Possible evidence for a pair-instability supernova nature of ultra-early JWST sources
Pith reviewed 2026-05-16 15:29 UTC · model grok-4.3
The pith
A variable ultra-high-redshift JWST source matches the light curve and spectrum of a pair-instability supernova from a 250-solar-mass metal-free star at redshift 15.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using state-of-the-art PISN light curves, spectral energy distributions, and synthetic spectra, a pair-instability supernova from a 250-260 solar-mass, metal-free star at z≃15 can plausibly reproduce the observed brightness, temporal evolution, photometry, and NIRSpec spectrum of the Capotauro source.
What carries the argument
PISN light curves, spectral energy distributions, and synthetic spectra computed for massive metal-free stars.
If this is right
- The source lies at z≈15 rather than the initially suggested z~30.
- Very massive Population III stars existed and exploded as pair-instability supernovae.
- Some ultra-high-redshift galaxy candidates may be contaminated by transient events.
- Variability monitoring and specific spectral tests can separate PISNe from galaxies or brown dwarfs.
Where Pith is reading between the lines
- Confirmation would constitute the first identified supernova from the first generation of stars.
- High-redshift surveys should routinely include multi-epoch observations to flag transients.
- Similar PISN events may appear in other JWST fields and could be used to map the early star-formation rate.
Load-bearing premise
The observed brightness changes over the 800-day baseline are produced by the supernova light-curve evolution rather than by other astrophysical processes, instrumental effects, or an unrelated object.
What would settle it
Continued monitoring showing brightness evolution that deviates from the predicted PISN decline or spectroscopy lacking the expected supernova features at the predicted epoch would rule out the interpretation.
Figures
read the original abstract
Recent JWST observations have revealed a population of unexpectedly bright sources at ultra-high redshift ($z > 15$), challenging current models of early galaxy formation. One extreme example is 'Capotauro', an F356W-dropout identified in the CEERS survey and initially interpreted as a luminous galaxy at $z\sim30$, but subsequently found to be variable over an $\sim 800$ day baseline. Motivated by this variability, we explore the alternative hypothesis that Capotauro is a pair-instability supernova (PISN) originating from a massive ($250-260\,M_\odot$), metal-free star. Using state-of-the-art PISN light curves, spectral energy distributions, and synthetic spectra, we show that a PISN at $z\simeq 15$ can plausibly reproduce the observed brightness, temporal evolution, photometry, and NIRSpec spectrum. We compare this scenario with alternative interpretations, including a local Y0 brown dwarf, and discuss observational tests to discriminate among them. If confirmed, this event would provide a rare window onto Population III stars, and highlights the importance of transient contamination in ultra-high redshift galaxy samples.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes that the variable JWST source 'Capotauro' (an F356W dropout initially interpreted as a z~30 galaxy) is instead a pair-instability supernova from a 250-260 M⊙ metal-free Population III progenitor at z≈15. Using published PISN light-curve libraries, SEDs, and synthetic spectra, the authors argue that this model can plausibly reproduce the observed brightness, ~800-day temporal evolution, multi-band photometry, and NIRSpec spectrum, while briefly comparing to a local Y0 brown-dwarf alternative and outlining future tests.
Significance. If the quantitative matches hold, the result would constitute the first plausible identification of a PISN at z>10, providing direct evidence for the endpoints of the most massive Population III stars and underscoring transient contamination in ultra-high-redshift galaxy samples. The adoption of state-of-the-art PISN model grids is a clear strength.
major comments (4)
- [Abstract and light-curve comparison] Abstract and light-curve comparison section: no χ², likelihood, or posterior values are reported for the match between the observed photometric points and the time-dilated PISN model; the statement that the models 'reproduce' the data therefore cannot be assessed for goodness-of-fit or uniqueness.
- [Variability analysis] Variability analysis: the central claim that the ~800-day baseline changes track the PISN light curve rests on only a few photometric epochs spanning ~47 rest-frame days; no quantitative test (e.g., likelihood ratio against microlensing, low-level AGN variability, or calibration drift) is presented to exclude these alternatives.
- [Redshift and spectrum] Redshift and spectrum section: the adopted z≈15 is photometric (F356W dropout) with no reported uncertainty or secondary solutions explored; the NIRSpec spectrum match is described only as 'plausible' without a quantitative spectral fit metric (reduced χ², line-strength residuals, etc.).
- [Alternative interpretations] Brown-dwarf comparison: the exclusion of a Y0 dwarf is qualitative; no posterior odds or Bayes factor relative to the PISN hypothesis is provided despite the claim that the PISN scenario is favored.
minor comments (1)
- [Figures] Figure captions should explicitly list the exact progenitor mass, metallicity, and explosion energy of the PISN model shown, together with the rest-frame time sampling of the data points.
Simulated Author's Rebuttal
We thank the referee for their constructive and detailed comments, which have prompted us to strengthen the quantitative aspects of the analysis. We address each major comment below and indicate the revisions made to the manuscript.
read point-by-point responses
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Referee: [Abstract and light-curve comparison] Abstract and light-curve comparison section: no χ², likelihood, or posterior values are reported for the match between the observed photometric points and the time-dilated PISN model; the statement that the models 'reproduce' the data therefore cannot be assessed for goodness-of-fit or uniqueness.
Authors: We agree that quantitative goodness-of-fit metrics are necessary to properly evaluate the model match. In the revised manuscript we now report χ² and reduced-χ² values for the comparison of the observed photometry to the time-dilated PISN light curve at z≈15, together with a brief assessment of alternative redshifts and progenitor masses that yield substantially worse fits. revision: yes
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Referee: [Variability analysis] Variability analysis: the central claim that the ~800-day baseline changes track the PISN light curve rests on only a few photometric epochs spanning ~47 rest-frame days; no quantitative test (e.g., likelihood ratio against microlensing, low-level AGN variability, or calibration drift) is presented to exclude these alternatives.
Authors: The referee correctly notes the limited number of epochs. We have expanded the variability section to explain, on the basis of amplitude, color evolution and rest-frame timescale, why microlensing and low-level AGN variability are less plausible. However, with only a handful of points a formal likelihood-ratio test against all alternatives cannot be performed; we therefore treat this as an acknowledged limitation and highlight the need for future monitoring. revision: partial
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Referee: [Redshift and spectrum] Redshift and spectrum section: the adopted z≈15 is photometric (F356W dropout) with no reported uncertainty or secondary solutions explored; the NIRSpec spectrum match is described only as 'plausible' without a quantitative spectral fit metric (reduced χ², line-strength residuals, etc.).
Authors: We have revised the redshift section to include the photometric-redshift probability distribution, its 1σ uncertainty, and a brief exploration of secondary lower-redshift solutions. For the NIRSpec spectrum we now provide a reduced-χ² value for the comparison with the synthetic PISN spectrum and tabulate residuals for the strongest spectral features. revision: yes
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Referee: [Alternative interpretations] Brown-dwarf comparison: the exclusion of a Y0 dwarf is qualitative; no posterior odds or Bayes factor relative to the PISN hypothesis is provided despite the claim that the PISN scenario is favored.
Authors: We accept that a quantitative comparison is required. The revised manuscript now includes an approximate Bayesian odds-ratio calculation that uses the available photometry and spectrum; under the stated assumptions the PISN hypothesis is favored over the Y0-dwarf hypothesis by a factor of ~10. The assumptions and limitations of this estimate are explicitly noted. revision: yes
Circularity Check
No significant circularity; derivation relies on external PISN models
full rationale
The paper's central claim compares observed photometry, variability, and spectrum of Capotauro to state-of-the-art PISN light curves, SEDs, and synthetic spectra drawn from externally published libraries for 250-260 M⊙ metal-free progenitors. No equation or step defines a parameter from the JWST data and then renames its output as a 'prediction.' The redshift is photometric, the match is described as 'plausible,' and alternatives (brown dwarf, microlensing) are discussed without reducing to self-referential fits. The derivation is therefore self-contained against independent external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (2)
- progenitor mass
- redshift
axioms (1)
- domain assumption State-of-the-art PISN light curves and synthetic spectra accurately describe metal-free stars in the 250-260 solar-mass range.
Forward citations
Cited by 5 Pith papers
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JWST difference imaging from COSMOS-Web and PRIMER has yielded 68 high-redshift supernovae including a core-collapse event at z>3 and a Type Ia at z>2, demonstrating the feasibility of wide-area time-domain searches i...
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NEFERTITI simulations show that the Milky Way's most metal-poor stars largely come from a handful of accreted massive dwarf galaxies, while reproducing the JWST Hebe galaxy at z~11 as a pure Population III system.
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The Pristine HeII Emitter near GN-z11: Constraining the Mass Distribution of the First Stars
High-redshift HeII emitter observations confirm a >50% PopIII stellar mass fraction and favor top-heavy IMFs for the first stars with total masses 2e4 to 6e5 solar masses.
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Metal Enrichment by the First Stars Exploding at the Lower Energy Limit of Pair-Instability Supernovae
Low-energy PISNe from 140 solar-mass Pop III stars produce second-generation stars at median [Fe/H] ~ -5.5 with odd-even patterns, but their absence from EMP observations disfavors PISNe as the main early enrichment channel.
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Two Exciting High-redshift Galaxy Candidates Turn Out to Be Two Exciting Ultra-cool Brown Dwarfs
Two high-redshift galaxy candidates are reidentified as ultra-cool Y-type brown dwarfs at ~500 pc based on NIRSpec spectra matching templates and detected proper motions of 49 and 24 mas/yr.
Reference graph
Works this paper leans on
-
[1]
Abel, T., Bryan, G. L., & Norman, M. L. 2000, ApJ, 540, 39, doi: 10.1086/309295 Arrabal Haro, P., Dickinson, M., Finkelstein, S. L., et al. 2023a, arXiv e-prints, arXiv:2303.15431, doi: 10.48550/arXiv.2303.15431 Are ultra-early galaxies PISNe instead?9 —. 2023b, ApJL, 951, L22, doi: 10.3847/2041-8213/acdd54
-
[2]
2025, arXiv e-prints, arXiv:2507.03124, doi: 10.48550/arXiv.2507.03124
Asada, Y., Willott, C., Muzzin, A., et al. 2025, arXiv e-prints, arXiv:2507.03124, doi: 10.48550/arXiv.2507.03124
-
[3]
Atek, H., Shuntov, M., Furtak, L. J., et al. 2022, Revealing Galaxy Candidates out toz∼16 with JWST Observations of the Lensing Cluster SMACS0723, arXiv, doi: 10.48550/ARXIV.2207.12338
-
[4]
Beiler, S. A., Cushing, M. C., Kirkpatrick, J. D., et al. 2023, ApJL, 951, L48, doi: 10.3847/2041-8213/ace32c
-
[5]
Beiler, S. A., Cushing, M. C., Kirkpatrick, J. D., et al. 2024, The Astrophysical Journal, 973, 107, doi: 10.3847/1538-4357/ad6301
-
[6]
2023, ApJ, 944, 113, doi: 10.3847/1538-4357/acb5ea
Biagetti, M., Franciolini, G., & Riotto, A. 2023, ApJ, 944, 113, doi: 10.3847/1538-4357/acb5ea
-
[7]
Blinnikov, S. I., Eastman, R., Bartunov, O. S., Popolitov, V. A., & Woosley, S. E. 1998, ApJ, 496, 454, doi: 10.1086/305375
-
[8]
Bromm, V., Ferrara, A., Coppi, P. S., & Larson, R. B. 2001, MNRAS, 328, 969, doi: 10.1046/j.1365-8711.2001.04915.x
-
[9]
Bunker, A. J., Saxena, A., Cameron, A. J., et al. 2023, arXiv e-prints, arXiv:2302.07256, doi: 10.48550/arXiv.2302.07256
-
[10]
2024, Nature, 633, 318, doi: 10.1038/s41586-024-07860-9
Carniani, S., Hainline, K., D’Eugenio, F., et al. 2024, Nature, 633, 318, doi: 10.1038/s41586-024-07860-9
-
[11]
Casey, C. M., Akins, H. B., Shuntov, M., et al. 2024, ApJ, 965, 98, doi: 10.3847/1538-4357/ad2075
-
[12]
2024, arXiv e-prints, arXiv:2403.10238, doi: 10.48550/arXiv.2403.10238
Castellano, M., Napolitano, L., Fontana, A., et al. 2024, arXiv e-prints, arXiv:2403.10238, doi: 10.48550/arXiv.2403.10238
-
[13]
2025, arXiv e-prints, arXiv:2504.05893, doi: 10.48550/arXiv.2504.05893
Castellano, M., Fontana, A., Merlin, E., et al. 2025, arXiv e-prints, arXiv:2504.05893, doi: 10.48550/arXiv.2504.05893
-
[14]
Whalen, D. J. 2014, ApJ, 792, 44, doi: 10.1088/0004-637X/792/1/44
-
[15]
2005, SSRv, 116, 625, doi: 10.1007/s11214-005-3592-0
Ciardi, B., & Ferrara, A. 2005, SSRv, 116, 625, doi: 10.1007/s11214-005-3592-0
-
[16]
R., Hutter, A., Dayal, P., et al.\ 2024, , 686, A138
Cueto, E. R., Hutter, A., Dayal, P., et al. 2024, A&A, 686, A138, doi: 10.1051/0004-6361/202349017
-
[17]
2023, Nature Astronomy, doi: 10.1038/s41550-023-01918-w
Curtis-Lake, E., Carniani, S., Cameron, A., et al. 2023, Nature Astronomy, doi: 10.1038/s41550-023-01918-w de Souza, R. S., Ishida, E. E. O., Johnson, J. L., Whalen, D. J., & Mesinger, A. 2013, MNRAS, 436, 1555, doi: 10.1093/mnras/stt1680
-
[18]
2025, ApJ, 990, 31, doi: 10.3847/1538-4357/ade78c
DeCoursey, C., Egami, E., Sun, F., et al. 2025, ApJ, 990, 31, doi: 10.3847/1538-4357/ade78c
-
[19]
2023, MNRAS, 523, 3201, doi: 10.1093/mnras/stad1557
Li, Z. 2023, MNRAS, 523, 3201, doi: 10.1093/mnras/stad1557 D’Eugenio, F., Cameron, A. J., Scholtz, J., et al. 2025, ApJS, 277, 4, doi: 10.3847/1538-4365/ada148
-
[20]
Donnan, C. T., McLeod, D. J., Dunlop, J. S., et al. 2023, MNRAS, 518, 6011, doi: 10.1093/mnras/stac3472
-
[21]
Donnan, C. T., McLure, R. J., Dunlop, J. S., et al. 2024, arXiv e-prints, arXiv:2403.03171, doi: 10.48550/arXiv.2403.03171
-
[22]
Donnan, C. T., Dickinson, M., Taylor, A. J., et al. 2025, ApJ, 993, 224, doi: 10.3847/1538-4357/ae0a1f
-
[23]
Eisenstein, D. J., Johnson, B. D., Robertson, B., et al. 2023, arXiv e-prints, arXiv:2310.12340, doi: 10.48550/arXiv.2310.12340
-
[24]
2024a, A&A, 684, A207, doi: 10.1051/0004-6361/202348321 —
Ferrara, A. 2024a, A&A, 684, A207, doi: 10.1051/0004-6361/202348321 —. 2024b, A&A, 689, A310, doi: 10.1051/0004-6361/202450944
-
[25]
2023, MNRAS, 522, 3986, doi: 10.1093/mnras/stad1095
Ferrara, A., Pallottini, A., & Dayal, P. 2023, MNRAS, 522, 3986, doi: 10.1093/mnras/stad1095
-
[26]
Finkelstein, S. L., Leung, G. C. K., Bagley, M. B., et al. 2023, arXiv e-prints, arXiv:2311.04279, doi: 10.48550/arXiv.2311.04279 —. 2024, ApJL, 969, L2, doi: 10.3847/2041-8213/ad4495
-
[27]
Finkelstein, S. L., Bagley, M. B., Arrabal Haro, P., et al. 2025, ApJL, 983, L4, doi: 10.3847/2041-8213/adbbd3
-
[28]
2023, ApJL, 943, L27, doi: 10.3847/2041-8213/acb5f2
Travascio, A. 2023, ApJL, 943, L27, doi: 10.3847/2041-8213/acb5f2
-
[29]
2023, arXiv e-prints, arXiv:2308.11609, doi: 10.48550/arXiv.2308.11609
Fujimoto, S., Wang, B., Weaver, J., et al. 2023, arXiv e-prints, arXiv:2308.11609, doi: 10.48550/arXiv.2308.11609
-
[30]
2024, MNRAS, 534, 151, doi: 10.1093/mnras/stae2048
Gabrielli, F., Lapi, A., Boco, L., et al. 2024, MNRAS, 534, 151, doi: 10.1093/mnras/stae2048
-
[31]
Gandolfi, G., Rodighiero, G., Bisigello, L., et al. 2025a, arXiv e-prints, arXiv:2502.02637, doi: 10.48550/arXiv.2502.02637
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2502.02637
-
[32]
Gandolfi, G., Rodighiero, G., Castellano, M., et al. 2025b, arXiv e-prints, arXiv:2509.01664, doi: 10.48550/arXiv.2509.01664 Haemmerl´ e, L., Mayer, L., Klessen, R. S., et al. 2020, SSRv, 216, 48, doi: 10.1007/s11214-020-00673-y
-
[33]
Harikane, Y., Inoue, A. K., Ellis, R. S., et al. 2025, ApJ, 980, 138, doi: 10.3847/1538-4357/ad9b2c
-
[34]
2018, MNRAS, 479, 2202, doi: 10.1093/mnras/sty1576
Hartwig, T., Bromm, V., & Loeb, A. 2018, MNRAS, 479, 2202, doi: 10.1093/mnras/sty1576
-
[35]
Heger, A., & Woosley, S. E. 2002, ApJ, 567, 532, doi: 10.1086/338487
-
[36]
Helton, J. M., Rieke, G. H., Alberts, S., et al. 2024, arXiv e-prints, arXiv:2405.18462, doi: 10.48550/arXiv.2405.18462 10Ferrara et al
-
[37]
Y.-Y., Abdurro’uf, Coe, D., et al
Hsiao, T. Y.-Y., Abdurro’uf, Coe, D., et al. 2023, arXiv e-prints, arXiv:2305.03042, doi: 10.48550/arXiv.2305.03042
-
[38]
Hummel, J. A., Pawlik, A. H., Milosavljevi´ c, M., & Bromm, V. 2012, ApJ, 755, 72, doi: 10.1088/0004-637X/755/1/72
-
[39]
Inayoshi, K., Harikane, Y., Inoue, A. K., Li, W., & Ho, L. C. 2022, ApJL, 938, L10, doi: 10.3847/2041-8213/ac9310
- [40]
-
[41]
Kasen, D., Woosley, S. E., & Heger, A. 2011, ApJ, 734, 102, doi: 10.1088/0004-637X/734/2/102
-
[42]
Kirkpatrick, J. D., Gelino, C. R., Faherty, J. K., et al. 2021, ApJS, 253, 7, doi: 10.3847/1538-4365/abd107
-
[43]
Klessen, R. S., & Glover, S. C. O. 2023, ARA&A, 61, 65, doi: 10.1146/annurev-astro-071221-053453
-
[44]
2025, ApJL, 983, L22, doi: 10.3847/2041-8213/adc458
Kokorev, V., Atek, H., Chisholm, J., et al. 2025, ApJL, 983, L22, doi: 10.3847/2041-8213/adc458
-
[45]
2014, A&A, 565, A70, doi: 10.1051/0004-6361/201423447
Kozyreva, A., Blinnikov, S., Langer, N., & Yoon, S.-C. 2014, A&A, 565, A70, doi: 10.1051/0004-6361/201423447
-
[46]
2022, MNRAS, 511, 2505, doi: 10.1093/mnras/stac176
Lazar, A., & Bromm, V. 2022, MNRAS, 511, 2505, doi: 10.1093/mnras/stac176
-
[47]
Li, Z., Dekel, A., Sarkar, K. C., et al. 2024, A&A, 690, A108, doi: 10.1051/0004-6361/202348727
-
[48]
Impact of primordial black holes on the formation of the first stars and galaxies
Liu, B., & Bromm, V. 2023, arXiv e-prints, arXiv:2312.04085, doi: 10.48550/arXiv.2312.04085
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2312.04085 2023
-
[49]
Mason, C. A., Trenti, M., & Treu, T. 2023, MNRAS, 521, 497, doi: 10.1093/mnras/stad035
-
[50]
2025a, A&A, 701, A186, doi: 10.1051/0004-6361/202554728
Matteri, A., Ferrara, A., & Pallottini, A. 2025a, A&A, 701, A186, doi: 10.1051/0004-6361/202554728
-
[51]
Can primordial black holes explain the overabundance of bright super-early galaxies?
Matteri, A., Pallottini, A., & Ferrara, A. 2025b, A&A, 697, A65, doi: 10.1051/0004-6361/202553701
-
[52]
McLeod, D. J., Donnan, C. T., McLure, R. J., et al. 2024, MNRAS, 527, 5004, doi: 10.1093/mnras/stad3471
-
[53]
Meiksin, A., & Whalen, D. J. 2013, MNRAS, 430, 2854, doi: 10.1093/mnras/stt089
-
[54]
Mirocha, J., & Furlanetto, S. R. 2023, MNRAS, 519, 843, doi: 10.1093/mnras/stac3578
-
[55]
Moriya, T. J., Wong, K. C., Koyama, Y., et al. 2019, PASJ, 71, 59, doi: 10.1093/pasj/psz035
-
[56]
J., Jiang, J.-a., Yasuda, N., et al
Moriya, T. J., Jiang, J.-a., Yasuda, N., et al. 2021, ApJ, 908, 249, doi: 10.3847/1538-4357/abcfc0
-
[57]
Naidu, R. P., Oesch, P. A., van Dokkum, P., et al. 2022, Two Remarkably Luminous Galaxy Candidates at z≈11−13 Revealed by JWST, arXiv, doi: 10.48550/ARXIV.2207.09434
-
[58]
Naidu, R. P., Oesch, P. A., Brammer, G., et al. 2025, arXiv e-prints, arXiv:2505.11263, doi: 10.48550/arXiv.2505.11263
-
[59]
2023, MNRAS, 521, 5699, doi: 10.1093/mnras/stad912
Pagnini, G., Salvadori, S., Rossi, M., et al. 2023, MNRAS, 521, 5699, doi: 10.1093/mnras/stad912
-
[60]
2023, A&A, 677, L4, doi: 10.1051/0004-6361/202347384
Pallottini, A., & Ferrara, A. 2023, A&A, 677, L4, doi: 10.1051/0004-6361/202347384
-
[61]
2014, MNRAS, 440, 2498, doi: 10.1093/mnras/stu451
Pallottini, A., Ferrara, A., Gallerani, S., Salvadori, S., & D’Odorico, V. 2014, MNRAS, 440, 2498, doi: 10.1093/mnras/stu451
-
[62]
Pan, T., Kasen, D., & Loeb, A. 2012, MNRAS, 422, 2701, doi: 10.1111/j.1365-2966.2012.20837.x
-
[63]
2023, MNRAS, 526, L63, doi: 10.1093/mnrasl/slad107 P´ erez-Gonz´ alez, P
Parashari, P., & Laha, R. 2023, MNRAS, 526, L63, doi: 10.1093/mnrasl/slad107 P´ erez-Gonz´ alez, P. G.,¨Ostlin, G., Costantin, L., et al. 2025, arXiv e-prints, arXiv:2503.15594, doi: 10.48550/arXiv.2503.15594 Planck Collaboration, Ade, P. A. R., Aghanim, N., et al. 2014, A&A, 571, A16, doi: 10.1051/0004-6361/201321591 Reg˝ os, E., Vink´ o, J., & Ziegler, ...
-
[64]
2024, ApJ, 976, 193, doi: 10.3847/1538-4357/ad85d3
Roberts-Borsani, G., Treu, T., Shapley, A., et al. 2024, ApJ, 976, 193, doi: 10.3847/1538-4357/ad85d3
-
[65]
Robertson, B., Johnson, B. D., Tacchella, S., et al. 2024, ApJ, 970, 31, doi: 10.3847/1538-4357/ad463d
-
[66]
Salvadori, S., & Ferrara, A. 2009, MNRAS, 395, L6, doi: 10.1111/j.1745-3933.2009.00627.x
-
[67]
2005, ApJ, 633, 1031, doi: 10.1086/444450
Ferrara, A. 2005, ApJ, 633, 1031, doi: 10.1086/444450
-
[68]
2025a, arXiv e-prints, arXiv:2510.01034, doi: 10.48550/arXiv.2510.01034
Scholtz, J., Carniani, S., Parlanti, E., et al. 2025, arXiv e-prints, arXiv:2510.01034, doi: 10.48550/arXiv.2510.01034
-
[69]
Shen, X., Vogelsberger, M., Boylan-Kolchin, M., Tacchella, S., & Naidu, R. P. 2024, MNRAS, 533, 3923, doi: 10.1093/mnras/stae1932
-
[70]
Smidt, J., Whalen, D. J., Chatzopoulos, E., et al. 2015, ApJ, 805, 44, doi: 10.1088/0004-637X/805/1/44
-
[71]
Somerville, R. S., Yung, L. Y. A., Lancaster, L., et al. 2025, MNRAS, 544, 3774, doi: 10.1093/mnras/staf1824
-
[72]
Tacchella, S., Eisenstein, D. J., Hainline, K., et al. 2023, ApJ, 952, 74, doi: 10.3847/1538-4357/acdbc6
-
[73]
Tegmark, M., Silk, J., Rees, M. J., et al. 1997, ApJ, 474, 1, doi: 10.1086/303434
-
[74]
2009, ApJ, 694, 879, doi: 10.1088/0004-637X/694/2/879
Trenti, M., & Stiavelli, M. 2009, ApJ, 694, 879, doi: 10.1088/0004-637X/694/2/879
-
[75]
Schneider, R. 2024, MNRAS, 527, 5102, doi: 10.1093/mnras/stad3513
-
[76]
Population III star-forming environments
Venditti, A., Graziani, L., Schneider, R., et al. 2023, MNRAS, 522, 3809, doi: 10.1093/mnras/stad1201 Are ultra-early galaxies PISNe instead?11
-
[77]
2023, The Astrophysical Journal Letters, 957, L34, doi: 10.3847/2041-8213/acfe07
Wang, B., Fujimoto, S., Labb´ e, I., et al. 2023, The Astrophysical Journal Letters, 957, L34, doi: 10.3847/2041-8213/acfe07
-
[78]
Whalen, D. J., Even, W., Frey, L. H., et al. 2013, ApJ, 777, 110, doi: 10.1088/0004-637X/777/2/110
-
[79]
Whitler, L., Stark, D. P., Topping, M. W., et al. 2025, ApJ, 992, 63, doi: 10.3847/1538-4357/adfddc
-
[80]
Wise, J. H., & Abel, T. 2005, ApJ, 629, 615, doi: 10.1086/430434
discussion (0)
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