JWST has brought us new insights into Cosmic Dawn with tentative detection of the unique signatures of metal-free Population III (Pop III) stars, such as strong HeII emission, extremely blue UV spectrum, and enhanced nitrogen abundance. Self-consistent theoretical predictions of the formation rates, sites, and masses of Pop III stars are crucial for interpreting the observations, but are challenging due to complex physical processes operating over the large range of length scales involved. One solution is to combine analytical models for the small-scale star formation process with cosmological simulations that capture the large-scale physics, such as structure formation, radiation backgrounds, and baryon-dark matter streaming motion that regulate the conditions of Pop III star formation.
We build an analytical model to predict the final masses of Pop III stars/clusters from the properties of star-forming clouds, based on the key results of small-scale star formation simulations and stellar evolution models. Our model for the first time considers the interplay between feedback and fragmentation and covers different modes of Pop III star formation, ranging from ordinary small (∼10−2000 M⊙) clusters in molecular-cooling clouds to massive (≳10^4 M⊙) clusters containing supermassive (∼10^4−3×10^5 M⊙) stars under violent collapse of atomic-cooling clouds.
As an example, the model is applied to the Pop III star-forming clouds in the progenitors of typical haloes hosting high-z luminous quasars, which shows that formation of Pop III massive clusters is common (∼20−70%) in such biased (∼4σ) regions, and the resulting heavy black hole seeds from supermassive stars can account for a significant fraction of observed luminous (≳10^46 erg s−1) quasars at z∼6.
For theoretical studies on Pop III remnants as seeds of high-z quasars in cosmic average conditions with cosmological simulations and semi-analytical models, see Jeon et al. (2023, 2024, 2025).
Population III (Pop III) stars are also expected to form in clusters according to simulations. The dynamical evolution of clusters determine the binary statistics, which is crucial for the feedback effect and observational signatures of Pop III stars.
In this work, we address this topic with N-body simulations. We design a physically-motivated model for the initial conditions of Pop III star clusters, based on small-scale hydrodynamic simulations and the scale-free nature of disk evolution during Pop III star formation. This novel model enables us to explore the dependence of binary statistics on initial condition parameters and make predictions for the signals of Pop III X-ray binaries (XRBs) and black hole binary (BHB) mergers.
We found that the binary properties are highly sensitive to the initial cluster size and distribution of binary separation, while the effect of initial mass function is relatively minor. Our simulations predict much (a factor of 10-10^4) lower efficiencies for the formation and accretion of Pop III XRBs than inferred/assumed in previous studies. We also estimate the efficiency of BBH mergers as a few per 10^4 to 10^5 Msun.
With these binary parameters, we also explore the Pop III origin of the BHB merger GW190521 recently reported by the LIGO collaboration, which involves BH masses in the mass gap of (pulsational) pair-instability supernovae (PPISNe) from standard stellar evolution models. Pop III stars are promising progenitors of the BHs found in GW190521, because Pop III stars, with small sizes and little mass loss, are likely to retain most of their hydrogen envelopes until the pre-supernova (SN) stage, avoid the PPISN regime and form BHs in the mass gap. We find that Pop III BBHs can naturally explain the observation, especially for the BBH evolution channel via dynamical hardening in nuclear star clusters. Our results are published in ApJ Letters.
Our Pop III scenario is further proved to be able to reproduce the observed merger rate density of GW190521-like events by more detailed modelling of the galactic dynamics and internal evolution of Pop III binary BHs, see the page Gravitational Waves & First Stars for details.