong to the same species. A mutation occurring in A can be transmitted to the offspring of A and B that can, in turn, pass the mutation on when mating with C or its offspring. Considering this strategy to delimitate species, ring species are identified as a population in which we would identify two species when considering only the individuals located in the area of secondary contact (Fig. S1), but a single species when considering the population as a whole.
In all figures in which individuals are shown in color, the color is according to the genetic distance to a reference individual, marked as a star. Dark blue corresponds to potential mates for the reference individual (those whose genetic distance is less than the critical value, G). The remaining colors represent genetic distances in the following intervals: light blue (G, 1.15G); green (1.15G, 1.152 G); yellow (1.152 G, 1.153 G); orange (1.153 G, 1.154 G); and red, greater than or equal to 1.154 G. Ring species formation is sensitive to variations in S, G, µ, K, and D. The effects of varying K and D are described in the text and figures; varying other parameters combinations yield qualitatively similar results.
Supplementary Material
Acknowledgments
The authors thank Sergey Gavrilets, Trevor Price, and Les Kaufman for helpful comments on the manuscript; and M.A.M.d.A. thanks Conselho Nacional de Desenvolvimento Científico e Tecnológico. This study was supported by Fundação de Amparo a Pesquisa do Estado de São Paulo (A.B.M. and M.A.M.d.A.).
Footnotes
The authors declare no conflict of interest.
This article is a PNAS Direct Submission.
This article contains supporting information online at www.pnas.org/lookup/suppl/doi:10.1073/pnas.1217034110/-/DCSupplemental.
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