Chapter 3 · PGT-mt fundamentals

The mitochondrial genetic bottleneck

In a woman carrying an mtDNA variant in a heteroplasmic state, heteroplasmy levels can vary widely among her oocytes, from very low levels to near homoplasmy. This variability is attributed to the mitochondrial genetic bottleneck and makes PGT-mt possible.

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Essentials

Heteroplasmy can differ between tissues and oocytes

In a 30-year-old carrier of m.3243A>G with 35% heteroplasmy in blood, the mutant load ranged from 9% to 90% in oocytes and from 7% to 91% in embryos (Treff et al., 2012). This example shows that the heteroplasmy level can differ substantially between oocytes of one carrier. The heteroplasmy level in an individual oocyte cannot be predicted from a measurement in the mother’s somatic tissues alone (Smeets et al., 2023).

What the bottleneck is

The mitochondrial genetic bottleneck is the process by which, in the female germline, the mtDNA composition of each developing oocyte is determined by a pool of segregating units far smaller than the total number of molecules in a mature oocyte (Stewart & Chinnery, 2015; Xie et al., 2026). Draw 1,000 marbles from a bag in which 30% are red, and the proportion of red ones will almost certainly be close to 30%. Draw 10, and it may be 0% or 60%. The same applies to mtDNA: the smaller the effective pool, the larger the random shifts in heteroplasmy between oocytes.

Physical copies and effective units

Early in germline development the mtDNA content per cell does fall sharply: primordial germ cells of human embryos contain about 1,000-fold less mtDNA than a mature oocyte (Floros et al., 2018; Cree et al., 2008). But the “effective size” of the bottleneck is not the same as the number of physical molecules: mtDNA molecules are packaged in protein complexes called nucleoids, and mouse data suggest that only a subset of molecules may be replicated (Wai et al., 2008). The effective size is a statistical quantity estimated from the spread of heteroplasmy among offspring (Otten et al., 2018).

Chance and, possibly, selection

Much of this variability is explained by the random distribution of mtDNA molecules (genetic drift). However, evidence is accumulating that some mtDNA mutations are subject to selection — against high loads or, conversely, in favour of mutant molecules — and that it depends on the specific variant (Otten et al., 2018; Zhang et al., 2021; Floros et al., 2018). No single mechanism has yet been established as the universal explanation for all variants and developmental stages.

Why it matters for PGT-mt

Differences in heteroplasmy level between oocytes make it possible to select an embryo with a lower heteroplasmy level and thereby reduce the risk of disease in the future child. But the same variability makes the outcome of a cycle unpredictable: one cycle may produce several low-heteroplasmy embryos, another none (Hyslop et al., 2025). The simulator below illustrates how effective pool size affects the spread of heteroplasmy. It is an educational model, not a prediction for an individual patient.

The bottleneck explains why one woman’s oocytes differ. It does not allow the heteroplasmy of a particular embryo to be predicted in advance.

Advanced

Genetic drift, selection or both?

A central question of mtDNA genetics was posed long ago: are pathogenic variants transmitted like neutral ones, by random drift alone, or are they subject to selection (Chinnery et al., 2000)? Current evidence indicates that the answer depends on the variant and the developmental stage (Xie et al., 2026). The bottleneck hypothesis itself arose from observations in Holstein cows, in which a newly identified mtDNA variant shifted from heteroplasmy to homoplasmy within a few generations; for neutral variants this genetic bottleneck merely accelerates random drift, whereas for deleterious variants the distribution in offspring is skewed, pointing to selection (Xie et al., 2026).

Effective size of the segregating pool

Population-genetic models compare the variance of heteroplasmy among offspring with p₀(1 − p₀), where p₀ is the starting level, and use the ratio to estimate the effective number of segregating units. Otten and colleagues described segregation in oocytes, zygotes and blastomeres of carriers with the Kimura distribution and obtained bottleneck-size estimates ranging from 10 to 145 between carriers (Otten et al., 2018). This means that even if two mothers have the same heteroplasmy level, their risk of passing disease to a child may differ substantially. The effective size summarises many processes — the number of segregating units and the number of rounds of division and replication — and is not equal to the physical copy number.

Physical mtDNA copy number

Floros and colleagues showed that primordial germ cells of human embryos at CS12 contain about 1,000-fold less mtDNA than oocytes (median 1,425 copies per cell versus a mean of 1.22×10⁶ in oocytes), with approximately five mtDNA molecules in each mitochondrion; rare variants reached higher heteroplasmy levels after completion of migration, consistent with a bottleneck (Floros et al., 2018). Copy number in human primordial germ cells was lower than in mice at corresponding stages; the authors infer a “tighter” bottleneck and faster segregation in humans (Floros et al., 2018). In mice, Cree and colleagues explained rapid segregation by a reduction in the number of molecules during embryogenesis (Cree et al., 2008), whereas Wai and colleagues concluded that the bottleneck arises during postnatal folliculogenesis through replication of a subpopulation of genomes (Wai et al., 2008). The disagreement on timing and mechanism illustrates that no single model fully resolves the mechanism. According to the review by Xie and colleagues, mathematical modelling with the measured copy number and number of cell divisions showed that the reduction in copy number alone is sufficient to explain the spread of heteroplasmy in offspring, even without selection; the biological meaning of the bottleneck is still debated — it may make harmful mutations susceptible to natural selection (Xie et al., 2026).

A possible role for replication and selection

  • Selection in primordial germ cells. Floros and colleagues found signatures of selection against non-synonymous, tRNA-gene and D-loop variants, coinciding with a shift to oxidative metabolism (Floros et al., 2018).
  • Preferential propagation of mutant mtDNA in the oocyte. In mice carrying the m.5024C>T mutation, the proportion of mutant mtDNA increased as oocytes matured (without cell division), but the accumulation of critically high levels was blocked by purifying selection; a similar pattern — preferential transmission at low and selection at high load — has been described in pedigrees with m.3243A>G, m.8344A>G and m.8993T>G/C (Zhang et al., 2021).
  • Purifying selection and age. In mice carrying mutations in complex I genes generated by base editing, purifying selection occurred predominantly during postnatal oocyte maturation and intensified as the mother aged (Ru et al., 2024). These are mouse data; in human pedigree studies, by contrast, the number of new mtDNA mutations in children correlated positively with maternal age, and direct observations are needed before clinical conclusions can be drawn (Xie et al., 2026).
  • Human oocytes. Duplex sequencing of mtDNA in individual oocytes found no age-related increase in new mutations and pointed to frequency-dependent purifying selection (Arbeithuber et al., 2025); a preprint re-analysing the same data reaches a different conclusion: positive selection predominates on average, for non-coding control-region mutations and, according to the authors, even coding mutations (Franco et al., 2026, preprint).
  • Different windows of selection. In mice, elimination of defective mtDNA is tied to different developmental stages depending on the specific mutation. Selection may begin after the primordial germ cell and oocyte stages (m.3875delC), during follicle maturation (m.2820G>A, m.12918G>A), at the secondary follicle stage (m.3177G>A), or in early embryogenesis through mitophagy (m.5019A>G). It is not yet clear how much of these differences reflects real biology and how much reflects the research methods used (Xie et al., 2026).
  • Levels at which selection acts. Mechanisms have been described at the level of cells (follicular atresia), organelles (mitochondrial fission, mitophagy) and molecules (preferential replication); most data come from mice, Drosophila and nematodes (Xie et al., 2026).
  • Population data. Pathogenic mtDNA variants with low heteroplasmy levels occur in roughly 1 in 200 people, whereas mtDNA disease affects roughly 1 in 5,000–10,000; this discrepancy points to selection against transmission of deleterious variants. Human data are less consistent than mouse data: large deletions are rarely inherited; in a large study of mother–child pairs, mutations in rRNA genes were transmitted to offspring less often than expected, while variants in the D-loop region were inherited neutrally or with an advantage (Xie et al., 2026).
  • Variant specificity in carriers. For m.3243A>G the data were better described by a Kimura distribution truncated at 76.5% (no high loads); for m.8993T>G values were predominantly extreme and, in pedigree data, offspring levels were more often higher than maternal levels; for m.14487T>C no signs of selection were found (Otten et al., 2018).

Differences between oocytes of one woman

A mother’s somatic heteroplasmy level cannot predict the heteroplasmy level in a particular oocyte. In the study by Spath and colleagues, women with detectable somatic heteroplasmy had a higher proportion of embryos carrying the variant, yet they still produced embryos without a detectable variant; m.8993T>G showed skewed segregation (Spath et al., 2021). Hellebrekers and colleagues noted that most carriers of point variants will have some oocytes with loads below the 18% reference point (Hellebrekers et al., 2012).

Variant-specific distributions in embryos

The published embryo values compiled in the Between different embryos section show mostly extreme values for m.8993T>G and a substantial proportion of intermediate values for m.3243A>G. These distributions are observed data from individual families and cycles; they are not population probabilities and do not account for differences between families.

Implications for PGT-mt

  • Whether PGT-mt is feasible depends on the spread of heteroplasmy among a particular patient’s embryos, not on the average for a specific pathogenic mtDNA variant.
  • Mathematical models estimate risks and chances of success before a treatment cycle using maternal heteroplasmy as an input; the model was developed using pedigree data (Ji et al., 2023); these estimates rest on assumptions about bottleneck size and thresholds.
  • In the Newcastle programme, five patients undergoing PGT obtained no embryo with heteroplasmy below 30% (Hyslop et al., 2025). This observation shows that PGT-mt does not always yield an embryo that meets the chosen criterion.

No single mechanism — genetic drift, selection or restricted replication — has been established as a universal explanation of the bottleneck across all variants and developmental stages. The relative contribution of each mechanism has not been measured in humans and probably differs between variants and developmental stages.

Diagrams and models

Interactive model

Genetic bottleneck simulator

Model calculation

A simplified stochastic model showing how the effective pool size affects variation in heteroplasmy among oocytes. It does not predict the distribution among an individual patient’s embryos.

Virtual oocytes
0255075100Heteroplasmy in a simulated oocyte, %starting level

Median 30%; half of the values lie between 25% and 39%; range 10–50%. Theoretical standard deviation: 10.2 pp. (draw no. 1)

Mathematical model

Each virtual oocyte receives N segregating units drawn at random and independently from a pool in which the proportion of mutant mtDNA is h₀. The number of mutant units K follows a binomial distribution, K ~ Bin(N, h₀); the oocyte’s heteroplasmy is h = K / N. The mean of h is h₀ and its variance is h₀(1 − h₀) / N. This is a single Wright–Fisher sampling step; the Kimura distribution used to describe segregation in carriers generalises it to repeated drift (Otten et al., 2018).

K ~ Bin(N, h₀) · h = K / N · E[h] = h₀ · SD(h) = √(h₀(1 − h₀) / N)

Limitations of the model

  • N is a notional statistical quantity, not the physical number of mtDNA molecules in a cell; published estimates for carriers vary widely (for example, 10–145) (Otten et al., 2018).
  • The model includes random drift only: it has no selection, preferential replication, cell death or oocyte maturation, which appear to matter for some variants (Chapter 3).
  • Oocytes are modelled as independent and identically distributed; the model includes no within-family correlation, variation between cycles or age effect.
  • There is no measurement error, no limit of detection and no distinction between oocyte, embryo and biopsy.

Between different embryos →

From concepts to Atlas data

  • Between different embryos →

    Observed embryo heteroplasmy distributions for each variant — real published values, unlike the model above.

  • PGT-mt × PGT-A model →

    A scenario calculation: how many blastocysts are needed to obtain, with a given probability, at least one euploid blastocyst with low heteroplasmy.

Chapter references (17)

All DOIs were checked against PubMed records; exceptions are marked at the entry.

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