Main

Global warming is pushing sea surface temperatures and ocean stratifications to record levels1, with predictions that by 2100, much of the tropical and subtropical surface oceans will regularly exceed 30 °C (ref. 2). Such changes in ocean conditions threaten marine ecosystems, potentially leading to the extinction of key species due to profound and complex impacts on the competition and distribution of organisms3. Microscopic, unicellular phytoplankton are fundamental to the function of marine ecosystems as their photosynthesis generates the organic carbon consumed by other organisms. However, as future oceans warm and become more stratified and circulation patterns change, the flow of deep-water nutrients essential for phytoplankton growth may decrease4,5, potentially favouring smaller phytoplankton species that are more efficient at nutrient uptake6,7. This shift towards communities dominated by small phytoplankton is expected to alter carbon cycling within ecosystems as their rapid turnover and slow sinking rates may lead to increased nutrient cycling in surface waters6, less efficient transfer of carbon to higher trophic levels and reduced sinking of organic carbon to the deep ocean8. And yet, our understanding of how small phytoplankton will respond to future ocean temperatures remains largely based on laboratory studies using model organisms9,10, which cannot recapitulate the complexity of interactions and genetic diversity found in natural populations. Here we document the in situ thermal sensitivity of natural populations of the keystone cyanobacterium Prochlorococcus, revealing a decrease in division rate at high temperatures. Our numerical simulations predict that rising temperatures will decrease Prochlorococcus biomass production in future oceans, potentially triggering cascading effects throughout open ocean food webs.

The cyanobacterium Prochlorococcus is the smallest (0.5–1 µm) and most abundant photosynthetic organism on Earth. It inhabits over 75% of the world’s sunlit surface oceans, thriving in the nutrient-poor tropical and subtropical waters where it contributes nearly half of the phytoplankton biomass11. Due to its small size and ability to genetically adapt to a wide range of environmental conditions12, Prochlorococcus is predicted to reach even greater dominance in future warmer oceans owing to its potential range expansion towards the poles and an increased relative abundance under the low-nutrient conditions predicted for more stratified oceans13,14. The extent to which these predictions based on laboratory experiments reflect the true thermal sensitivity of Prochlorococcus in diverse, more complex communities remains uncertain, partly owing to the limited availability of cell division rate estimates for natural populations, a challenge compounded by the difficulties of conducting non-disruptive measurements at sea15.

Results

In situ thermal limits of Prochlorococcus

Over the past decade, we have deployed our continuous-flow cytometer, SeaFlow16, on 90 research cruises, to collect per-cell fluorescence and light scatter data—optical measurements that reveal cell type and cell size, respectively—for approximately 800 billion phytoplankton cells less than 5 μm in size, including Prochlorococcus (Methods), across 200,000 km of surface ocean17. We generated 180 cell division rate estimates for Prochlorococcus populations using hourly binned size distributions in a size-structured matrix population model18, a mathematical approach that tracks how cell size distributions change over time as cells grow and divide (Fig. 1, Supplementary Table 1 and Methods). These estimates are derived from changes in the relative cell size distribution rather than cell abundance, which avoids the confounding effects of mortality agents such as grazing. The model uses Bayesian inference and retains only estimates with strong model fit and convergence, excluding those with abrupt changes in size distributions that can arise when sampling across different water masses containing Prochlorococcus populations with distinct cell sizes. This non-disruptive approach requires no manipulations or incubations, providing in situ division rates comparable to estimates from dilution experiments and cell cycle analysis19,20,21,22. To broaden the spatial coverage of Prochlorococcus’s distribution range, we complemented our data with publicly available data from cell cycle analysis20,23,24,25 and dilution experiments that estimate Prochlorococcus division rates from shipboard incubations24,26,27,28,29,30,31,32,33,34,35,36 (n = 114; Extended Data Fig. 1).

Fig. 1: Global patterns in Prochlorococcus division rates (d−1) in surface waters.
figure 1

a, Geographic distribution of daily division rates derived from the matrix population model (n = 180 independent samples), along with publicly available data from dilution experiments24,26,27,28,29,30,31 (n = 103 independent samples) and cell cycle analysis20,23,24,25 (n = 11 independent samples). The vertical bars represent methodological uncertainties associated with the matrix population model and cell cycle analysis; uncertainty estimates were not reported for dilution experiments. The inset map shows sampling locations coloured by methodology. be, Relationships between division rates and environmental variables: daily average seawater temperature (°C) (b), daily average photosynthetically active radiation (light, µmol E m−2 s−1) (c) and phosphate (d) and nitrate (e) concentrations (nmol l−1). Temperature and light were directly measured in situ for all methodologies. Nutrient data sources varied by methodology: for the matrix population model, 21 out of 180 measurements came from direct observations and 159 out of 180 came from the Mercator-PISCES biogeochemical model; for cell cycle and dilution experiments, 65 out of 114 included measured nutrient data while the remainder was omitted from the plot. Statistical relationships were assessed using ordinary least squares regression with two-sided tests (α = 0.01). The black line in b shows a second-order polynomial regression fit (P = 5.746 × 10−9), while the black lines in ce show linear regression fits to the respective environmental factors. No adjustments for multiple comparisons were applied.

Our results reveal high variability in the division rates of Prochlorococcus across latitudes, highlighting the complex interactions of temperature, nutrient and light availability on its growth (Fig. 1a) and motivating evaluation of the individual effects of each of these parameters. We observed a notable nonlinear relationship between division rate and temperature (Fig. 1b and Supplementary Table 2), with an initial increase in division rate followed by a decline at high temperatures, a pattern consistent across multiple cruises, locations and methodologies. A second-order polynomial regression fit to the data reveals a significant positive linear term (1.58 ± 0.28, P < 0.001), supporting the previously observed increase of division rate with temperature20, but also a significant negative quadratic term (−0.85 ± 0.28, P = 0.003). Light intensity and nutrient concentrations showed less pronounced effects within the observed ranges, with non-significant terms in their regressions (Fig. 1c–e and Supplementary Table 2). Across all environmental conditions, in situ division rates of Prochlorococcus never exceeded 1.6 d−1, equivalent to a population doubling time of about 10.5 h, with the highest values observed in tropical Atlantic24 and Indian Oceans23.

Given the apparent impact of temperature on Prochlorococcus division rates, we analysed the maximum division rates (top 80%) across various sea surface temperatures for each method (that is, the matrix population model, dilution experiments and cell cycle analysis) (Fig. 2a). This approach minimized potential confounding effects of the methodology and environmental conditions to better determine the upper limit of the division rate at a given temperature (Extended Data Fig. 2). The analysis revealed that maximum division rates increased exponentially with rising temperature up to an in situ threshold of approximately 28 °C. Above this temperature, maximum division rates declined sharply, with a nearly threefold reduction by 31 °C, comparable to rates observed at ~19 °C. This decline appeared primarily driven by temperature (generalized additive model: P < 0.001; generalized linear model: P < 0.004), while the effects of photosynthetically active radiation (PAR) and phosphorus and nitrogen concentrations were not statistically significant within the observed ranges (Extended Data Fig. 2 and Supplementary Table 3). Importantly, we have not observed the high division rates predicted by exponential thermal curves (>2.5 d−1 at 30 °C; solid line in Fig. 2a) even in warmer regions such as the Indian Ocean, where nutrient conditions are more favourable (Extended Data Fig. 2), further supporting our findings of thermal limits in Prochlorococcus communities. Although environmental factors interact in complex ways and are difficult to disentangle in natural phytoplankton communities, the field-observed patterns mirrored the thermal responses of 13 Prochlorococcus culture isolates grown with sufficient light and nutrient-replete conditions37,38,39 (Fig. 2a). We should note that only 2 of these 13 isolates originated from regions where annual mean sea surface temperatures exceed 28 °C, indicating that our culture collection does not fully represent Prochlorococcus from the warmest waters (Extended Data Fig. 3). Similarly, most of our field measurements come from cooler subtropical waters rather than warmer tropical regions, so we might be missing important data on Prochlorococcus that live in the hottest parts of the ocean. Despite this geographical sampling bias, culture isolates often show broader temperature tolerances than their isolation environment would suggest40. The slightly lower division rates in cultures compared with natural populations further highlight the challenge of extrapolating laboratory findings to natural communities, as culture conditions cannot fully replicate the complex interactions with other marine microorganisms that influence Prochlorococcus growth in its natural environment. Notwithstanding these inherent limitations in both field sampling coverage of the warmest ocean regions and laboratory culture representation, the remarkable consistency between laboratory cultures and field observations across different methodologies and ocean regions indicates that Prochlorococcus growth rates probably do not increase exponentially beyond a temperature threshold of approximately 28 °C (solid line in Fig. 2a).

Fig. 2: Temperature-dependent responses in Prochlorococcus populations.
figure 2

a, Maximum division rate (top 80%, d−1) of field populations, estimated from the matrix population model (n = 100 independent samples, blue circles) and from data compilations of dilution experiments24,26,27,28,29,30,31,32,33,34,35,36 (n = 45 independent samples, orange circles), cell cycle analysis20,23,24,25 (n = 9 independent samples, red circles) and culture isolates37,38,39 (n = 94 independent samples, white squares) grown under nutrient-replete conditions, plotted as a function of daily average seawater temperature (°C). The solid and dashed lines represent the 99th quantile regression fits using a standard exponential curve and a metabolic theory approach, respectively. Shading around the dashed line indicates the standard deviation of 1,000 bootstrap replicates. b, Cell abundance (106 cells l−1) as a function of temperature, where points represent the median values of the top 80% of abundance measurements observed at each temperature bin. Data combine hourly binned SeaFlow measurements and compiled datasets14,23,43, with colour coding representing the number of observations at each temperature. The error bars show the 5th and 95th percentiles within the top 80% subset. The red boxes highlight the observed detrimental effects of warm temperatures on the organism (>28 °C). The inset maps show the geographical distribution of sample locations, with samples collected in water above 28 °C indicated in red.

Prochlorococcus loss at high temperatures

The thermal sensitivity observed in natural populations of Prochlorococcus can be captured using a metabolic reaction function (dashed line in Fig. 2a), which incorporates the thermal sensitivity of enzyme kinetics, directly linking temperature changes to changes in metabolic rates10. This unimodal thermal response better captures Prochlorococcus temperature dependence than the traditional exponential curve approach (mean squared error of 0.11 and 0.79, respectively) that uses a Q10 temperature coefficient—a measure of how much growth rate changes with a 10 °C increase (solid line in Fig. 2a, Supplementary Fig. 1 and Supplementary Table 4). However, this Q10 function fits better for Synechococcus, the second smallest phytoplankton, across many ecotypes (Extended Data Fig. 4). The Q10 formulation also fits better for species groups within other taxa (for example, diatoms, coccolithophores)41,42. By contrast, the exponential curve predicts unrealistically high maximum division rates for Prochlorococcus above 28 °C (solid line in Fig. 2a), overlooking its actual thermal sensitivity.

Building upon these observations, we investigated the relationship between slower division rates at higher temperatures and population abundances by combining our hourly average Prochlorococcus cell abundance data (n = 12,814) with those from compiled datasets14,23,43 (n = 5,386). We identified three distinct thermal responses: below 19 °C, Prochlorococcus abundance maxima (top 80%) increased exponentially with temperature; between 19 °C and 28 °C, abundance maxima leveled off despite exponentially increasing division rates, suggesting a proportional increase in mortality rates (Fig. 2a); and above 28 °C, maximum abundances began declining, with cell abundances reduced about twofold by 30 °C (Fig. 2b). Synechococcus abundances did not show a similar decline at high temperatures (Extended Data Fig. 5), maintaining populations in waters above 28 °C where Prochlorococcus abundances decrease. This differential response provides additional evidence against nutrient limitation as the primary driver of decline. If nutrient limitation at high temperatures were responsible, we would expect Synechococcus, with larger cell sizes and higher nutrient requirements, to be more severely affected than Prochlorococcus. This contrasting pattern supports our findings that direct temperature stress, rather than nutrient limitation, is the dominant factor causing the observed decline in both Prochlorococcus division rates and abundance at the warmest ocean regions.

Predicted Prochlorococcus future under climate change

We explored how our findings might affect future ocean ecosystems by integrating the observed Prochlorococcus thermal sensitivity into a comprehensive three-dimensional numerical ecosystem model within a global circulation framework42. The model simulates the distribution and fitness of many functional groups, including heterotrophic bacteria, autotrophs, mixotrophs and zooplankton types, linking physiological traits to biogeochemical function and cell size through size-dependent power laws (Supplementary Fig. 2 and Methods). Changes in population biomass are based on growth, grazing, mortality, sinking, and ocean fluid dynamics and mixing effects44. For all functional groups except Prochlorococcus, we incorporated exponential thermal response curves (Supplementary Fig. 3 and Supplementary Table 4) for both growth and grazing rates. This Q10 parameterization aligns with previous studies for all other autotroph functional groups, including Synechococcus45,46 (Extended Data Fig. 4). However, for Prochlorococcus specifically, we implemented the metabolic thermal response curve from our data, with decreased division rates above 28 °C (dashed line in Fig. 2, Supplementary Fig. 3 and Supplementary Table 4). To project future impacts, we compared a baseline ocean derived from pre-industrial conditions (1860; Methods) with end-of-century conditions under two different climate scenarios (Supplementary Table 5). The first scenario projects stabilized greenhouse gas concentrations at ~650 ppm CO2 equivalent by 2100 (similar to the Representative Concentration Pathways RCP 4.5), while the second assumes high emissions leading to CO2 equivalent concentrations of ~1,370 ppm by the end of the century (similar to RCP 8.5). These scenarios result in a 1.9 °C and 3.8 °C increase in average sea surface temperatures and a nearly 6% and 9% reduction in nutrient supply in the sunlit surface waters, respectively (Extended Data Fig. 6 and Methods).

Our model incorporating Prochlorococcus’s upper thermal limit predicts a substantial decrease in both depth-integrated biomass (Extended Data Fig. 7) and production (Fig. 3a,b,g,i and Extended Data Fig. 8) in the tropical regions where future surface temperatures are projected to exceed 28 °C for much of the year (Extended Data Fig. 6). By 2090–2100, Prochlorococcus production in tropical regions will decline between 17% and 51% depending on whether moderate or high warming scenarios unfold (Supplementary Table 6). Regions such as the Western Pacific Warm Pool face particularly severe impacts, with our model predicting a near-complete collapse of Prochlorococcus populations (Fig. 3g,i). Thermal stress, not decreased nutrient supply, drives this decline (Extended Data Fig. 9 and Supplementary Table 6), supporting our observations (Fig. 2b). Despite habitat expansion into warmer, higher latitudes, global Prochlorococcus production will decline by 10–37% depending on the climate scenario (Supplementary Table 6). These substantial changes exceed the interannual variability in model projections by an order of magnitude (Methods and Supplementary Table 6) and will occur even under a moderate warming scenario, highlighting the potential threat to these foundational organisms. These projections contrast sharply with simulations relying on the more typically used exponential thermal response curve (solid line in Fig. 2a, Supplementary Fig. 3 and Supplementary Table 4), which instead forecasts moderate increases in annual Prochlorococcus production (18–30% under different scenarios) (Fig. 3a,b,h, j, Extended Data Fig. 8 and Supplementary Table 6).

Fig. 3: Projected changes in annual phytoplankton biomass production between pre-industrial (1860) and future (2090–2100) conditions, based on alterations in temperature, nutrient supply, mixing and ocean circulation anticipated under a moderate and high warming scenario.
figure 3

af, Latitudinal change (%) in depth-integrated biomass production for Prochlorococcus (a,b), Synechococcus (c,d) and all other phytoplankton (e,f) using either a standard exponential curve (grey) or a metabolic reaction approach (red) that relates the Prochlorococcus division rate to temperature, with shading representing longitudinal variation from the mean (s.d.). gr, The corresponding maps illustrate the percentage change in depth-integrated annual biomass production for Prochlorococcus (gj), Synechococcus (kn) and all other phytoplankton (or) projected under the two thermal norm assumptions and two climate scenarios. The white areas in di indicate that the phytoplankton type does not exist in those regions either pre-industrially or by the end of the century. Values of 100% increase indicate an expansion in the geographical range.

As Prochlorococcus declines owing to the unimodal nature of its thermal norm, our model projects a compensatory increase from Synechococcus, seen in both increased biomass (Extended Data Fig. 7) and production (Fig. 3c,d,k,m). This compensation appears the strongest in tropical regions, where Prochlorococcus decline is most severe, resulting in an 11–34% increase in mean depth-integrated annual Synechococcus production across climate scenarios (Supplementary Table 6). Notably, this pattern of Synechococcus thriving in the very regions where Prochlorococcus populations collapse, such as in the Western Pacific Warm Pool, further supports that temperature stress, not nutrient limitation, is the primary driver of Prochlorococcus decline. As warming enables range expansion towards the poles, global Synechococcus production increases by 5–20% depending on the climate scenario (Fig. 3c,d,k,m and Supplementary Table 6). Larger phytoplankton, primarily picoeukaryotes, show modest changes with production decreasing 4–7% (Fig. 3e,f,o,q and Supplementary Table 6). These results contrast sharply with projections assuming exponential Prochlorococcus temperature response, with a 15–26% decrease in Synechococcus production and a 6–11% decrease for larger phytoplankton across climate scenarios (Fig. 3c–f,l,n,p,r and Supplementary Table 6).

Thermal adaptation potential of Prochlorococcus

We created an in silico warm-adapted strain with an increased thermal tolerance to evaluate the potential impacts of Prochlorococcus populations adapted to warmer temperatures that were not included in the current metabolic response model. We reasoned that these warm-adapted populations could come to dominate future oceans either because they currently exist within regions not covered in our current dataset or because they emerge over time through adaptation or mutation and selection in response to continued warming ocean conditions. We retained the metabolic response function for these warm-adapted strains, increasing the optimal temperature from 28 °C to 30 °C and the maximum division rates from 1.3 d−1 to 1.6 d−1 (Supplementary Fig. 4), a temperature shift comparable to that observed for Synechococcus following long-term thermal tolerance experiments47. Given that nutrient limitation has been shown to lower optimal temperature and reduce division rates in diverse species of phytoplankton, including cyanobacteria48, this thermal shift represents a reasonable upper bound on thermal adaption in Prochlorococcus. At the global scale, replacement of the observed thermal sensitivity (Fig. 2a) with the enhanced thermal adaptation into our global ecosystem model partially mitigates the negative impacts on Prochlorococcus production (Fig. 3), resulting in a projected 6% increase under moderate warming and a 7% decrease under high warming in global Prochlorococcus production (Fig. 4a,b, Extended Data Fig. 10 and Supplementary Table 6). Under the high warming scenario, Synechococcus production increased by only 2% when competing with warm-adapted Prochlorococcus strains (Fig. 4c,d) and the larger phytoplankton groups showed moderate production decreases (7–9%) under the same conditions (Fig. 4e,f). Enhanced temperature adaptation proved effective in maintaining Prochlorococcus populations in tropical regions where temperatures remained below the warm-adapted strain’s temperature threshold. However, even with increased thermal tolerance, significant production declines still occurred in the warmest tropical regions under the high warming scenario (15%; Extended Data Fig. 10 and Supplementary Table 6), suggesting that thermal adaptation may delay but not prevent the negative impacts of ocean warming on Prochlorococcus.

Fig. 4: Impacts of a hypothetical warm-adapted Prochlorococcus strain on projected biomass production.
figure 4

af, Latitudinal change (%) in depth-integrated biomass production for Prochlorococcus (a,b), Synechococcus (c,d) and all other phytoplankton (e,f) comparing the standard metabolic reaction model (blue) with a warm-adapted variant (red) for Prochlorococcus. The lines represent the mean across longitudes, and shading indicates longitudinal variation (±s.d.). Both projections use the same future climate scenario (2090–2100) and pre-industrial baseline (1860) as Fig. 3.

Discussion

The thermal sensitivity observed in natural populations of Prochlorococcus suggests fundamental physiological constraints that distinguish it from larger phytoplankton. Our findings show that Prochlorococcus division rates increase exponentially with temperature up to approximately 28 °C, then decline sharply at higher temperatures. This thermal response differs markedly from that of Synechococcus and other phytoplankton groups, whose growth rates continue to increase at temperatures where Prochlorococcus begins to decline.

This differential thermal sensitivity probably reflects distinct evolutionary histories and habitat adaptations. Prochlorococcus evolved in relatively stable tropical and subtropical environments where temperature fluctuations are minimal, potentially favouring resource efficiency over thermal versatility. Unlike coastal and high-latitude phytoplankton that experience substantial temperature variations and maintain broader thermal tolerances, Prochlorococcus shows specific vulnerabilities at high temperatures. At 30 °C, Prochlorococcus isolates from warm regions such as the Sargasso Sea and Red Sea show suppressed photosystem gene expression49 and disrupted circadian regulation50, both critical for carbon fixation. By contrast, Synechococcus thrives at high temperatures, probably owing to proteomic adaptation that helps them minimize oxidative stress51 and resource reallocation strategies that maintain growth as temperature increases52. These physiological differences stem from divergent evolutionary trajectories: Prochlorococcus underwent genome streamlining, shedding many stress-response genes to minimize resource requirements while optimizing performance within a narrower environmental range. Synechococcus, however, maintains a more complex cellular machinery that, although costlier to maintain, provides greater resilience across variable conditions, including high temperatures. This evolutionary trade-off explains why Prochlorococcus, despite its dominance in stable nutrient-poor regions, may be more vulnerable to warming than Synechococcus.

These evolutionary trade-offs raise the critical question of whether Prochlorococcus can overcome its thermal limits in the near future. Despite its remarkable genetic diversity across ecotypes12, the streamlined genome that enabled Prochlorococcus to dominate nutrient-poor waters may now limit its capacity to adapt to rapid warming, as evidenced by its reduced abundance in the warmest ocean region (Fig. 2b). Our model incorporating a hypothetical warm-adapted strain (with a 2 °C increase in thermal optimum) shows that adaptive evolution could partially buffer Prochlorococcus populations against warming impacts. However, even with this adaptation, significant declines are still projected in tropical regions, highlighting the limitations of evolutionary rescue when faced with rapid environmental change. For approximately 150 Myr, Prochlorococcus has evolved to thrive in nutrient-poor conditions, minimizing cell and genome sizes to reduce resource requirements, the very genomic streamlining that may now constrain its thermal adaptability. While Prochlorococcus probably persisted through past extreme climate events, such as the Early Eocene Climate Optimum when tropical seawater temperatures reached 35 °C (ref. 53), it probably did so by shifting polewards to cooler waters, a strategy that our ecosystem simulation also predicts for future warming (Fig. 3). Whether beneficial mutations could sweep through global populations within the timeframe of projected warming remains uncertain, especially given the unprecedented rate of anthropogenic warming and potential fitness trade-offs associated with thermal adaptation.

While our analysis provides evidence for thermal limits in Prochlorococcus, we must acknowledge several methodological limitations that complement the evolutionary considerations discussed above. Our field observations capture integrated responses of mixed communities rather than individual ecotypes, potentially masking the performance of rare, heat-tolerant variants. Strains with higher thermal tolerance may exist but remain uncommon owing to environmental trade-offs. Our sampling also presents geographic limitations. Laboratory studies disproportionately represent easily cultured ecotypes, with those from the warmest tropical regions remaining underrepresented (Extended Data Fig. 3). Similarly, while our field measurements spanned various ocean regions, many consistently high-temperature tropical areas remain unexplored. Despite these sampling limitations, our observations across the tropical Pacific consistently show reduced division rates at temperatures above 28 °C. The consistency of this pattern across diverse natural communities suggests a fundamental thermal limitation rather than an artefact of sampling bias. This thermal vulnerability demands serious consideration given Prochlorococcus’s global significance.

Prochlorococcus’s thermal limitation potentially has profound implications beyond the species itself. The predicted decline of Prochlorococcus could trigger cascading effects throughout marine food webs, particularly given the lack of functional redundancy within the Prochlorococcus ecological niche54. While our model predicts some compensatory response from Synechococcus, the overall community shift would be substantial. As warming oceans favour larger phytoplankton expanding into the ecological niche currently occupied by Prochlorococcus (Fig. 3e,f,o,q and Extended Data Fig. 7), this fundamental shift at the base of the food web could alter the composition and abundance of grazers, impacting predators higher in the food chain55, including fish populations56. In addition, a reduction in Prochlorococcus populations may disrupt mutualistic relationships with other organisms such as SAR11 (ref. 57), the ocean’s most abundant heterotrophic bacteria, potentially destabilizing the microbial community58 and altering carbon cycling59. Ultimately, a decline in Prochlorococcus production could have far-reaching consequences beyond a simple shift in species abundance, revealing the complex and interconnected nature of microbial communities. These findings underscore the importance of considering thermal constraints when projecting marine ecosystem responses to climate change, as our results suggest that Prochlorococcus, despite its ecological success and numerical dominance, may be sensitive to the temperature increases projected for tropical oceans in coming decades.

Methods

Phytoplankton abundance and composition

Data collection

We deployed the SeaFlow shipboard flow cytometer16 on 90 cruises from 2010 to 2023. The instrument continuously sampled seawater from the ship’s underway intake, located at 3–8 m below the surface. Seawater was pumped through a 100-µm stainless steel mesh filter to prevent clogging of the 200-µm sampling nozzle. We continuously injected 1-µm yellow-green Fluoresbrite microspheres (Polysciences) into the flow stream for scattering and fluorescence signal normalization. Particle emission was detected using two position-sensitive detectors for optimal focus determination. We measured red fluorescence (692/40 nm bandpass filter), orange fluorescence (572/28 nm bandpass filter) and forward light scatter (457/50 nm bandpass filter). Data were stored in 3-min intervals, yielding a sampling resolution of approximately 1 km along the cruise track (based on a ship cruising at ~ 20 km h−1).

Data analysis

Raw data were processed to identify in-focus optimally positioned particles within the SeaFlow virtual core17. Optimally positioned particle analysis was performed using the R package Popcycle (version 4.7.3) available on GitHub. We defined five sets of gates based on forward light scatter, red fluorescence and orange fluorescence to identify 1-µm beads, Prochlorococcus, Synechococcus and small eukaryotic phytoplankton (<5 µm). Gate coordinates for each file were saved and stored in a structured query language (SQL) database. The equivalent spherical diameter (ESD) of each cell was estimated from forward scatter using the Mie light scatter theory. We then converted the ESD to carbon quotas using volume-to-carbon relationships for small phytoplankton17. Prochlorococcus size distributions were obtained by combining data collected every 3 min over each 1-h period (n = 12,814 hourly binned data points) to ensure robust statistical representation of the particle size distribution, with each hourly bin typically containing measurements from more than 10,000 individual cells.

Throughout our sampling campaigns, we validated SeaFlow cell abundance measurements against conventional flow cytometry (that is, BD Influx) for samples collected from both high- and low-temperature regions (n = 683; Supplementary Fig. 5). These validation efforts showed a good agreement between methods for Prochlorococcus abundance measurements across the temperature range, showing that dim Prochlorococcus cells in nutrient-poor warm waters were sufficiently resolved by our instrumentation for the purpose of this study.

Ancillary data

SeaFlow data were complemented with underway sea surface temperature measurements from shipboard thermosalinographs. These measurements were either broadcast in real time over the ship’s network or retrieved from the Rolling Deck to Repository. The temperature data recorded simultaneously with SeaFlow measurements are available along with the SeaFlow data on GitHub (https://github.com/seaflow-uw/seaflow-sfl/tree/master/curated).

We complemented cell abundances derived from SeaFlow data with the Global Cyanobacteria dataset hosted on the Simons Collaborative Marine Atlas Project60 (CMAP) database (that is, the tblFlombaum table), which contains global observations of Prochlorococcus abundance collected from 103 cruises14. As this dataset contains satellite-derived sea surface temperature data, we selected only samples from the upper 10 m to ensure appropriate temperature matching and excluded all zero values and empty entries (n = 5,125). We also incorporated two additional cruises in the Indian Ocean23,43 (n = 261) which included temperature data from the shipboard thermosalinograph. For these additional Indian Ocean datasets, we included all depth measurements with available temperature data.

Size-structured matrix model of division rates

Model parameters

We applied a size-structured matrix population model following the approach described in a previous study18, to estimate phytoplankton division rates. This category of model has shown its suitability for estimating in situ phytoplankton division rates for Prochlorococcus18,20, Synechocococus19,61 and mixed populations of small eukaryotic cells22,62 in a wide range of environmental conditions, from estuarine to coastal to open ocean environments, and validated using culture experiments18, cell cycle analysis20 and dilution experiments19. The latter indicates that the effects of size-specific mortality agents, if any, on the relative cell size distribution do not affect cell division estimation.

The size-structured matrix population model mechanistically simulates the evolution of the size distribution over a day–night cycle. The model discretizes cell counts across size classes and time using the parameter Δv and time using the parameter Δt. It quantifies the rates of the three key biological processes (cell division, carbon fixation and carbon loss), which are represented by the parameter vector θ = (θδ, θγ, θρ, ω0). These parameters, along with a concentration parameter σ (which allows for overdispersion in the data), determine the dynamics of the model. Below is a breakdown of the modelled processes:

  1. (1)

    Cell division (δ): Division rates are size dependent, reflecting the probability of cells transitioning to subsequent life-cycle stages. The model assumes a monotonically increasing division rate as a function of cell size.

  2. (2)

    Carbon fixation (γ): Carbon fixation rates are determined by light availability (PAR measurements) and cellular carbon content. This captures diel cycle dynamics and phytoplankton growth rates. The model incorporates a power–law relationship between carbon fixation and cell size.

  3. (3)

    Carbon loss (ρ): The model accounts for carbon loss through respiration and exudation, estimating rates separately for each size class. This reflects cell shrinkage due to metabolic processes other than division.

Prochlorococcus size distribution was obtained by combining data collected every 3 min over each 1-h period. These distributions were then discretized into 30 size classes based on the log of their carbon quotas, ranging from 80 fgC to 260 fgC per cell. This range was selected to fully encompass the variation in Prochlorococcus cell size observed in the SeaFlow dataset. We chose the volume bins and a time step of 10 min to ensure that cells would probably undergo only a single transition at a time within the model.

Data analysis

We used Bayesian inference, implemented through the Stan software package and Hamiltonian Monte Carlo algorithms, to process the data. A total of 6 Hamiltonian Monte Carlo chains were run for 2,000 Markov chain Monte Carlo iterations. This approach strikes a balance between computational efficiency and the complexity of our model. A list of model parameters and priors is available in Supplementary Table 1.

We implemented rigorous quality control measures to ensure accuracy and reliability of our model estimates. These measures included:

  1. (1)

    Model convergence: Samples with poor model convergence (R-hat > 1.1) were excluded, as this indicated potential unreliability of model-derived estimates63.

  2. (2)

    Sample adequacy: Samples with insufficient cell counts (total number of particles counted over 1 h <10,000) were excluded from analysis.

  3. (3)

    Data completeness: We excluded datasets with large gaps in temporal coverage (>4 h).

  4. (4)

    Data integrity: We excluded 24-h periods containing abrupt shifts in cell size distributions. As phytoplankton cells typically increase their size by no more than a factor of two during a complete day–night growth cycle (that is, cells divide when they reach a critical size), larger or sudden changes in mean population size strongly indicate that we were sampling different populations with inherently distinct cell size characteristics. We detected these shifts using a change point detection method specifically developed for environmental flow cytometry data64. While most of these shifts are usually filtered by our model convergence criteria, this additional step provided additional assurance that our estimates reflected genuine biological processes rather than sampling artefacts.

  5. (5)

    Biological consistency: We examined the correlation between carbon fixation patterns estimated by the model and division rates. As carbon fixation during daylight hours drives cell growth, which subsequently enables division, samples showing weak or absent correlations between these processes were flagged for potential anomalies, as this might indicate that factors other than normal physiological processes were affecting the size distributions.

Ancillary data

Prochlorococcus division rates were complemented with dissolved inorganic nutrient concentrations (nitrate plus nitrite and phosphate). For division rates obtained from the SeaFlow data, nutrient data were obtained mostly from Mercator-PISCES biogeochemical model forecasts (¼° resolution), with 21 out of 180 data points from in situ measurements collected during research cruises in which the SeaFlow instrument was deployed. The PISCES model is a widely used tool for simulating marine biological productivity and the biogeochemical cycles of key nutrients (carbon, oxygen, phosphorus, nitrogen, silicon and iron) in the global ocean, and has been extensively validated against a wide range of available observations, including in nutrient-poor regions65,66. Both in situ observations and model estimates are hosted in the CMAP database60. The specific CMAP datasets for measured nutrient values were the following:

  • tblKOK1606_Gradients1_Nutrients

  • tblMGL1704_Gradients2_Nutrients

  • tblKM1906_Gradients3_Organic_Inorganic_Nutrients

  • tblTN397_Gradients4_NutrientsAndParticulates

  • tblGradients5_TN412_NutrientsUW

  • tblTN398_nutr

  • tblHOT_CTD

and Mercator_Pisces_Biogeochemistry_Daily_Forecast_Nut for modelled data.

We extended our SeaFlow-derived Prochlorococcus division rates with a data compilation of in situ dilution experiments24,26,27,28,29,30,31,32,33,34,35,36 and cell cycle analysis20,23,24,25 (Extended Data Fig. 1). This dataset represents 114 estimates of Prochlorococcus division rates. For 65 out of 114 of these data points, measured environmental variables, including temperature, nitrate and phosphate concentrations, and PAR values, were provided directly within the compiled studies, based on field observations rather than model estimates or remote sensing data. These complementary datasets expand our geographic coverage beyond the North Pacific region where most SeaFlow deployments occurred, providing broader representation of different oceanic regimes.

We incorporated publicly available data on Prochlorococcus division rates derived from 13 different isolates cultured under nutrient-replete conditions37,38,39 (Extended Data Fig. 3). These isolates represent various ecotypes including both high-light- and low-light-adapted strains from different ocean regions. Of these 13 isolates, 2 originated from regions where annual mean sea surface temperatures exceed 28 °C, while others were isolated from cooler regions. This compiled dataset includes over 702 estimates of division rates under various temperature and light conditions. While isolate-based estimates are often lower than rates measured in situ, they provide valuable insights into physiological responses under controlled laboratory conditions and are used to test assumptions regarding how division rates respond to environmental variations.

Modelling the temperature response of the maximum division rate

Model parameters

The change in the cell division rate (μ) with temperature was characterized with either an exponential function (Eppley equation), an exponential function with mortality (Eppley–Norberg equation) or a metabolic theory of ecology (Hinshelwood equation), as described previously67:

$$\begin{array}{cc}\mu ={{ae}}^{b(T-{T}_{0})} & ({\rm{Eppley}})\end{array}$$
$$\begin{array}{cc}\mu =a{e}^{b\left(T-{T}_{0}\right)}\left(1-\left(\frac{T-{T}_{c}}{w/2}\right)^{2}\right) & ({\rm{Eppley}}{-}{\rm{Norberg}})\end{array}$$
$$\begin{array}{cc}\mu =A1{e}^{-E\;1/{RT}}-A2{e}^{-E2/{RT}} & ({\rm{Hinshelwood}})\end{array}$$

where T represents the temperature and a represents the maximum division rates at T0 (typically 20 °C), b is the exponential change in division rate with increasing temperature, Tc corresponds to the maximum of the quadratic portion of the equation, w is the thermal niche width (that is, the range of temperatures over which the division rate is positive), R is the gas constant (8.315 J mol−1 K−1), A1 and A2 are related to entropy and E1 and E2 are related to enthalpy.

Parameter estimation

To parametrize the coefficients, we fitted the 99th quantile regression to capture the division rate maxima at a given temperature. The 99th quantile is commonly used studying phytoplankton response to temperature, as it helps identify the upper limits of its thermal tolerance41,68. Parameters were estimated using a least squared approach and a differential evolution algorithm for optimization, using the Deoptim package in R69. The Hinshelwood and Eppley–Norberg approaches yielded similar curves (Supplementary Fig. 1).

Temperature as the primary driver of maximum division rates in Prochlorococcus

Our goal was to evaluate whether the observed decline in division rates at higher temperatures was primarily driven by temperature or by other covarying factors. The data were binned by 0.25 °C intervals of seawater temperature, and we analysed the 80th percentile division rate across each bin. The 80th percentile was chosen over the 99th percentile to increase the sample size for statistical analysis while still focusing on the upper range of division rates. We used two complementary statistical models:

  1. (1)

    A generalized linear model was constructed using the glm function in R, incorporating polynomial terms for temperature, PAR, nitrate and phosphate. This allowed us to capture potential nonlinear relationships between these factors and division rates within a linear framework. Before the model fitting, all environmental factors were rescaled to have a mean of zero and a standard deviation of one to facilitate the comparison of their relative importance on division rates. To assess the robustness of model results, we applied a bootstrapping technique with 1,000 replicates, generating standard deviations for the model coefficients. Model fit was assessed using standard diagnostic plots and summary statistics.

  2. (2)

    A generalized additive model was constructed using the mgcv package in R, incorporating smooth terms (that is, estimated degree of freedom) for temperature, PAR, nitrogen (nitrate and nitrite) and phosphorus (phosphate) concentrations. A simulation-based test with 1,000 replicates indicated sufficient basis dimensions for all smooth terms, suggesting that the model adequately captured the complexity of the relationships. Model selection was performed using restricted maximum likelihood, and the basis dimension (k) was checked to ensure adequate model complexity.

Global climate change simulation

Ecosystem model

We used the Massachusetts Institute of Technology (MIT) marine ecosystem model (Darwin), including the cycling of carbon, nitrogen, phosphorus, silicon, iron and oxygen through inorganic, organic detritus and 50 plankton types, modified from previous studies45,70. The model includes 31 phytoplankton types, analogues of the pico-cyanobacterium Prochlorococcus, Synechococcus, 2 sizes of green algae (picoeukaryotes), 5 sizes of coccolithophores, 5 diazotrophs, 9 diatoms and 8 mixotrophic dinoflagellates (Supplementary Fig. 2). To represent the wide range of phytoplankton sizes, we defined 14 size classes ranging from 0.6 µm to 104 µm ESD, evenly distributed on a logarithmic scale. The model also captures trophic interactions through 3 size classes of heterotrophic bacteria (0.4 µm to 0.9 µm ESD) that remineralize the organic matter and 16 size classes of zooplankton (4.5 µm to 1,636 µm ESD) that graze on prey following a Holling type II function71.

Phytoplankton growth parameters are allometrically defined with functional group specifics72. Growth rates are influenced by multiple potentially limiting nutrients (dissolved inorganic nitrogen, phosphate, iron and silicic acid) using Liebig’s law of the minimum (growth limited by the scarcest resource) and parameterized with a Monod function (a mathematical relationship describing nutrient-limited growth). Nutrient half-saturation coefficients are allometrically assigned, favouring smaller phytoplankton with the highest nutrient affinity. Phytoplankton growth is also a function of spectral light and photoacclimation72,73 with functional groups showing distinct absorption patterns based on their specific pigment composition. Temperature affects all biological rates, including phytoplankton growth rates, zooplankton grazing rates and other loss rates. While these rates incorporate Q10-based temperature dependencies, whose uncertainties and impacts on projections have been assessed in previous studies42,45, our analysis shows that the choice of thermal response functions (that is, with or without thermal limits) represents a more significant source of uncertainty. This is particularly evident for Prochlorococcus, in which we evaluated two distinct thermal response curves: a conventional exponential function (solid blue curve; Supplementary Fig. 3) and a metabolic function incorporating thermal limits (dashed blue curve; Supplementary Fig. 3), both derived from in situ and laboratory studies (Fig. 2a). For Synechococcus, we use an exponential thermal response curve (black curve; Supplementary Fig. 3) derived from in situ dilution experiments27 and laboratory studies42. For all non-pico-cyanobacteria, we use exponential thermal growth functions (Supplementary Fig. 3 and parameters in Supplementary Table 4) derived from laboratory observations45.

Climate model and simulation procedure

Our study integrates the biological and biogeochemical components of the Darwin ecosystem within an Earth system model of intermediate complexity, the MIT Integrated Global System Model (IGSM)74,75,76. The IGSM couples the MIT general circulation model77, a three-dimensional ocean circulation model at a coarse resolution configuration (2° by 2.5° horizontally, 22 vertical levels that range from 10 m at the surface to 500 m at depth)76, with a simplified representation of the atmospheric dynamics, physics and chemistry, terrestrial water, energy and biogeochemical processes78. The Darwin model is run in ‘offline’ mode using physical ocean fields (for example, circulation, mixing, salinity and temperature) from representative members of an ensemble of IGSM simulations. The ocean component of the IGSM shows a realistic climatology and year-to-year variability (for example, El Niño-Southern Oscillation) with frequency, seasonality, magnitude and patterns in general agreement with observations75. As is typical with climate change studies, the IGSM performed a ‘control’ simulation in which greenhouse gas and aerosol concentrations were held constant at 1860 levels. This pre-industrial control shows interannual variability but lacks any long-term warming trends or circulation changes. In addition, the IGSM performed a transient simulation from 1860 to 2100 under observed pre-industrial changes in greenhouse gas and aerosol concentrations followed by two future greenhouse gas and aerosol emission scenarios, a moderate and high scenario similar to Intergovernmental Panel Climate Change RCP 4.5 and 8.5. These simulations have been previously described and evaluated in detail75. Following the approach in a previous study45, we conducted paired ecosystem model experiments (20 years each) to contrast pre-industrial and projected future ocean conditions (Extended Data Fig. 6). This capitalized on the significant differences in ocean physics between the pre-industrial control run of the IGSM and its end-of-century moderate and high warming scenarios. We initialized each simulation with nutrient and detritus fields from previous transient simulations79, ensuring consistency with pre-industrial or future conditions. Plankton types were initialized at low abundances, and robust ecosystem structures were established within 3 years. Our results represent averages over the past 10 years of each simulation. This averaging mitigates the impact of interannual variability on the comparison between pre-industrial and future conditions.

Series of simulations

We perform a series of simulations varying both physical conditions and the thermal response function used for Prochlorococcus (Supplementary Table 4). We refer to simulations with constant 1860 greenhouse gas and aerosol concentrations (control run) as ‘pre-industrial’ and those based on projected end-of-century physical conditions as ‘2090–2100’. Simulations in which Prochlorococcus maximum division rates follow an exponential temperature function are termed ‘exponential’, while those using a metabolic function with an upper thermal limit are termed ‘metabolic’. Our initial set of six simulations (two paired experiments; Supplementary Table 5) are the ones discussed in the main text: ‘exponential’ pre-industrial, moderate and warming scenarios, and ‘metabolic’ pre-industrial, moderate and high warming scenarios. Phytoplankton distributions and production in pre-industrial simulations align well with real-world observations (Extended Data Figs. 7 and 8), as shown in previous studies45,70. While the computational demands of this global three-dimensional ecosystem model preclude comprehensive parameter sensitivity analyses, we note that the projected changes between ‘pre-industrial’ and future climate simulations exceed the model’s interannual variability by an order of magnitude (Supplementary Table 6). This, combined with the model’s demonstrated skill in reproducing present-day distributions, provides confidence in the robustness of our key findings.

To isolate the direct impact of temperature change on Prochlorococcus, we conducted two additional simulations. In these experiment, we maintained pre-industrial circulation patterns and nutrient concentrations to control for changes in nutrient supply, while allowing biological rates (including Prochlorococcus growth rate) to respond to projected end-of-century warming for both climate scenarios (Supplementary Table 5). In the main text, we compare the results of the 2090–2100 simulations to their paired pre-industrial counterparts (Figs. 3 and 4 and Extended Data Figs. 7 and 10).

Reporting summary

Further information on research design is available in the Nature Portfolio Reporting Summary linked to this article.