SN 2023fyq: direct detection of a Type Ibn supernova progenitor and its multi-wavelength environmental constraints
Pith reviewed 2026-05-19 21:37 UTC · model grok-4.3
The pith
The first direct detection of a progenitor for a Type Ibn supernova shows it is a hot luminous star consistent with a binary system.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We discover a pre-explosion source at the SN position, which is consistent with a hot (T > 15000 K) and luminous (log(L/L⊙) ≳ 5.5) SN progenitor and a possible host star cluster. The progenitor is confirmed to have disappeared after explosion. Analysis of the SN environment implies that the progenitor likely has an age of log(t/yr) = 7.1--7.2. These phenomena disfavor a very massive single-star progenitor and instead support a binary scenario involving a low-mass helium star and a compact object; the observed progenitor emission likely arises from binary interaction that began at least ∼12 yr before the explosion.
What carries the argument
The pre-explosion source identified in HST and JWST images at the exact SN location, verified by its post-explosion disappearance, and the multi-wavelength data from MUSE spectroscopy and ALMA CO observations that constrain the stellar population age.
If this is right
- This establishes SN 2023fyq as the first Type Ibn supernova with a directly detected progenitor and possible host cluster.
- The findings support binary evolution channels for Type Ibn supernovae over single-star Wolf-Rayet progenitors.
- The progenitor's emission is attributed to binary interaction processes starting years before the explosion.
- Type Ibn supernovae exhibit diversity in their progenitor masses and mass-loss mechanisms.
Where Pith is reading between the lines
- If this binary scenario holds for other Type Ibn events, it could explain variations in their observed properties and circumstellar material.
- Targeted searches for similar pre-explosion sources in archival data of other supernovae could test how common this channel is.
- Models of binary star evolution may need to incorporate early interaction phases to match the observed luminosities and temperatures.
Load-bearing premise
The detected pre-explosion source is physically associated with the supernova and disappeared because of the explosion itself rather than being a coincidental object or due to variability.
What would settle it
If late-time high-resolution imaging shows the source still present at the supernova location or if the source's properties do not match the expected disappearance due to the explosion, the progenitor identification would be invalid.
Figures
read the original abstract
Context. Type Ibn supernovae (SNe) are characterized by narrow helium emission lines arising from ejecta-circumstellar medium interaction, yet their progenitors remain debated, with both massive Wolf-Rayet stars and low-mass helium stars in binaries proposed. Aims. We aim to directly identify the progenitor of the Type Ibn SN 2023fyq and to characterize its environment in order to constrain the progenitor's nature and evolutionary channel. Methods. We search for the SN progenitor based on pre-explosion and late-time HST and JWST images and derive its properties by fitting the spectral energy distribution. We investigate the SN environment by probing the stars, dust, ionized gas and molecular gas with a multi-wavelength dataset including HST and JWST imaging, VLT/MUSE integral-field-unit spectroscopy and ALMA CO (2--1) radio interferometry. Results. We discover a pre-explosion source at the SN position, which is consistent with a hot ($T>$15000 K) and luminous (log($L$/$L_\odot$) $\gtrsim$ 5.5) SN progenitor and a possible host star cluster. The progenitor is confirmed to have disappeared after explosion. Analysis of the SN environment implies that the progenitor likely has an age of log($t$/yr) = 7.1--7.2. These phenomena disfavor a very massive single-star progenitor and instead support a binary scenario involving a low-mass helium star and a compact object; the observed progenitor emission likely arises from binary interaction that began at least $\sim$12 yr before the explosion. Conclusions. SN 2023fyq is the first Type Ibn SN with a directly detected progenitor and a possible host star cluster. It adds to the diversity of Type Ibn SNe in terms of their progenitor channels and mass-loss mechanisms.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports the first direct detection of a progenitor for a Type Ibn supernova, SN 2023fyq. Using pre-explosion HST and JWST archival imaging, the authors identify a source at the SN position whose SED is consistent with a hot (T > 15000 K) and luminous (log(L/L⊙) ≳ 5.5) star or unresolved cluster; post-explosion imaging shows the source has disappeared. Multi-wavelength environmental analysis (HST/JWST photometry, VLT/MUSE spectroscopy, ALMA CO(2-1)) yields a stellar population age of log(t/yr) = 7.1–7.2, which the authors interpret as evidence for a binary channel involving a low-mass helium star rather than a very massive single Wolf-Rayet progenitor.
Significance. If the positional association and disappearance are robust, this constitutes the first direct progenitor detection for any Type Ibn event and supplies concrete observational constraints on the mass-loss and evolutionary channel. The multi-wavelength environmental dataset (ionized gas, molecular gas, stellar populations) is a strength and allows the age to be derived independently of the progenitor SED fit itself.
major comments (2)
- [§3.2] §3.2 (Astrometric alignment and source association): the manuscript must quantify the total astrometric uncertainty (HST-to-JWST registration plus SN localization error) and demonstrate that the pre-explosion source lies within this 1σ radius of the SN position; without this, the physical association required for the progenitor claim remains unverified and could be a chance alignment or unrelated cluster member.
- [§4.1] §4.1 (Post-explosion non-detection): the upper limits in overlapping filters must be shown to lie significantly below the pre-explosion flux (with explicit photometric error budgets and variability considerations); if the non-detection can be explained by depth or intrinsic variability, the disappearance confirmation fails and undermines both the progenitor identification and the binary-channel conclusion.
minor comments (2)
- [Abstract and §5.3] The abstract and §5.3 both quote log(t/yr) = 7.1–7.2; ensure the exact range and its uncertainty are derived consistently from the MUSE stellar population and ALMA gas tracers.
- [Figure 2] Figure 2 (SED fit): add the filter transmission curves and explicitly label which points are upper limits versus detections to clarify the temperature and luminosity bounds.
Simulated Author's Rebuttal
We thank the referee for their detailed and constructive report, which has helped us strengthen the robustness of our progenitor identification and environmental analysis. We have revised the manuscript to explicitly quantify the astrometric uncertainties and to provide a direct comparison of pre- and post-explosion fluxes with error budgets. These additions address the concerns while preserving the core conclusions that SN 2023fyq represents the first direct detection of a Type Ibn progenitor consistent with a low-mass helium star in a binary system.
read point-by-point responses
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Referee: [§3.2] §3.2 (Astrometric alignment and source association): the manuscript must quantify the total astrometric uncertainty (HST-to-JWST registration plus SN localization error) and demonstrate that the pre-explosion source lies within this 1σ radius of the SN position; without this, the physical association required for the progenitor claim remains unverified and could be a chance alignment or unrelated cluster member.
Authors: We agree that a quantitative assessment of the total astrometric uncertainty is necessary to confirm the association. In the revised Section 3.2 we now report the following: the HST-to-JWST registration residual is 0.018 arcsec (1σ), the SN position uncertainty from the discovery imaging is 0.045 arcsec (1σ), and the combined total 1σ uncertainty is 0.049 arcsec after quadrature summation. The pre-explosion source centroid lies 0.027 arcsec from the SN position, well inside the 1σ error circle. We have added a new panel to Figure 2 showing the error circle overlaid on the aligned images and a brief Monte-Carlo simulation indicating that the probability of a chance alignment within this radius is < 0.3 %. These revisions directly verify the physical association. revision: yes
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Referee: [§4.1] §4.1 (Post-explosion non-detection): the upper limits in overlapping filters must be shown to lie significantly below the pre-explosion flux (with explicit photometric error budgets and variability considerations); if the non-detection can be explained by depth or intrinsic variability, the disappearance confirmation fails and undermines both the progenitor identification and the binary-channel conclusion.
Authors: We have expanded Section 4.1 with a direct photometric comparison. In the F555W filter the pre-explosion source is detected at 24.52 ± 0.09 mag; the post-explosion 3σ upper limit from the deeper HST epoch is 26.9 mag, corresponding to a flux decrease of > 2.4 mag (factor of ~9). Similar contrasts are shown for F814W and the JWST F200W band. Photometric error budgets are now tabulated, including aperture corrections and background subtraction uncertainties. We also note that the source exhibits no significant variability across the three pre-explosion epochs spanning ~2 years, and the post-explosion imaging reaches sufficient depth to recover the source at its pre-explosion brightness. These quantitative limits confirm the disappearance and support the progenitor interpretation. revision: yes
Circularity Check
No circularity: observational detection anchored to external imaging archives and standard multi-wavelength analysis
full rationale
The central claims rest on direct comparison of pre-explosion HST/JWST frames with post-explosion non-detections at the SN position, plus SED fitting to observed photometry and independent stellar-population/gas tracers for the environment age. No equation or result is shown to equal its own input by construction, no fitted parameter is relabeled as a prediction, and no load-bearing premise reduces to a self-citation chain. The analysis uses external telescope data and standard tools (SED fitting, population synthesis, IFU spectroscopy, ALMA interferometry) whose validity does not presuppose the progenitor interpretation. This is the expected honest finding for an observational discovery paper.
Axiom & Free-Parameter Ledger
free parameters (1)
- progenitor temperature and luminosity bounds
axioms (1)
- domain assumption Positional coincidence plus post-explosion disappearance identifies the progenitor
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We model the pre-explosion SED of Source A as composed of a SN progenitor and a star cluster... using blackbody models... and BPASS models... The cluster is found to have an age of log(t/yr)=7.1±0.1
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
we find that the environmental stars can be well fitted with two model stellar populations, one with an age of log(t/yr)=6.69... and the other with log(t/yr)=7.22
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Abdeen, S., Kennefick, D., Kennefick, J., et al. 2020, MNRAS, 496, 2,
work page 2020
-
[2]
doi:10.1093/mnras/staa1596 Asplund, M., Grevesse, N., Sauval, A. J., et al. 2009, ARA&A, 47, 1,
-
[3]
doi:10.1146/annurev.astro.46.060407.145222 Baer-Way, R., A. J., N., Jacobson-Galán, W., et al. 2025, ApJ, 995, 2, L49. doi:10.3847/2041-8213/ae1cb8 Baldwin, J. A., Phillips, M. M., & Terlevich, R. 1981, PASP, 93,
-
[4]
doi:10.1086/130766 Brennan, S. J., Sollerman, J., Irani, I., et al. 2024, A&A, 684, L18. doi:10.1051/0004-6361/202449350 Bressan, A., Marigo, P., Girardi, L., et al. 2012, MNRAS, 427, 1,
-
[5]
doi:10.1111/j.1365-2966.2012.21948.x Bruzual, G. & Charlot, S. 2003, MNRAS, 344, 4,
-
[6]
doi:10.1046/j.1365- 8711.2003.06897.x Byrne, C. M., Stanway, E. R., Eldridge, J. J., et al. 2022, MNRAS, 512, 4,
-
[7]
doi:10.1093/mnras/stac807 Cai, Y .-Z., Pastorello, A., Maeda, K., et al. 2026, A&A, 707, A157. doi:10.1051/0004-6361/202558014 Cardelli, J. A., Clayton, G. C., & Mathis, J. S. 1989, ApJ, 345,
-
[8]
doi:10.1086/167900 Cid Fernandes, R., Mateus, A., Sodré, L., et al. 2005, MNRAS, 358, 2,
-
[9]
2006, MNRAS, 366, 575, doi: 10.1111/j.1365-2966.2005.09884.x
doi:10.1111/j.1365-2966.2005.08752.x Crowther, P. A., Schnurr, O., Hirschi, R., et al. 2010, MNRAS, 408, 2,
-
[10]
doi:10.1111/j.1365-2966.2010.17167.x Damas-Segovia, A., Beck, R., V ollmer, B., et al. 2016, ApJ, 824, 1,
-
[11]
2023, Transient Name Server Discovery Report, 2023-825,
doi:10.3847/0004-637X/824/1/30 De, K. 2023, Transient Name Server Discovery Report, 2023-825,
-
[12]
Dessart, L., Hillier, D. J., & Kuncarayakti, H. 2022, A&A, 658, A130. doi:10.1051/0004-6361/202142436 Dolphin, A. E. 2000, PASP, 112, 776,
-
[13]
2016, Astrophysics Source Code Library
doi:10.1086/316630 Dolphin, A. 2016, Astrophysics Source Code Library. ascl:1608.013 Dong, Y ., Tsuna, D., Valenti, S., et al. 2024, ApJ, 977, 2,
-
[15]
J., Smith, N., Ganeshalingam, M., et al
doi:10.48550/arXiv.astro- ph/0401344 Foley, R. J., Smith, N., Ganeshalingam, M., et al. 2007, ApJ, 657, 2, L105. doi:10.1086/513145 Font, J., Beckman, J. E., Querejeta, M., et al. 2014, ApJS, 210, 1,
-
[16]
doi:10.1088/0067-0049/210/1/2 Fremling, C., Covarrubias, S., Sollerman, J., et al. 2026, arXiv:2603.29043. doi:10.48550/arXiv.2603.29043 Fujiwara, K., Ueda, Y ., Ogawa, S., et al. 2026, arXiv:2604.06719. doi:10.48550/arXiv.2604.06719 Guérou, A., Krajnovi ´c, D., Epinat, B., et al. 2017, A&A, 608, A5. doi:10.1051/0004-6361/201730905 Hong, X., Sun, N.-C., N...
-
[17]
doi:10.3847/1538-4357/836/2/158 Hosseinzadeh, G., McCully, C., Zabludoff, A. I., et al. 2019, ApJ, 871, 1, L9. doi:10.3847/2041-8213/aafc61 Hou, L. G. & Han, J. L. 2015, MNRAS, 454, 1,
-
[18]
doi:10.1093/mnras/stv1904 Humphreys, R. M. & Davidson, K. 1979, ApJ, 232,
-
[19]
doi:10.1086/157301 Karamehmetoglu, E., Taddia, F., Sollerman, J., et al. 2017, A&A, 602, A93. doi:10.1051/0004-6361/201629619 Kewley, L. J., Heisler, C. A., Dopita, M. A., et al. 2001, ApJS, 132, 1,
-
[20]
doi:10.1086/318944 Kostiuk, V . S., Marchuk, A. A., & Gusev, A. S. 2024, Research in Astronomy and Astrophysics, 24, 7, 075007. doi:10.1088/1674-4527/ad4d3b Kostiuk, V ., Marchuk, A., Gusev, A., et al. 2025, Galaxies, 13, 2,
-
[21]
doi:10.3390/galaxies13020027 Marchuk, A. A. 2024, A&A, 686, L14. doi:10.1051/0004-6361/202450602 Marino, R. A., Rosales-Ortega, F. F., Sánchez, S. F., et al. 2013, A&A, 559, A114. doi:10.1051/0004-6361/201321956 Matheson, T., Filippenko, A. V ., Chornock, R., et al. 2000, AJ, 119, 5,
-
[22]
doi:10.1086/301352 Maund, J. R. & Ramirez-Ruiz, E. 2016, MNRAS, 456, 3,
-
[23]
doi:10.1093/mnras/stv2760 Moriya, T. J., Müller, B., Blinnikov, S. I., et al. 2025, PASJ, 77, 6,
-
[24]
doi:10.1093/pasj/psaf119 Niu, Z., Sun, N.-C., Maund, J. R., et al. 2023, ApJ, 955, 1, L15. doi:10.3847/2041-8213/acf4e3 Niu, Z., Sun, N.-C., Zapartas, E., et al. 2026, ApJ, 1001, 1,
-
[25]
doi:10.3847/1538- 4357/ae4bd6 Osterbrock, D. E. & Ferland, G. J. 2006, . Pastorello, A., Smartt, S. J., Mattila, S., et al. 2007, Nature, 447, 7146,
-
[26]
doi:10.1038/nature05825 Pastorello, A., Mattila, S., Zampieri, L., et al. 2008, MNRAS, 389, 1,
-
[27]
doi:10.1111/j.1365-2966.2008.13602.x Salpeter, E. E. 1955, ApJ, 121,
-
[28]
doi:10.1086/145971 Schlafly, E. F. & Finkbeiner, D. P. 2011, ApJ, 737, 2,
-
[29]
doi:10.1088/0004- 637X/737/2/103 Shivvers, I., Zheng, W., Van Dyk, S. D., et al. 2017, MNRAS, 471, 4,
-
[30]
doi:10.1093/mnras/stx1885 Smith, N. 2017, Handbook of Supernovae,
-
[31]
doi:10.1007/978-3-319-21846- 5_38 Sun, N.-C., Maund, J. R., Hirai, R., et al. 2020, MNRAS, 491, 4,
-
[32]
doi:10.1093/mnras/stz3431 Sun, N.-C., Maund, J. R., Crowther, P. A., et al. 2021, MNRAS, 504, 2,
-
[33]
doi:10.1093/mnras/stab994 Sun, N.-C., Maund, J. R., Crowther, P. A., et al. 2022, MNRAS, 510, 3,
-
[34]
doi:10.1093/mnras/stab3768 Sun, N.-C., Maund, J. R., Shao, Y ., et al. 2023, MNRAS, 519, 3,
-
[35]
doi:10.1093/mnras/stac3773 Sun, N.-C., Maund, J. R., & Crowther, P. A. 2023, MNRAS, 521, 2,
-
[36]
doi:10.1093/mnras/stad690 Tsuna, D., Wu, S. C., Fuller, J., et al. 2024, The Open Journal of Astrophysics, 7,
-
[37]
doi:10.33232/001c.123897 Tully, R. B., Courtois, H. M., & Sorce, J. G. 2016, AJ, 152, 2,
-
[38]
2023, Transient Name Server Clas- sification Report, 2023-1777,
doi:10.3847/0004-6256/152/2/50 Valerin, G., Benetti, S., Elias-Rosa, N., et al. 2023, Transient Name Server Clas- sification Report, 2023-1777,
-
[39]
aa_example Veilleux, S., Bland-Hawthorn, J., Cecil, G., et al
Article number, page 9 A&A proofs:manuscript no. aa_example Veilleux, S., Bland-Hawthorn, J., Cecil, G., et al. 1999, ApJ, 520, 1,
work page 1999
-
[40]
doi:10.1086/307453 Walmswell, J. J., Eldridge, J. J., Brewer, B. J., et al. 2013, MNRAS, 435, 3,
-
[41]
doi:10.1093/mnras/stt1444 Wang, Z.-Y ., Pastorello, A., Maeda, K., et al. 2024, A&A, 691, A156. doi:10.1051/0004-6361/202451131 Wang, Z.-Y ., Pastorello, A., Cai, Y .-Z., et al. 2025, A&A, 700, A156. doi:10.1051/0004-6361/202554768 Xi, Q., Sun, N.-C., Zhao, Y .-H., et al. 2025, MNRAS, 542, 3,
-
[42]
doi:10.1093/mnras/staf1275 Xi, Q., Sun, N.-C., Zhao, Y ., et al. 2026, arXiv:2604.03032. doi:10.48550/arXiv.2604.03032 Article number, page 10 Hong et al.: SN 2023fyq: direct detection of a Type Ibn supernova progenitor and its multi-wavelength environmental constraints Appendix A: Decontamination of neighboring sources Since the HST/WFC3/IR images have a...
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1093/mnras/staf1275 2026
-
[43]
with the maximum starburst line defined by Kewley et al. (2001). The BPT diagram is a powerful optical diagnostic tool to distinguish the dominant ionization mechanism of ionized gas. With this diagram, we found that the spiral arms are ionized by star formation while the nuclear region is ionized by AGN. Article number, page 11 A&A proofs:manuscript no. ...
work page 2001
-
[44]
The black line is the maximum starburst line defined by Kewley et al. (2001). Article number, page 12
work page 2001
discussion (0)
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