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Feedback-regulated star formation and escape of LyC photons from mini-haloes during reionisation
Astrophysics of Galaxies · Submitted 16 Aug 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Based on simple analytic calculations, we show that LyC photons from mini-haloes are, despite their high escape fractions, of minor importance for reionisation due to inefficient star formation.
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The abstract, sentence by sentence
Reionisation in the early Universe is likely driven by dwarf galaxies. Using cosmological radiation-hydrodynamic simulations, we study star formation and the escape of Lyman continuum (LyC) photons from mini-haloes with $M_{\rm halo} \le 10^8\,M_\odot$. Our simulations include a new thermo-turbulent star formation model, non-equilibrium chemistry, and relevant stellar feedback processes (photoionisation by young massive stars, radiation pressure, and mechanical supernova explosions). We find that feedback reduces star formation very efficiently in mini-haloes, resulting in the stellar mass consistent with the slope and normalisation reported in Kimm \& Cen and the empirical stellar mass-to-halo mass relation derived in the local Universe. Because star formation is stochastic and dominated by a few gas clumps, the escape fraction in mini-haloes is generally determined by radiation feedback (heating due to photo-ionisation), rather than supernova explosions. We also find that the photon number-weighted mean escape fraction in mini-haloes is higher ($\sim20$-$40\%$) than that in atomic-cooling haloes, although the instantaneous fraction in individual haloes varies significantly. The escape fraction from Pop III stars is found to be significant ($\ge10\%$) only when the mass is greater than $\sim$100\,\msun. Based on simple analytic calculations, we show that LyC photons from mini-haloes are, despite their high escape fractions, of minor importance for reionisation due to inefficient star formation. We confirm previous claims that stars in atomic-cooling haloes with masses $10^8\,M_\odot\le M_{\rm halo} \le 10^{11}\,M_\odot$ are likely to be the most important source of reionisation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Reionisation in the early Universe is likely driven by dwarf galaxies. | background 1.00 | 0.05 | 0.05 | hedged possibility 1.00 |
| s1 | Using cosmological radiation-hydrodynamic simulations, we study star formation and the escape of Lyman continuum (LyC) photons from mini-haloes with $M_{\rm halo} \le 10^8\,M_\odot$. | method 0.51 | 0.93 | 0.03 | asserted 0.85 |
| s2 | Our simulations include a new thermo-turbulent star formation model, non-equilibrium chemistry, and relevant stellar feedback processes (photoionisation by young massive stars, radiation pressure, and mechanical supernova explosions). | method 0.97 | 0.78 | 0.03 | asserted 0.99 |
| s3 | We find that feedback reduces star formation very efficiently in mini-haloes, resulting in the stellar mass consistent with the slope and normalisation reported in Kimm \& Cen and the empirical stellar mass-to-halo mass relation derived in the local Universe. | result 1.00 | 0.94 | 0.14 | asserted 0.99 |
| s4 | Because star formation is stochastic and dominated by a few gas clumps, the escape fraction in mini-haloes is generally determined by radiation feedback (heating due to photo-ionisation), rather than supernova explosions. | result 0.85 | 0.93 | 0.10 | asserted 0.99 |
| s5 | We also find that the photon number-weighted mean escape fraction in mini-haloes is higher ($\sim20$-$40\%$) than that in atomic-cooling haloes, although the instantaneous fraction in individual haloes varies significantly. | result 1.00 | 0.97 | 0.11 | asserted 1.00 |
| s6 | The escape fraction from Pop III stars is found to be significant ($\ge10\%$) only when the mass is greater than $\sim$100\,\msun. | result 1.00 | 0.95 | 0.06 | asserted 1.00 |
| s7 | Based on simple analytic calculations, we show that LyC photons from mini-haloes are, despite their high escape fractions, of minor importance for reionisation due to inefficient star formation. | result 0.58 | 0.92 | 0.54 | asserted 1.00 |
| s8 | We confirm previous claims that stars in atomic-cooling haloes with masses $10^8\,M_\odot\le M_{\rm halo} \le 10^{11}\,M_\odot$ are likely to be the most important source of reionisation. | result 0.75 | 0.50 | 0.31 | hedged possibility 0.87 |
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The paper
Original abstract
Reionisation in the early Universe is likely driven by dwarf galaxies. Using cosmological radiation-hydrodynamic simulations, we study star formation and the escape of Lyman continuum (LyC) photons from mini-haloes with $M_{\rm halo} \le 10^8\,M_\odot$. Our simulations include a new thermo-turbulent star formation model, non-equilibrium chemistry, and relevant stellar feedback processes (photoionisation by young massive stars, radiation pressure, and mechanical supernova explosions). We find that feedback reduces star formation very efficiently in mini-haloes, resulting in the stellar mass consistent with the slope and normalisation reported in Kimm \& Cen and the empirical stellar mass-to-halo mass relation derived in the local Universe. Because star formation is stochastic and dominated by a few gas clumps, the escape fraction in mini-haloes is generally determined by radiation feedback (heating due to photo-ionisation), rather than supernova explosions. We also find that the photon number-weighted mean escape fraction in mini-haloes is higher ($\sim20$-$40\%$) than that in atomic-cooling haloes, although the instantaneous fraction in individual haloes varies significantly. The escape fraction from Pop III stars is found to be significant ($\ge10\%$) only when the mass is greater than $\sim$100\,\msun. Based on simple analytic calculations, we show that LyC photons from mini-haloes are, despite their high escape fractions, of minor importance for reionisation due to inefficient star formation. We confirm previous claims that stars in atomic-cooling haloes with masses $10^8\,M_\odot\le M_{\rm halo} \le 10^{11}\,M_\odot$ are likely to be the most important source of reionisation.
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References
How later papers used it
135 later papers cite it
1 later paper by other authors is listed below: 1 used its method or tool. 6 more papers by the same authors are listed: 6 used its method or tool.
Uses its method or tool 7 of 56 papers with this label · 6 by the same authors
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Based its approach on one suggested by another work, introduced in ramses by this paper, and extended to account for magnetic fields in another work.
The Azahar Project: Non-Thermal Physics Drives Star Formation Burstiness and the Evolution of the UV Luminosity Density at Cosmic Dawn (2026) · 0.91 · paraphrased: the licence does not allow quoting
By the same authors
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We determine this following the magneto-thermo-turbulent (MTT) star formation model presented in [ref] and in [ref] for its MHD version.
The impact of cosmic rays on the interstellar medium and galactic outflows of Milky Way analogues (2023) (same authors) · The suite of simulations · 0.99
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Focused on the star formation implementation used by this paper and other works, among other feedback and turbulence approaches.
Cosmological simulations of the same spiral galaxy: the impact of baryonic physics (2020) (same authors) · 0.97 · paraphrased: the licence does not allow quoting
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The first is our fiducial prescription: a magneto-thermo-turbulent (MTT) star formation model, presented in [ref] , and [ref] in its MHD extension.
The Pandora project. I: the impact of radiation and cosmic rays on baryonic and dark matter properties of dwarf galaxies (2022) (same authors) · Star formation and stellar feedback · 0.98
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Used the subgrid model for star formation presented by this paper and another work, which is well adapted and tested in this regime.
Simulating the diversity of shapes of the Lyman-$\alpha$ line (2023) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Incorporated models for star formation from this paper along with stellar feedback from another work and a variable speed of light approximation from another work.
Two Modes of LyC Escape From Bursty Star Formation: Implications for [C II] Deficits and the Sources of Reionization (2022) (same authors) · 0.93 · paraphrased: the licence does not allow quoting
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Formed star particles according to a Schmidt law with the star formation efficiency per free-fall time determined by the local thermo-turbulent conditions of the ISM as given in this paper.
Predicting the Observability of Population III Stars with ELT-HARMONI via the Helium $1640{\rm\AA}$ emission line (2021) (same authors) · 0.82 · paraphrased: the licence does not allow quoting
How the literature uses it
11 arXiv papers cite this in 23 sentences
Papers citing it · 17 sentences without a confident label
Uses its method or tool 1 paper
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The model adopts a magneto-thermo-turbulent prescription for star formation [ref] , mechanical supernova (SN) feedback [ref] and astrophysically-seeded magnetic fields through magnetised SN feedback [ref] .
Deciphering Lyman-$\alpha$ Emission Deep into the Epoch of Reionisation · Introduction · 0.98
Uses its data or values 1 paper
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In particular, the stellar-to-halo mass ratio (determined by the parameters $f_*,0$, $α_*$, and $M_t$) is calibrated to the luminosity functions from the Hubble Space Telescope [ref] , the escape fraction ($f_esc,0$, $α_esc$) is inspired by radiative-hydrodynamical simulations [ref] , and the X-ray flux parameters ($f_X$, $E_min$) are obtained from Ref. [ref] .
Cosmological forecast of the 21-cm power spectrum using the halo model of reionization · MCMC results · 1.00
Compares with it 1 paper
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[ref] find that LMACHs begin to dominate minihalos at $z≈17$ (see their Fig. 15), whereas we find they are subdominant at all redshifts prior to overlap (Fig. 7).
Fully Coupled Simulation of Cosmic Reionization. III. Stochastic Early Reionization by the Smallest Galaxies · Comparable works · 0.90
What it cites · 16 sentences without a confident label
Uses data or values from 3 papers
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We then adopt the formation rate of Pop III from the large volume simulations of [ref] (the “Normal” run) by using the fit, $logṀ_popIII / (M_⊙ yr^-1 Mpc^-3)= -6.428 + 0.275 z - 0.011 z^2$.
Galaxy Properties and UV Escape Fractions During Epoch of Reionization: Results from the Renaissance Simulations · Importance of mini-haloes for reionisation · 0.99
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The latest results utilising the high frequency instrument to measure the low-multipole polarisation signal point to a possibility of an even lower value of $τ_e=0.055±0.009$ [ref] .
Planck intermediate results. XLVI. Reduction of large-scale systematic effects in HFI polarization maps and estimation of the reionization optical depth · Introduction · 0.91
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However, a more accurate modelling of dust emission in our Galaxy [ref] and the use of the low frequency instrument on the Planck satellite lead to a decrease in the optical depth to $τ_e=0.066±0.016$ [ref] .
Planck 2015 results. XIII. Cosmological parameters · Introduction · 0.88
Compares with 2 papers
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However, the escape fractions in atomic-cooling haloes appears to be less certain, and thus we compare three different models: i) an escape fraction that slowly decreases with the halo mass [ref] , ii) an escape fraction showing a more rapid decline [ref] , and iii) an escape fraction with a lower limit of 20 %.
Galaxy Properties and UV Escape Fractions During Epoch of Reionization: Results from the Renaissance Simulations · Importance of mini-haloes for reionisation · 0.81
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We also find that the evolution of $Q_HII$ lies between that of the `Late' and the `Very Late' reionisation model of [ref] at $z≥8$ [ref] , both of which are shown to be able to reproduce the rapid drop in the fraction of emitters at $z7$ [ref] .
Models of the Cosmological 21 cm Signal from the Epoch of Reionization Calibrated with Lyman-alpha and CMB Data · Importance of mini-haloes for reionisation · 0.98
Cites as background 2 papers
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Many studies agree that the primary source of reionisation is likely to be massive stars in dwarf galaxies [ref] ; however, the timescale over which reionisation occurred and the mass range of haloes which provided the majority of the ionising photons are issues that remain unresolved [ref] .
Radiation Backgrounds at Cosmic Dawn: X-Rays from Compact Binaries · Introduction · 0.84
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More details of the photo-chemistry will be presented in [ref] in terms of the prediction of molecular hydrogen in high-z galaxies.
Interpreting ALMA Observations of the ISM During the Epoch of Reionisation · Non-equilibrium photo-chemistry and radiative cooling · 0.80
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