Recognition: 1 theorem link
Blackbody Quasar and Radio Source (BBQSORS): A Candidate of Transitional Little Red Dots with a Tsim10⁴\ K Blackbody Spectrum
Pith reviewed 2026-05-15 12:13 UTC · model grok-4.3
The pith
A radio-loud quasar at z=1.715 shows a UV continuum that fits a 10000 K blackbody, indicating a transitional state from a Little Red Dot.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The UV spectrum of this z=1.715 radio-loud quasar shows a Lambda-shaped continuum that is accurately reproduced by a blackbody with temperature T approximately 10000 K. This fit is preferred over dust-extincted standard quasar spectra and is consistent with the full UV-to-MIR spectral energy distribution decomposed into three blackbodies: an SMBH envelope at about 9700 K, a torus at about 1500 K, and host dust at about 80 K. A marginal GALEX detection suggests the V-shape occurs near 1400 angstroms, shifted blueward from Little Red Dots due to the temperature difference, implying the source is in a transitional state with a fragmenting LRD envelope.
What carries the argument
The blackbody spectrum at T approximately 10000 K fitted to the UV continuum, which physically represents the SMBH envelope and whose temperature contrast with the cooler approximately 5000 K photospheres of Little Red Dots accounts for the observed wavelength shift of the V-shaped spectral feature.
If this is right
- The source illustrates an evolutionary pathway from Little Red Dots to unobscured quasars through progressive fragmentation of the dense gas envelope.
- Similar transitional objects may be identifiable in radio-loud AGN samples by their Lambda-shaped UV continua and shifted V-shaped SEDs.
- The blackbody model implies that parts of the envelope are becoming optically thin, allowing direct view of the central engine.
- X-ray and radio detections could be signatures of accretion activity that emerges during envelope breakup.
Where Pith is reading between the lines
- If such transitional sources are common, the lifetime of the Little Red Dot phase could be estimated from their relative numbers in flux-limited surveys.
- Black hole growth models may need to include a brief hot blackbody phase before the quasar becomes fully visible.
- Higher-resolution imaging or time-domain monitoring could directly test whether the envelope shows signs of breakup or variability in the blackbody component.
Load-bearing premise
That the blackbody component corresponds to a physical dense gas envelope around the supermassive black hole whose fragmentation drives the transition to a visible quasar, rather than serving only as a convenient mathematical description of the observed continuum shape.
What would settle it
Deeper UV spectroscopy or photometry that shows the continuum deviating significantly from the 10000 K blackbody curve or fails to confirm the predicted V-shaped turnover near 1400 angstroms.
Figures
read the original abstract
We report Subaru/PFS spectroscopic follow-up of a radio-loud quasar at $z=1.715$ from the UNVEIL radio AGN catalog and with X-ray detections. The PFS spectrum displays a broad MgII emission line with an $\mathrm{FWHM}\gtrsim4000\ km/s$, accompanied by a narrow absorption feature. The spectrum reveals a characteristic $\Lambda$-shape over the rest-frame wavelength ranging $\sim1500-3500\ \r{A}$. This underlying UV continuum is too curved to be reproduced by simply applying dust extinction to the spectrum of typical unobscured quasars. Alternatively, it is well described by a blackbody spectrum with a temperature of $T\approx10000\ K$. This result is in good agreement with its UV to MIR photometry that can be well modeled by three blackbody components representing the SMBH envelope ($\mathit{T}\approx9700\ K$), dust torus ($T\approx1500\ K$), and host galaxy dust ($T\approx80\ K$). The source is marginally detected in the GALEX NUV, revealing a potential V-shaped spectral energy distribution around $1400\ \r{A}$, reminiscent of the spectral feature reported for recently discussed LRDs whose V-shapes occur around $3000-4000\ \r{A}$. This wavelength shift is broadly consistent with the temperature contrast between our blackbody component, with $T\sim10^4\ K$, and the lower effective temperature of $T\sim5000\ K$ expected for an optically thick photosphere surrounding the SMBH in LRDs. These properties suggest that this source might be caught in a transient evolutionary phase in which the dense gas envelope characteristic of LRD has begun to fragment, allowing us to witness the emergence of a quasar from an LRD-like state.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reports Subaru/PFS spectroscopy of a radio-loud quasar at z=1.715, showing a broad MgII line (FWHM ≳4000 km/s) and a Λ-shaped UV continuum (rest-frame 1500-3500 Å) that cannot be reproduced by dust extinction applied to typical unobscured quasar spectra but is instead well fit by a T≈10000 K blackbody. This is consistent with three-component blackbody modeling of the UV-to-MIR photometry (SMBH envelope T≈9700 K, torus T≈1500 K, host dust T≈80 K). The source shows a marginal GALEX NUV detection suggesting a V-shaped SED peaking near 1400 Å, interpreted as a transitional state from LRDs (whose V-shapes occur at 3000-4000 Å) due to fragmentation of a dense SMBH envelope, enabled by the higher temperature contrast with LRD photospheres (T∼5000 K).
Significance. If the blackbody preference and evolutionary interpretation hold, the result would identify a rare transitional AGN between LRDs and unobscured quasars, providing a concrete temperature-based mechanism for the observed shift in the V-shape wavelength and supporting envelope fragmentation as a key evolutionary step.
major comments (1)
- [Abstract and spectral analysis] Abstract and spectral analysis section: the central claim that the Λ-shaped continuum (1500-3500 Å) is too curved for dust extinction on typical quasars and is instead well described by a T≈10000 K blackbody is presented without any reported χ², BIC, likelihood-ratio, or other quantitative model-comparison statistics between the blackbody and dust-extincted quasar models on the same PFS spectrum. This comparison is load-bearing for the transitional interpretation, as the temperature contrast alone does not establish physical preference over a convenient parametrization.
minor comments (2)
- [Abstract] The abstract states the blackbody temperature as T≈10000 K while the photometry fit gives T≈9700 K; clarify whether these are independent or linked and report uncertainties on both.
- [Results] The narrow absorption feature on MgII is mentioned but not characterized (e.g., velocity, equivalent width); add a brief description or figure inset for completeness.
Simulated Author's Rebuttal
We thank the referee for their constructive feedback. We address the single major comment below.
read point-by-point responses
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Referee: [Abstract and spectral analysis] Abstract and spectral analysis section: the central claim that the Λ-shaped continuum (1500-3500 Å) is too curved for dust extinction on typical quasars and is instead well described by a T≈10000 K blackbody is presented without any reported χ², BIC, likelihood-ratio, or other quantitative model-comparison statistics between the blackbody and dust-extincted quasar models on the same PFS spectrum. This comparison is load-bearing for the transitional interpretation, as the temperature contrast alone does not establish physical preference over a convenient parametrization.
Authors: We agree that quantitative model-comparison statistics are needed to rigorously support the preference for the blackbody over a dust-extincted typical quasar spectrum. In the revised manuscript we will add χ², BIC, and likelihood-ratio test results for both models fitted directly to the PFS spectrum over 1500–3500 Å. This will provide a statistical basis for the claim and strengthen the transitional interpretation. revision: yes
Circularity Check
No significant circularity in the derivation chain
full rationale
The paper's central result follows from direct fitting of the observed PFS spectrum and multi-band photometry to a T≈10000 K blackbody component, presented as an alternative to dust-extincted quasar templates. This fit is not renamed as a prediction, nor does any equation reduce to a self-defined input. The transitional LRD interpretation rests on external comparison to literature LRD temperatures (~5000 K) and V-shape locations, without load-bearing self-citations or uniqueness theorems imported from the authors' prior work. No step exhibits self-definitional closure or fitted-input-as-prediction; the derivation remains self-contained against the reported data.
Axiom & Free-Parameter Ledger
free parameters (2)
- Blackbody temperature =
≈10000 K
- Three-component temperatures =
9700 K, 1500 K, 80 K
axioms (1)
- domain assumption The curved UV continuum is produced by thermal emission from an optically thick SMBH envelope rather than alternative continuum mechanisms
invented entities (1)
-
SMBH envelope
no independent evidence
Lean theorems connected to this paper
-
BlackBodyRadiationDeep.leanblackBodyRadiationDeepCert (wien_zero_cost, stefan_boltzmann_zero_cost, off_match_positive) echoes?
echoesECHOES: this paper passage has the same mathematical shape or conceptual pattern as the Recognition theorem, but is not a direct formal dependency.
the spectrum reveals a characteristic Λ-shape... well described by a blackbody spectrum with a temperature of T≈10000 K... three blackbody components representing the SMBH envelope (T≈9700 K)
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]
2020, ApJS, 249, 3, doi: 10.3847/1538-4365/ab929e
Ahumada, R., Allende Prieto, C., Almeida, A., et al. 2020, ApJS, 249, 3, doi: 10.3847/1538-4365/ab929e
-
[2]
2018, , 70, S4, 10.1093/pasj/psx066
Aihara, H., Arimoto, N., Armstrong, R., et al. 2018, PASJ, 70, S4, doi: 10.1093/pasj/psx066
-
[3]
Akins, H. B., Casey, C. M., Lambrides, E., et al. 2025, ApJ, 991, 37, doi: 10.3847/1538-4357/ade984
-
[4]
Ananna, T. T., Bogd´an, ´A., Kov´acs, O. E., Natarajan, P., & Hickox, R. C. 2024, ApJL, 969, L18, doi: 10.3847/2041-8213/ad5669
-
[5]
Begelman, M. C., & Dexter, J. 2026, ApJ, 996, 48, doi: 10.3847/1538-4357/ae274a
-
[6]
Bock, J. J., Aboobaker, A. M., Adamo, J., et al. 2026, ApJ, 999, 139, doi: 10.3847/1538-4357/ae2be2
-
[7]
Chen, K., Li, Z., Inayoshi, K., & Ho, L. C. 2025a, ApJL, 994, L42, doi: 10.3847/2041-8213/ae1955
-
[8]
Chen, X. 2025, S3Fit: Simultaneous Spectrum and photometric-SED Fitting code for galaxy observations, Astrophysics Source Code Library, record ascl:2503.024
work page 2025
-
[9]
2025b, arXiv e-prints, arXiv:2510.02801, doi: 10.48550/arXiv.2510.02801
Chen, X., Ichikawa, K., Akiyama, M., et al. 2025b, arXiv e-prints, arXiv:2510.02801, doi: 10.48550/arXiv.2510.02801
-
[10]
Cova, F., Gastaldello, F., Wik, D. R., et al. 2019, A&A, 628, A83, doi: 10.1051/0004-6361/201834644
-
[11]
2023, MNRAS, 518, 425 de Graaff, A., Brammer, G., Weibel, A., et al
Cutri, R. M., Wright, E. L., Conrow, T., et al. 2021, VizieR Online Data Catalog: AllWISE Data Release (Cutri+2013), VizieR On-line Data Catalog: II/328. Originally published in: IPAC/Caltech (2013) de Graaff, A., Hviding, R. E., Naidu, R. P., et al. 2025, arXiv e-prints, arXiv:2511.21820, doi: 10.48550/arXiv.2511.21820
-
[12]
Fawcett, V . A., Alexander, D. M., Rosario, D. J., et al. 2022, MNRAS, 513, 1254, doi: 10.1093/mnras/stac945
-
[13]
2025, arXiv e-prints, arXiv:2512.02096, doi: 10.48550/arXiv.2512.02096
Fu, S., Zhang, Z., Jiang, D., et al. 2025, arXiv e-prints, arXiv:2512.02096, doi: 10.48550/arXiv.2512.02096
-
[14]
Gabriel, C., Denby, M., Fyfe, D. J., et al. 2004, Astronomical Society of the Pacific Conference Series, V ol. 314, The XMM-Newton SAS - Distributed Development and Maintenance of a Large Science Analysis System: A Critical Analysis, ed. F. Ochsenbein, M. G. Allen, & D. Egret, 759
work page 2004
-
[15]
Gordon, K. D. 2024, Journal of Open Source Software, 9, 7023, doi: 10.21105/joss.07023
-
[16]
Gordon, K. D., Fitzpatrick, E. L., Massa, D., et al. 2024, ApJ, 970, 51, doi: 10.3847/1538-4357/ad4be1
-
[17]
Gwyn, S., McConnachie, A. W., Cuillandre, J.-C., et al. 2025, AJ, 170, 324, doi: 10.3847/1538-3881/ae03ab
-
[18]
N., Maiolino, R., Juodˇzbalis, I., et al
Hainline, K. N., Maiolino, R., Juodˇzbalis, I., et al. 2025, ApJ, 979, 138, doi: 10.3847/1538-4357/ad9920
-
[19]
Hopkins, P. F., Strauss, M. A., Hall, P. B., et al. 2004, AJ, 128, 1112, doi: 10.1086/423291
-
[20]
Hosokawa, T., Omukai, K., & Yorke, H. W. 2012, ApJ, 756, 93, doi: 10.1088/0004-637X/756/1/93
-
[21]
W., Inayoshi, K., Omukai, K., & Yoshida, N
Hosokawa, T., Yorke, H. W., Inayoshi, K., Omukai, K., & Yoshida, N. 2013, ApJ, 778, 178, doi: 10.1088/0004-637X/778/2/178
-
[22]
E., de Graaff, A., Liu, H., et al
Hviding, R. E., de Graaff, A., Liu, H., et al. 2026, arXiv e-prints, arXiv:2601.09778, doi: 10.48550/arXiv.2601.09778
-
[23]
2025, ApJL, 988, L22, doi: 10.3847/2041-8213/adea66
Inayoshi, K. 2025, ApJL, 988, L22, doi: 10.3847/2041-8213/adea66
-
[24]
2016, ApJ, 828, 110, doi: 10.3847/0004-637X/828/2/110
Inayoshi, K., & Haiman, Z. 2016, ApJ, 828, 110, doi: 10.3847/0004-637X/828/2/110
-
[25]
Inayoshi, K., & Ho, L. C. 2025, arXiv e-prints, arXiv:2512.03130, doi: 10.48550/arXiv.2512.03130
-
[26]
Inayoshi, K., Kimura, S. S., & Noda, H. 2025, PASJ, 77, 811, doi: 10.1093/pasj/psaf050
-
[27]
2025, ApJL, 980, L27, doi: 10.3847/2041-8213/adaebd
Inayoshi, K., & Maiolino, R. 2025, ApJL, 980, L27, doi: 10.3847/2041-8213/adaebd
-
[28]
2020, ARA&A, 58, 27, doi: 10.1146/annurev-astro-120419-014455
Inayoshi, K., Visbal, E., & Haiman, Z. 2020, ARA&A, 58, 27, doi: 10.1146/annurev-astro-120419-014455 IRSA, & SSC. 2020, Spitzer Enhanced Imaging Products, NASA IPAC DataSet, IRSA433, doi: 10.26131/IRSA433
-
[29]
2025, MNRAS, doi: 10.1093/mnras/staf1867 Juodˇ zbalis, I., Maiolino, R., Baker, W
Ji, X., Maiolino, R., ¨Ubler, H., et al. 2025, MNRAS, 544, 3900, doi: 10.1093/mnras/staf1867 Juodˇzbalis, I., Ji, X., Maiolino, R., et al. 2024, MNRAS, 535, 853, doi: 10.1093/mnras/stae2367
-
[30]
Kido, D., Ioka, K., Hotokezaka, K., Inayoshi, K., & Irwin, C. M. 2025, MNRAS, 544, 3407, doi: 10.1093/mnras/staf1898
-
[31]
2019, MNRAS, 488, 3109, doi: 10.1093/mnras/stz1771
Fotopoulou, S. 2019, MNRAS, 488, 3109, doi: 10.1093/mnras/stz1771
-
[32]
D., Onoue, M., Inayoshi, K., et al
Kocevski, D. D., Onoue, M., Inayoshi, K., et al. 2023, ApJL, 954, L4, doi: 10.3847/2041-8213/ace5a0
-
[33]
Kocevski, D. D., Finkelstein, S. L., Barro, G., et al. 2025, ApJ, 986, 126, doi: 10.3847/1538-4357/adbc7d
-
[34]
Kokorev, V ., Caputi, K. I., Greene, J. E., et al. 2024, ApJ, 968, 38, doi: 10.3847/1538-4357/ad4265
-
[35]
2025, ApJ, 995, 24, doi: 10.3847/1538-4357/ae119e
Kokubo, M., & Harikane, Y . 2025, ApJ, 995, 24, doi: 10.3847/1538-4357/ae119e
-
[36]
Lacy, M., Baum, S. A., Chandler, C. J., et al. 2020, PASP, 132, 035001, doi: 10.1088/1538-3873/ab63eb
-
[37]
2008, A&A, 486, 359, doi: 10.1051/0004-6361:200809538
Leccardi, A., & Molendi, S. 2008, A&A, 486, 359, doi: 10.1051/0004-6361:200809538
-
[38]
Li, Z., Inayoshi, K., Chen, K., Ichikawa, K., & Ho, L. C. 2025, ApJ, 980, 36, doi: 10.3847/1538-4357/ada5fb
-
[39]
2024, ApJ, 974, 147, doi: 10.3847/1538-4357/ad6565
Lin, X., Wang, F., Fan, X., et al. 2024, ApJ, 974, 147, doi: 10.3847/1538-4357/ad6565
-
[40]
Liu, H., Jiang, Y .-F., Quataert, E., Greene, J. E., & Ma, Y . 2025, ApJ, 994, 113, doi: 10.3847/1538-4357/ae0c19
-
[41]
Ma, Y ., Greene, J. E., Setton, D. J., et al. 2025a, arXiv e-prints, arXiv:2504.08032, doi: 10.48550/arXiv.2504.08032
-
[42]
Ma, Y ., Greene, J. E., V olonteri, M., et al. 2025b, arXiv e-prints, arXiv:2509.02662, doi: 10.48550/arXiv.2509.02662 BBQSORS 15
-
[43]
ApJS 251(1), 6 (2020) https://doi.org/10.3847/1538-4365/abb82a arXiv:1612.05242 [astro-ph.IM]
Magnier, E. A., Schlafly, E. F., Finkbeiner, D. P., et al. 2020, ApJS, 251, 6, doi: 10.3847/1538-4365/abb82a
-
[44]
Matthee, J., Naidu, R. P., Brammer, G., et al. 2024, ApJ, 963, 129, doi: 10.3847/1538-4357/ad2345
-
[45]
2026, ApJ, 998, 124, doi: 10.3847/1538-4357/ae32f3
Nandal, D., & Loeb, A. 2026, ApJ, 998, 124, doi: 10.3847/1538-4357/ae32f3
-
[46]
Obuchi, S., Ichikawa, K., Yamada, S., et al. 2026, ApJ, 997, 156, doi: 10.3847/1538-4357/ae1d6d Planck Collaboration, Aghanim, N., Akrami, Y ., et al. 2020, A&A, 641, A6, doi: 10.1051/0004-6361/201833910
-
[47]
Richards, G. T., Hall, P. B., Vanden Berk, D. E., et al. 2003, AJ, 126, 1131, doi: 10.1086/377014
-
[48]
T., Lacy, M., Storrie-Lombardi, L
Richards, G. T., Lacy, M., Storrie-Lombardi, L. J., et al. 2006, ApJS, 166, 470, doi: 10.1086/506525
-
[49]
Rosario, D. J., Alexander, D. M., Moldon, J., et al. 2021, MNRAS, 505, 5283, doi: 10.1093/mnras/stab1653
-
[50]
Santarelli, A. D., Farag, E., Bellinger, E. P., et al. 2026, ApJL, 998, L4, doi: 10.3847/2041-8213/ae3713
-
[51]
Schneider, A. C., Vrba, F. J., Bruursema, J., et al. 2025, AJ, 170, 86, doi: 10.3847/1538-3881/ade43c
-
[52]
Schneider, D. P., Richards, G. T., Hall, P. B., et al. 2010, AJ, 139, 2360, doi: 10.1088/0004-6256/139/6/2360
-
[53]
Setton, D. J., Greene, J. E., Spilker, J. S., et al. 2025, ApJL, 991, L10, doi: 10.3847/2041-8213/ade78b
-
[54]
Shen, Y ., Richards, G. T., Strauss, M. A., et al. 2011, ApJS, 194, 45, doi: 10.1088/0067-0049/194/2/45 SPHEREx Team. 2025, SPHEREx Quick Release Spectral Images - QR2, IPAC, doi: 10.26131/IRSA652
-
[55]
Sun, W. Q., Naidu, R. P., Matthee, J., et al. 2026, arXiv e-prints, arXiv:2601.20929, doi: 10.48550/arXiv.2601.20929
-
[56]
2024, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference
Tamura, N., Yabe, K., Koshida, S., et al. 2024, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference
work page 2024
-
[57]
13096, Ground-based and Airborne Instrumentation for Astronomy X, ed
Series, V ol. 13096, Ground-based and Airborne Instrumentation for Astronomy X, ed. J. J. Bryant, K. Motohara, & J. R. D. Vernet, 1309605, doi: 10.1117/12.3015967
-
[58]
Tanaka, T. S., Akins, H. B., Harikane, Y ., et al. 2025, ApJ, 995, 21, doi: 10.3847/1538-4357/ae145f
-
[59]
Thompson, T. A., Quataert, E., & Murray, N. 2005, ApJ, 630, 167, doi: 10.1086/431923
-
[60]
2006, ApJ, 650, 57, doi: 10.1086/506376 Vanden Berk, D
Tsuzuki, Y ., Kawara, K., Yoshii, Y ., et al. 2006, ApJ, 650, 57, doi: 10.1086/506376
-
[61]
Urrutia, T., Becker, R. H., White, R. L., et al. 2009, ApJ, 698, 1095, doi: 10.1088/0004-637X/698/2/1095 Vanden Berk, D. E., Wesolowski, S. C., Yeckley, M. J., et al. 2020, MNRAS, 493, 2745, doi: 10.1093/mnras/staa411 V´eron-Cetty, M.-P., Joly, M., & V´eron, P. 2004, A&A, 417, 515, doi: 10.1051/0004-6361:20035714
-
[62]
Vestergaard, M., & Osmer, P. S. 2009, ApJ, 699, 800, doi: 10.1088/0004-637X/699/1/800
-
[63]
Vestergaard, M., & Wilkes, B. J. 2001, ApJS, 134, 1, doi: 10.1086/320357
-
[64]
J., Yang, C., Wang, H., & Zhang, S
Wang, T., Ferland, G. J., Yang, C., Wang, H., & Zhang, S. 2016, ApJ, 824, 106, doi: 10.3847/0004-637X/824/2/106
-
[65]
A., Coriat, M., Traulsen, I., et al
Webb, N. A., Coriat, M., Traulsen, I., et al. 2020, A&A, 641, A136, doi: 10.1051/0004-6361/201937353
-
[66]
C., Alberts, S., Ji, Z., et al
Williams, C. C., Alberts, S., Ji, Z., et al. 2024, ApJ, 968, 34, doi: 10.3847/1538-4357/ad3f17
-
[67]
Willingale, R., Starling, R. L. C., Beardmore, A. P., Tanvir, N. R., & O’Brien, P. T. 2013, MNRAS, 431, 394, doi: 10.1093/mnras/stt175
-
[68]
2015, Nature, 518, 512, doi: 10.1038/nature14241
Wu, X.-B., Wang, F., Fan, X., et al. 2015, Nature, 518, 512, doi: 10.1038/nature14241
-
[69]
Yue, M., Eilers, A.-C., Ananna, T. T., et al. 2024, ApJL, 974, L26, doi: 10.3847/2041-8213/ad7eba
-
[70]
Zhang, Z., Jiang, L., Liu, W., & Ho, L. C. 2025a, ApJ, 985, 119, doi: 10.3847/1538-4357/adcb3e
-
[71]
2025c, arXiv e-prints, arXiv:2512.05180
Zhang, Z., Li, M., Oguri, M., et al. 2025b, arXiv e-prints, arXiv:2512.05180, doi: 10.48550/arXiv.2512.05180
-
[72]
Zhong, Y ., Inoue, A. K., Sugahara, Y ., et al. 2024, MNRAS, 529, 4531, doi: 10.1093/mnras/stae798
-
[73]
2025, ApJS, 281, 22, doi: 10.3847/1538-4365/ae03c3
Zhong, Y ., Ichikawa, K., Hildebrandt, H., et al. 2025, ApJS, 281, 22, doi: 10.3847/1538-4365/ae03c3
discussion (0)
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