Population III Stars: The Universe’s First Generation
Linas JuozėnasShare
Knowledge Ark · Universe · Chapter 02 / Article 02
Population III stars The universe’s first generation
Born from pristine gas, the first stars brought new light, new elements, and new possibilities to the young universe.
What happens when the gas has no stellar past?
Every familiar star formed in a universe already changed by other stars. The first generation began with a much simpler chemical inventory.
Its clouds contained mostly hydrogen and helium, with traces of light elements left from the early universe. Their birth gas had not received the carbon, oxygen, silicon, or iron supplied by previous stellar generations. That difference changed how the gas cooled, how stars gained mass, and what their light could do.
These are Population III stars. Understanding them connects the first star-forming clouds to the later chemical richness of galaxies, rocky planets, and minerals.[1]
What does Population III mean?
In astronomy, metals are elements heavier than helium. A star’s metallicity describes its abundance of those elements.
Population III stars formed from gas without previous stellar enrichment. They are commonly called “metal-free,” although primordial gas contained trace lithium. The term is conventional shorthand for an essentially pristine starting composition.
This is a definition based on birth material. It does not require all Population III stars to have formed at one moment, or every region to have stopped making them together.[1]
Population III
Stars born from essentially pristine gas, before enrichment by previous stars.
Population II
Generally old, metal-poor stars whose birth material had already been enriched.
Population I
More metal-rich stars, including the Sun, formed from chemically enriched gas.
How did pristine gas make stars?
The first stars are generally expected to have appeared within the first few hundred million years after the Big Bang. Their emergence marks cosmic dawn, bringing the starless Dark Ages to an end.
Early sites included dark matter minihalos with total masses of roughly 100,000 to a million solar masses, depending on conditions. Most of that mass was dark matter, not a single future star.[1], [2]
Gravity gathered gas, but gas pressure resisted contraction. Cooling allowed the cloud to lose energy and become denser. In typical minihalos, small amounts of molecular hydrogen, H2, supplied an important route for that heat to escape.[2]
The absence of stellar enrichment changed the available cooling channels. It did not prevent the gas from forming disks or breaking into smaller star-forming structures.
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01 · Gather
Gas collects inside a halo
A dark matter concentration provides a gravitational well. The amount and motion of the incoming gas influence what can happen at its center.
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02 · Cool
The cloud loses heat
Molecular emission allows contraction. At higher temperatures, atomic cooling can also become effective.
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03 · Grow
Protostars gain mass
A small protostar can grow through continued gas accretion. A surrounding disk may fragment into companions, producing a multiple system.[1], [4]
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04 · Respond
Starlight changes the supply
Ultraviolet radiation can heat gas and evaporate parts of the accretion flow. This feedback can slow or halt growth.[3]
These processes overlap. The final stellar masses depend on the cloud, the accretion history, interactions between protostars, and feedback.
A closer look at the cooling temperatures
In typical primordial minihalo conditions, H2 cooling can bring gas to around 200 K. Atomic hydrogen cooling becomes efficient at temperatures of roughly 10,000 K in hotter halos. Other molecules, including HD, can allow additional cooling under some conditions. These are characteristic regimes, not universal temperature limits.[1]
How massive, hot, and long-lived were they?
Many models predict that early pristine environments favored more massive stars than typical star-forming regions today. But a population can favor high masses while still including smaller members. Its mass distribution—how many stars form at each mass—remains a central uncertainty.[1], [4]
Of solar masses in many models
This is a commonly predicted range for massive members, not an observed rule or a lower limit for all Population III stars.
Hot, luminous massive stars
Some massive, metal-free main-sequence models approach surface temperatures of 100,000 K, producing abundant ionizing photons.[5]
A brief life for a massive example
A star around 100 solar masses can use its nuclear fuel in only a few million years. Smaller stars can live much longer.[5]
Massive stars consume fuel rapidly because their luminosities are so high. Their composition also affects their internal structure and the radiation that escapes. Many massive Population III models are hotter and more compact than metal-rich stars of comparable mass, although their properties change as they evolve.[5]
There was more than one possible ending
Massive Population III stars could finish their lives in several ways. Birth mass matters, but so do core structure, rotation, mass loss, and interactions with a companion. These are possible evolutionary paths, rather than a universal chart with fixed boundaries.[6], [7]
Core-collapse supernova
When the core can no longer support itself, it collapses. If an explosion successfully ejects the outer material, newly made elements can escape into the surroundings.
Pulsational pair instability
In certain massive cores, the creation of electron–positron pairs destabilizes the star and can trigger pulses that eject shells. The star survives the pulses for a time before its later evolution.
Pair-instability supernova
Pair creation weakens the pressure response in a sufficiently massive, hot core. Contraction triggers explosive burning that can release enough energy to tear the entire star apart.
Collapse into a black hole
Some stars can collapse with a weak explosion or without a successful explosion. Much of their material falls into the black hole instead of enriching the surrounding gas.
What about the familiar 140–260 solar-mass range?
Classic nonrotating models placed complete pair-instability disruption at initial masses of roughly 140–260 solar masses, corresponding to helium cores of about 64–133 solar masses. These figures are useful reference points, but the mapping from birth mass to core mass changes with stellar evolution assumptions.[6], [7]
These dramatic endings concern massive stars. Any low-mass members would evolve on much longer timescales and follow different paths. The first stars therefore cannot all be described as short-lived supernova progenitors.
How did the first stars change the universe?
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They changed nearby gas
Radiation and feedbackHot stars ionized and heated their surroundings, creating local regions of ionized hydrogen. They helped initiate the longer process of reionization, but their total contribution relative to later stars remains uncertain. The first starlight and the reionization of the wider universe were distinct milestones.[1], [3]
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They expanded the chemical inventory
Stellar enrichmentStars that expelled material spread newly synthesized elements into their surroundings. Carbon, oxygen, silicon, iron, and other products became available to later clouds. Their proportions depended on the progenitor and its fate; a collapse with little ejection could leave a much weaker chemical imprint.[6], [10]
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They altered future star formation
New cooling channelsHeavy elements and newly formed dust offered additional ways for gas to cool, encouraging fragmentation under suitable conditions. There is no single metallicity threshold that applies to every cloud: elemental ratios, dust properties, gas density, and radiation all matter.[8]
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Some left black hole seeds
A possible route to later growthStellar-remnant black holes could grow by accreting gas or merging. They are one proposed starting point for early supermassive black holes, alongside other seed pathways. Producing a stellar remnant does not automatically explain the enormous masses seen in young quasars.[9]
The wider chemical story eventually leads to the ingredients of rocky planets and minerals. It required continued stellar evolution and recycling across many environments.
How do astronomers search for them?
The most massive first stars disappeared long ago, but their light can still be traveling toward us. At great distances, individual stars are extremely faint and their light blends with that of their surroundings. Astronomers therefore use several complementary approaches.
Spectra of early star-forming regions
JWST can examine redshifted ultraviolet and optical features in the infrared. Strong helium recombination emission can point to an energetic ionizing source, while weak metal lines help constrain the gas composition.
Both must be interpreted together: other sources can produce hard radiation, and a missing line may simply fall below the detection limit.[5], [11]
Chemical fossils
A long-lived star born from gas enriched by an early explosion can retain clues to that event in its element abundances. Astronomers compare patterns in metal-poor stars with predicted stellar yields.
Such a star can be a descendant of Population III. Reconstructing its ancestry requires accounting for mixing and possible later changes to its surface.[10]
Ancient explosions
A distant pair-instability supernova could provide another route to studying a massive early star. Proposed searches also include some gamma-ray bursts associated with stellar collapse.
Brightness or high redshift alone would not establish a pristine progenitor. The event’s spectrum, evolution, and environment would all matter.[1], [6]
Population III is a birth-composition category, so searches need not be restricted to one fixed redshift range. Isolated pockets of pristine gas could continue forming such stars after neighboring regions had already become enriched.[1]
Hebe: a promising clue near GN-z11
What the observations show
JWST follow-up observations reported in 2026 confirmed helium emission from a compact region nicknamed Hebe, near the distant galaxy GN-z11. Hydrogen emission independently supported the identification, placing the source at a redshift of about 10.6.
The reported spectra showed no detected metal lines. The authors favored Population III stars as an explanation for the strong helium emission, while some black hole scenarios could not be completely excluded.[11], [12]
What are researchers still trying to learn?
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What was the mass distribution?
How often did primordial clouds make very massive stars, smaller companions, or long-lived survivors?
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How did the environment matter?
How did accretion, nearby radiation, and interactions within a stellar group change the final outcomes?
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How much material escaped?
Which kinds of explosions dominated early enrichment, and how quickly did their products mix into fresh gas?
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Which signatures are distinctive?
What combination of spectra, chemical patterns, and stellar models can securely identify pristine star formation?
Answering these questions requires bringing observations and simulations together. A convincing account must explain both the light from distant systems and the chemical inheritance recorded in later stars.[1], [10], [11]
The first stars changed what could form next.
Their radiation reshaped nearby gas. Their evolution made new elements, and the stars that expelled those elements began enriching future stellar nurseries. Some left compact remnants that could grow further.
The next article follows the environments that hosted this activity: early minihalos and protogalaxies, where gas, gravity, and the first stars began assembling young galactic systems.
Sources and further reading
- Klessen & Glover (2023) — The first stars: formation, properties, and impactResearch review of pristine gas, first-star formation, stellar properties, and feedback.
- Abel, Bryan & Norman (2002) — The Formation of the First Star in the UniverseA foundational simulation of primordial gas cooling and collapse inside a minihalo.
- Hosokawa et al. (2011) — Protostellar Feedback Halts the Growth of the First Stars in the UniverseHow a growing star’s ultraviolet radiation can limit its supply of gas.
- Stacy & Bromm (2014) — The First Stars: A Low-Mass Formation ModeSimulations exploring a possible route to smaller primordial stars and survivors.
- Schaerer (2002) — On the properties of massive Population III stars and metal-free stellar populationsStellar models for temperatures, lifetimes, and ionizing radiation.
- Heger & Woosley (2002) — The Nucleosynthetic Signature of Population IIIClassic models of pair-instability explosions, collapse, and elemental yields.
- Woosley (2017) — Pulsational Pair-Instability SupernovaeRepeated mass ejection and the different outcomes of pair instability.
- Dopcke et al. (2011) — The effect of dust cooling on low-metallicity star-forming cloudsDust cooling, fragmentation, and the transition toward lower stellar masses.
- Inayoshi, Visbal & Haiman (2020) — The Assembly of the First Massive Black HolesStellar remnants and other proposed origins of early massive black holes.
- Karlsson, Bromm & Bland-Hawthorn (2013) — Pre-galactic metal enrichment: The chemical signatures of the first starsHow ancient stars can retain evidence of earlier stellar enrichment.
- Maiolino et al. (2026) — The search for Population III: Confirmation of a HeII emitter with no metal lines at z=10.6JWST observations of Hebe and the proposed Population III interpretation.
- Übler et al. (2026) — GA-NIFS and JADES: Confirmation of pristine gas near GN-z11Hydrogen-line confirmation and limits on the chemical composition of the same region.
All articles in this chapter
- Gravitational Clumping and Density Fluctuations
- Population III Stars: The Universe’s First Generation — you are here
- Early Mini-Halos and Protogalaxies
- Supermassive Black Hole Seeds
- Primordial Supernovae: Element Synthesis
- Feedback Effects: Radiation and Winds
- Merging and Hierarchical Growth
- Galaxy Clusters and the Cosmic Web
- Active Galactic Nuclei in the Young Universe
- Observing the First Billion Years