REVIEW 2 major objections 8 minor 1 cited by
Testing for Intrinsic Type Ia Supernova Luminosity Evolution at z>2 with JWST
T0 review · 2 major / 8 minor · reviewed 2026-08-12 · deepseek-v4-flash
Pith's one-line read The paper reports that SN 2023aeax, a spectroscopically confirmed Type Ia supernova at $z=2.15$, has a BayeSN-standardized distance modulus of $\mu=46.10^{+0.17}_{-0.18}$ mag, matching the $\Lambda$CDM prediction of $46.12$ mag at the…
desk verdict A useful new z>2 SN Ia point, but the 0.1σ agreement with ΛCDM is softer than it looks once the BayeSN phase/color extrapolation is accounted for. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing machinery is the phase-extended BayeSN SED model, a Bayesian model trained on low-redshift Type Ia supernovae that jointly fits the light-curve shape parameter $\theta$, rest-frame host-galaxy dust extinction $A_V$, intrinsic scatter, and the distance modulus $\mu$ directly from multi-band photometry. The variant used here, trained on the sample of Ward et al. (2023), covers rest-frame phases to about 50 days after peak and extends beyond that by linear extrapolation in log-SED space, which is necessary because SN 2023aeax's observations sample late phases. Supporting machinery includes difference imaging with HOTPANTS, PSF-fitting photometry with space_phot, the NGSF spectral classification code, and the EAZY host SED fit. The NIRSpec spectrum establishes the classification and redshift ($z=2.15\pm0.01$), and the BayeSN fit then converts the photometry into the standardized distance that is compared with $\Lambda$CDM.
What would settle it
Fit SN 2023aeax's photometry with an independent standardization model such as SALT3-NIR, or simulate $z\simeq2.15$ Type Ia light curves from low-redshift BayeSN training SEDs with known distance moduli and run them through the same phase-extended pipeline; if the recovered distances are biased by more than the quoted $0.1\text{--}0.2$ mag uncertainty, or if the two models disagree by that amount, the reported $0.1\sigma$ agreement with $\Lambda$CDM would be an artifact of model extrapolation rather than evidence against luminosity evolution.
Extended reading notes
Core claim
On the paper's own terms, the central discovery is that SN 2023aeax is a normal Type Ia supernova at $z=2.15\pm0.01$ whose standardized luminosity distance agrees with $\Lambda$CDM: fitting the NIRCam photometry with the phase-extended BayeSN model yields $\mu=46.10^{+0.17}_{-0.18}$ mag against a predicted $46.12$ mag, a $0.1\sigma$ difference. The host-subtracted NIRSpec spectrum is best matched by normal low-redshift SN Ia templates, with Si II and Ca II features present and core-collapse templates strongly disfavored. The measured light-curve shape parameter corresponds to $\Delta m_{15}(B)\sim1.25$, within the normal population, while the peak rest-frame color $B-V\sim-0.3$ is bluer than almost all low-redshift cosmological SNe Ia. Re-fitting the other known $z>2$ SN Ia, SN 2023adsy, with the same BayeSN model gives $47.14^{+0.21}_{-0.24}$ mag, and combining both objects with the lower-redshift sample yields a $\sim1\sigma$ distance slope relative to $\Lambda$CDM, consistent with current cosmological constraints and not significant enough to claim luminosity evolution.
Load-bearing premise
The load-bearing premise is that the BayeSN SED model, trained on low-redshift Type Ia supernovae, can be extrapolated to $z=2.15$ and to phases beyond its 50-day training range without introducing a redshift-dependent bias in the inferred distance modulus.
Editorial extensions
If this is right
- The $0.1\sigma$ agreement between SN 2023aeax and $\Lambda$CDM means this object alone does not support intrinsic luminosity evolution at $z>2$.
- The two spectroscopically confirmed $z>2$ SNe Ia, with opposite extreme colors, produce a $\sim1\sigma$ distance slope relative to $\Lambda$CDM, so a larger sample is required to decide whether the slope is real.
- JWST is expected to add roughly ten more spectroscopically confirmed $z>2$ SNe Ia in the next two years, turning the current two-object sample into a population test.
- SN 2023aeax passes low-redshift cosmology cuts, so future surveys can include objects like it rather than treating high-redshift SNe Ia as pathological.
Reading between the lines
- The opposite extreme colors of the two known $z>2$ SNe Ia (blue for SN 2023aeax, red for SN 2023adsy) hint that the high-redshift population may have a broader intrinsic color distribution; if confirmed, current low-redshift color cuts could exclude a meaningful fraction of high-redshift SNe Ia and bias distance measurements.
- The paper's ad hoc treatment of the host-galaxy mass step -- applying half the measured low-redshift step as a systematic error -- may underestimate distance uncertainties if the mass step evolves with redshift; a dedicated high-redshift host-mass calibration would be a natural next step.
- The BayeSN phase extrapolation beyond 50 rest-frame days is not directly tested at $z\sim2$; a rest-frame UV-optical spectrum of a $z>2$ SN Ia at late phases, or a simulation campaign injecting low-redshift SEDs into high-redshift light curves, could confirm or refute the extrapolation's neutrality.
- If the $\sim1\sigma$ slope persists as JWST collects more objects, it will become a target for distinguishing mild luminosity evolution from new physics, but the current two-object slope cannot do that.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. SN 2023aeax is a JWST-discovered, spectroscopically confirmed Type Ia supernova at z=2.15, with NIRCam photometry in three epochs and a NIRSpec prism spectrum. The paper classifies it as a normal SN Ia, fits the light curve with the BayeSN SED model (using a phase-extended version with linear extrapolation beyond +50 rest-frame days), and obtains a distance modulus of 46.10+0.17-0.18 mag, which is in ~0.1 sigma agreement with the LambdaCDM prediction of 46.12 mag. The authors conclude there is no definitive evidence for SN Ia luminosity evolution with redshift, while noting that the two-object sample (including SN 2023adsy) shows a ~1 sigma slope relative to LambdaCDM. The paper also re-fits SN 2023adsy with the same methodology for a direct comparison.
Significance. The discovery is timely and important: it is only the second spectroscopically confirmed, non-lensed SN Ia at z>2, and the first that would pass traditional low-redshift cosmology cuts on light-curve properties (though it sits at the blue edge of the color distribution). The data are presented in sufficient detail (Table 1) with a public MAST archive link, and the spectral classification is supported by multiple template comparisons. The paper is appropriately cautious in its conclusions and includes a useful consistency check by re-fitting SN 2023adsy with the same BayeSN model. However, the central distance measurement rests on an extrapolation of a low-redshift-trained SED model into uncalibrated phase and wavelength territory, and the reported uncertainty does not include the systematic risk of that extrapolation.
major comments (2)
- [Section 4.1] The phase-extended BayeSN model is the load-bearing element of the distance measurement, yet it is applied at or beyond the edge of its training domain: the model is trained through +50 rest-frame days and extrapolated linearly in log-SED beyond that, and the final DDT epoch (MJD 60429) lands at roughly +50 rest-frame days after the fitted tpk (MJD 60270.34; Table 4). At z=2.15, F115W and F150W sample rest-frame wavelengths near 0.37 and 0.48 microns respectively, in the blue/UV region that is sparsely calibrated by the low-z training set. A prior application to a lensed SN at z=1.78 (Pierel et al. 2024b) is not a substitute for a validation tailored to this object's phase, wavelength, and color coverage, especially since the fitted B-V=-0.3 is at the blue edge of the low-z sample (Figure 7). I request a mock-recovery test: generate simulated z=2.15 SNe with known distance moduli from the BayeSN model (or from an independent SED model) at the same phases/wavelengths, add noise appropriate to Table 1, and re-fit with the same code and priors. The recovered bias and scatter should be quoted as a systematic uncertainty. Without this, the claimed 0.1 sigma agreement is not robust to an extrapolation bias of order 0.15 mag, which would erase the agreement.
- [Table 4 and Figure 6] The distance uncertainty (mu=46.10+0.14-0.12 before systematics) is derived from only three detections plus upper limits, with tpk, AV, theta, and mu fitted jointly. The posterior in Figure 6 shows AV pinned at the boundary (<0.04) and does not present covariances among the parameters. Because the object's color is at the extreme blue edge of the training distribution (B-V=-0.3), the intrinsic-scatter ('epsilon') model is unconstrained for this SN, and the posterior width may be driven by priors rather than by the data. I recommend reporting the full covariance matrix and performing a prior-sensitivity check (e.g., a wider theta prior, or a different AV prior that is not bounded so sharply at zero). The paper should also state how the upper limits are handled in the likelihood; this affects the reported uncertainty. As written, the statistical uncertainty likely understates the true uncertainty, making the 0.1 sigma agreement appear more significant than justified.
minor comments (8)
- [Abstract] The abstract contains an extra closing brace in "The James Webb Space Telescope}"; please correct.
- [Section 2.1] After the JHAT citation, the text has a stray "2)" that appears to be a footnote marker error.
- [Throughout] The name "SN2023aeax" and "SN 2023aeax" are used inconsistently; please standardize to the latter.
- [Section 4.2] The phrase "an additional0.055z mag" is missing a space; please write "an additional 0.055z mag" and clarify the lensing uncertainty formula.
- [Section 5] The sentence "a larger sample needed" should read "a larger sample is needed."
- [Table 4] The caption "The Bayesn light curve model parameters" has inconsistent capitalization; use "BayeSN" to match the rest of the text.
- [Section 3] The phrase "χ2 per degree of freedom (ν)" is redundant; use "reduced χ2" for clarity.
- [Section 4.2] The one-sentence dismissal of selection bias addresses detection brightness but not the search selection function; for the population-level interpretation, please expand this discussion even if only qualitatively.
Circularity Check
No circularity found: the claimed 0.1σ consistency with ΛCDM is an external benchmark comparison, not a value forced by the model or by prior author results.
full rationale
The paper's central result is a single-object distance measurement: BayeSN fits the SN 2023aeax light curve and returns μ = 46.10, which is then compared with the independently computed ΛCDM expectation μ = 46.12 at z = 2.15. No equation in the paper defines the fitted distance in terms of the ΛCDM value, and no fitted parameter is renamed as a prediction; the 0.1σ agreement is a comparison, not a construction. The BayeSN SED model is calibrated on low-redshift SNe and applied at z = 2.15 with stated linear extrapolation beyond +50 rest-frame days, which is a real extrapolation risk but an explicit modeling assumption rather than a logical circularity. The paper's citations to prior work by its own authors (e.g., Pierel et al. 2024b,d) are used as supporting evidence of model applicability and selection-bias arguments, but the central ΛCDM comparison does not reduce to those citations. The conclusion of no definitive evolution is a null result with acknowledged small-sample caveats, not an output enforced by the fitting procedure.
Assumptions & free parameters
free parameters (5)
- distance modulus mu =
46.10+0.17/-0.18 mag
- time of peak tpk =
60270.34+2.89/-2.23 MJD
- host extinction AV =
<0.04 mag
- light curve shape theta =
-0.52+0.33/-0.36
- host mass step systematic =
0.027 mag (half of 0.054 mag)
assumptions (4)
- domain assumption BayeSN model trained on low-redshift SNe Ia is valid at z=2.15, including linear extrapolation beyond 50 rest-frame days
- standard math Reference cosmology is flat LambdaCDM with H0=70 km/s/Mpc and Omega_m=0.315
- domain assumption NGSF template matching with a photometric redshift prior gives a correct redshift and SN Ia classification
- ad hoc to paper Selection effects can be ignored because the supernova is several magnitudes above the detection limit
Cite this review
Pith. "Pith review of Testing for Intrinsic Type Ia Supernova Luminosity Evolution at z>2 with JWST." pith.science (2026). https://pith.science/paper/SQG436RA
@misc{pith2026241111953,
author = {Pith},
title = {Pith review of: Testing for Intrinsic Type Ia Supernova Luminosity Evolution at z>2 with JWST},
year = {2026},
howpublished = {\url{https://pith.science/paper/SQG436RA}},
note = {Machine review of arXiv:2411.11953}
}
abstract
The James Webb Space Telescope} (JWST) is opening new frontiers of transient discovery and follow-up at high-redshift. Here we present the discovery of a spectroscopically confirmed Type Ia supernova (SN Ia; SN $2023$aeax) at $z=2.15$ with JWST, including a NIRCam multi-band light curve. SN $2023$aeax lands at the edge of traditional low-$z$ cosmology cuts because of its blue color (peak rest-frame $B-V\sim-0.3$) but with a normal decline rate ($\Delta m_{15}(B)\sim1.25$), and applying a fiducial standardization with the BayeSN model we find the SN $2023$aeax luminosity distance is in $\sim0.1\sigma$ agreement with $\Lambda$CDM. SN $2023$aeax is only the second spectroscopically confirmed SN Ia in the dark matter-dominated Universe at $z>2$ (the other is SN $2023$adsy), giving it rare leverage to constrain any potential evolution in SN Ia standardized luminosities. Similar to SN $2023$adsy ($B-V\sim0.8)$, SN $2023$aeax has a fairly extreme (but opposite) color, which may be due to the small sample size or a secondary factor, such as host galaxy properties. Nevertheless, the SN $2023$aeax spectrum is well-represented by normal low-$z$ SN Ia spectra and we find no definitive evolution in SN Ia standardization with redshift. Still, the first two spectroscopically confirmed $z>2$ SNe Ia have peculiar colors and combine for a $\sim1\sigma$ distance slope relative to $\Lambda$CDM, though in agreement with recent SN Ia cosmological measurements.
Figures
Figures from the paper (5 more)
Forward citations
Cited by 1 Pith paper
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Discovery of a likely Type II SN at $z$=3.6 with JWST
AT 2023adsv is a likely Type IIP supernova at z=3.613, the most distant photometrically classified SN IIP with a spectroscopic host redshift.
Reference graph
Works this paper leans on
-
[1]
2015, HOTPANTS: High Order Transform of PSF ANd Template Subtraction
Becker, A. 2015, HOTPANTS: High Order Transform of PSF ANd Template Subtraction
2015
-
[2]
2014, A&A, 568, A22, doi: 10.1051/0004-6361/201423413
Betoule, M., Kessler, R., Guy, J., et al. 2014, A&A, 568, A22, doi: 10.1051/0004-6361/201423413
-
[3]
Bildsten, L., Shen, K. J., Weinberg, N. N., & Nelemans, G. 2007, The Astrophysical Journal Letters, 662, L95, doi: 10.1086/519489
doi:10.1086/519489 2007
-
[4]
Brammer, G. B., van Dokkum, P. G., & Coppi, P. 2008, The Astrophysical Journal, 686, 1503, doi: 10.1086/591786
doi:10.1086/591786 2008
-
[5]
2021, ApJ, 909, 26, doi: 10.3847/1538-4357/abd69b
Brout, D., & Scolnic, D. 2021, ApJ, 909, 26, doi: 10.3847/1538-4357/abd69b
-
[6]
2022, The Astrophysical Journal, 938, 110, doi: 10.3847/1538-4357/ac8e04
Brout, D., Scolnic, D., Popovic, B., et al. 2022, The Astrophysical Journal, 938, 110, doi: 10.3847/1538-4357/ac8e04
-
[7]
2022, JWST Calibration Pipeline, Zenodo, doi: 10.5281/zenodo.7325378
Bushouse, H., Eisenhamer, J., Dencheva, N., et al. 2022, JWST Calibration Pipeline, Zenodo, doi: 10.5281/zenodo.7325378
-
[8]
Casey, C. M., Kartaltepe, J. S., Drakos, N. E., et al. 2023, The Astrophysical Journal, 954, 31, doi: 10.3847/1538-4357/acc2bc
Show all 70 references
-
[9]
L., Frye, B
Chen, W., Kelly, P. L., Frye, B. L., et al. 2024, ApJ, 970, 102, doi: 10.3847/1538-4357/ad50a5
2024 doi
-
[10]
J., Wolf, C., & Zahid, H
Childress, M. J., Wolf, C., & Zahid, H. J. 2014, Monthly Notices of the Royal Astronomical Society, 445, 1898, doi: 10.1093/mnras/stu1892
2014 doi
-
[11]
2024, The High-z Menagerie: A Rare Chance to Study the Early and Exotic Transient Universe
Coulter, D., Engesser, M., Pierel, J., et al. 2024, The High-z Menagerie: A Rare Chance to Study the Early and Exotic Transient Universe
2024
- [12]
-
[13]
M., Tzanidakis, A., et al
De, K., Kasliwal, M. M., Tzanidakis, A., et al. 2020, The Astrophysical Journal, 905, 58, doi: 10.3847/1538-4357/abb45c
2020 doi
-
[14]
DeCoursey, C., Egami, E., Pierel, J. D. R., et al. 2024, arXiv e-prints, arXiv:2406.05060 DES Collaboration, Abbott, T. M. C., Acevedo, M., et al. 2024, arXiv e-prints, arXiv:2401.02929, doi: 10.48550/arXiv.2401.02929
2024 arXiv
- [15]
-
[16]
S., Abraham, R
Dunlop, J. S., Abraham, R. G., Ashby, M. L. N., et al. 2021, PRIMER: Public Release IMaging for Extragalactic Research
2021
-
[17]
2022, åp, 661, A81, doi: 10.1051/0004-6361/202142673
Ferruit, P., Jakobsen, P., Giardino, G., et al. 2022, åp, 661, A81, doi: 10.1051/0004-6361/202142673
2022 doi
-
[18]
Filippenko, A. V . 1997, Annual Review of Astronomy and Astrophysics, 35, 309, doi: 10.1146/annurev.astro.35.1.309
1997 doi
-
[19]
1999, Monthly Notices of the Royal Astronomical Society, 304, 67, doi: 10.1046/j.1365-8711.1999.02299.x
Fisher, A., Branch, D., Hatano, K., & Baron, E. 1999, Monthly Notices of the Royal Astronomical Society, 304, 67, doi: 10.1046/j.1365-8711.1999.02299.x
1999
-
[20]
1999, Publications of the Astronomical Society of the Pacific, 111, 63, doi: 10.1086/316293
Fitzpatrick, E. 1999, Publications of the Astronomical Society of the Pacific, 111, 63, doi: 10.1086/316293
1999 doi
-
[21]
Foley, R. J. 2015, Monthly Notices of the Royal Astronomical Society, 452, 2463, doi: 10.1093/mnras/stv789
2015 doi
-
[22]
J., Hoffmann, S
Foley, R. J., Hoffmann, S. L., Macri, L. M., et al. 2020, Monthly Notices of the Royal Astronomical Society, 491, 5991, doi: 10.1093/mnras/stz3324
2020 doi
-
[23]
J., & Mandel, K
Foley, R. J., & Mandel, K. 2013, The Astrophysical Journal, 778, 167, doi: 10.1088/0004-637X/778/2/167
2013 doi
-
[24]
L., Pascale, M., Pierel, J., et al
Frye, B. L., Pascale, M., Pierel, J., et al. 2024, ApJ, 961, 171, doi: 10.3847/1538-4357/ad1034
2024 doi
-
[25]
2022, Transient Name Server AstroNote, 191, 1
Goldwasser, S., Yaron, O., Sass, A., et al. 2022, Transient Name Server AstroNote, 191, 1
2022
-
[26]
L., Foley, R
Graham, M. L., Foley, R. J., Zheng, W., et al. 2015, Monthly Notices of the Royal Astronomical Society, 446, 2073, doi: 10.1093/mnras/stu2221
2015 doi
- [27]
-
[28]
A., Kocevski, D
Grogin, N. A., Kocevski, D. D., Faber, S. M., et al. 2011, ApJS, 197, 35, doi: 10.1088/0067-0049/197/2/35
2011 doi
-
[29]
2007, Astronomy & Astrophysics, 466, 11, doi: 10.1051/0004-6361:20066930
Guy, J., Astier, P., Baumont, S., et al. 2007, Astronomy & Astrophysics, 466, 11, doi: 10.1051/0004-6361:20066930
2007 doi
-
[30]
1986, PASP, 98, 609, doi: 10.1086/131801
Horne, K. 1986, PASP, 98, 609, doi: 10.1086/131801
1986 doi
-
[31]
J., et al
Hounsell, R., Scolnic, D., Foley, R. J., et al. 2018, The Astrophysical Journal, 867, 23, doi: 10.3847/1538-4357/aac08b
2018 doi
-
[32]
M., Tyson, J
Ivezic, Z., Kahn, S. M., Tyson, J. A., et al. 2019, The Astrophysical Journal, 873, 111, doi: 10.3847/1538-4357/ab042c
2019 doi
-
[34]
M., Kulkarni, S
Kasliwal, M. M., Kulkarni, S. R., Gal-Yam, A., et al. 2012, The Astrophysical Journal, 755, 161, doi: 10.1088/0004-637X/755/2/161
2012 doi
-
[35]
L., Hicken, M., Burke, D
Kelly, P. L., Hicken, M., Burke, D. L., Mandel, K. S., & Kirshner, R. P. 2010, The Astrophysical Journal, 715, 743, doi: 10.1088/0004-637X/715/2/743
2010 doi
-
[36]
D., Jones, D
Kenworthy, W. D., Jones, D. O., Dai, M., et al. 2021, arXiv e-prints, arXiv:2104.07795
2021 arXiv
-
[37]
2017, The Astrophysical Journal, 836, 56, doi: 10.3847/1538-4357/836/1/56
Kessler, R., & Scolnic, D. 2017, The Astrophysical Journal, 836, 56, doi: 10.3847/1538-4357/836/1/56
2017 doi
-
[38]
M., Aussel, H., Calzetti, D., et al
Koekemoer, A. M., Aussel, H., Calzetti, D., et al. 2007, ApJS, 172, 196, doi: 10.1086/520086 13
2007 doi
-
[39]
M., Faber, S
Koekemoer, A. M., Faber, S. M., Ferguson, H. C., et al. 2011, ApJS, 197, 36, doi: 10.1088/0067-0049/197/2/36
2011 doi
-
[40]
C., et al
Lampeitl, H., Smith, M., Nichol, R. C., et al. 2010, The Astrophysical Journal, 722, 566, doi: 10.1088/0004-637X/722/1/566
2010 doi
-
[41]
2022, The Astrophysical Journal, 941, 71, doi: 10.3847/1538-4357/ac9f49
Lu, J., Wang, L., Chen, X., et al. 2022, The Astrophysical Journal, 941, 71, doi: 10.3847/1538-4357/ac9f49
2022 doi
-
[42]
S., Thorp, S., Narayan, G., Friedman, A
Mandel, K. S., Thorp, S., Narayan, G., Friedman, A. S., & Avelino, A. 2022, Monthly Notices of the Royal Astronomical Society, 510, 3939, doi: 10.1093/mnras/stab3496
2022 doi
-
[43]
2023, ApJ, 944, 212, doi: 10.3847/1538-4357/acb057
Mitra, A., Kessler, R., More, S., Hlozek, R., & LSST Dark Energy Science Collaboration. 2023, ApJ, 944, 212, doi: 10.3847/1538-4357/acb057
2023 doi
-
[44]
E., Mollá, M., López-Sánchez, Á
Moreno-Raya, M. E., Mollá, M., López-Sánchez, Á. R., et al. 2016, The Astrophysical Journal, 818, L19, doi: 10.3847/2041-8205/818/1/L19
2016 doi
-
[45]
L., Pierel, J
Pascale, M., Frye, B. L., Pierel, J. D. R., et al. 2025, ApJ, 979, 13, doi: 10.3847/1538-4357/ad9928
2025 doi
-
[46]
B., Gal-Yam, A., Mazzali, P
Perets, H. B., Gal-Yam, A., Mazzali, P. A., et al. 2010, Nature, 465, 322, doi: 10.1038/nature09056
2010 doi
-
[47]
1999, The Astrophysical Journal, 517, 565, doi: 10.1086/307221
Perlmutter, S., Aldering, G., Goldhaber, G., et al. 1999, The Astrophysical Journal, 517, 565, doi: 10.1086/307221
1999 doi
-
[48]
2024, Space-Phot: Simple Python-Based Photometry for Space Telescopes, Zenodo, doi: 10.5281/zenodo.12100100
Pierel, J. 2024, Space-Phot: Simple Python-Based Photometry for Space Telescopes, Zenodo, doi: 10.5281/zenodo.12100100
2024 doi
-
[49]
Pierel, J. D. R., Rodney, S., Vernardos, G., et al. 2021, The Astrophysical Journal, 908, 190, doi: 10.3847/1538-4357/abd8d3
2021 doi
-
[50]
Pierel, J. D. R., Jones, D. O., Kenworthy, W. D., et al. 2022, The Astrophysical Journal, 939, 11, doi: 10.3847/1538-4357/ac93f9
2022 doi
-
[51]
Pierel, J. D. R., Frye, B. L., Pascale, M., et al. 2024b, The Astrophysical Journal, 967, 50, doi: 10.3847/1538-4357/ad3c43
- [52]
-
[53]
Pierel, J. D. R., Engesser, M., Coulter, D. A., et al. 2024d, The Astrophysical Journal Letters, 971, L32, doi: 10.3847/2041-8213/ad6908
-
[54]
2023, arminrest/jhat: The JWST HST Alignment Tool (JHAT), Zenodo, doi: 10.5281/zenodo.7892935
Rest, A., Pierel, J., Correnti, M., et al. 2023, arminrest/jhat: The JWST HST Alignment Tool (JHAT), Zenodo, doi: 10.5281/zenodo.7892935
2023 doi
-
[55]
C., et al
Rest, A., Stubbs, C., Becker, A. C., et al. 2005, The Astrophysical Journal, 634, 1103, doi: 10.1086/497060
2005 doi
-
[56]
G., & Livio, M
Riess, A. G., & Livio, M. 2006, The Astrophysical Journal, 648, 884, doi: 10.1086/50479110.48550/arXiv.astro-ph/0601319
2006
-
[57]
G., Filippenko, A
Riess, A. G., Filippenko, A. V ., Challis, P., et al. 1998, The Astronomical Journal, 116, 1009, doi: 10.1086/300499
1998 doi
-
[58]
G., Yuan, W., Macri, L
Riess, A. G., Yuan, W., Macri, L. M., et al. 2022, The Astrophysical Journal Letters, 934, L7, doi: 10.3847/2041-8213/ac5c5b
2022 doi
-
[59]
A., Riess, A
Rodney, S. A., Riess, A. G., Strolger, L.-G., et al. 2014, The Astronomical Journal, 148, 13, doi: 10.1088/0004-6256/148/1/13
2014 doi
- [60]
-
[61]
F., & Finkbeiner, D
Schlafly, E. F., & Finkbeiner, D. P. 2011, The Astrophysical Journal, 737, 103, doi: 10.1088/0004-637X/737/2/103
2011 doi
-
[62]
M., Jones, D
Scolnic, D. M., Jones, D. O., Rest, A., et al. 2018, The Astrophysical Journal, 859, 101, doi: 10.3847/1538-4357/aab9bb
2018 doi
-
[63]
2010, The Astrophysical Journal, 715, 767, doi: 10.1088/0004-637X/715/2/767
Scannapieco, E. 2010, The Astrophysical Journal, 715, 767, doi: 10.1088/0004-637X/715/2/767
2010 doi
-
[64]
R., Decoursey, C., Coulter, D
Siebert, M. R., Decoursey, C., Coulter, D. A., et al. 2024, arXiv e-prints, arXiv:2406.05076
2024 arXiv
-
[65]
A., et al
Sullivan, M., Conley, A., Howell, D. A., et al. 2010, Monthly Notices of the Royal Astronomical Society, no, doi: 10.1111/j.1365-2966.2010.16731.x
2010
-
[66]
1998, Astronomy & Astrophysics, 331, 815
Tripp, R. 1998, Astronomy & Astrophysics, 331, 815
1998
-
[67]
2011, The Astrophysical Journal, 738, 21, doi: 10.1088/0004-637X/738/1/21
Waldman, R., Sauer, D., Livne, E., et al. 2011, The Astrophysical Journal, 738, 21, doi: 10.1088/0004-637X/738/1/21
2011 doi
-
[68]
M., Thorp, S., Mandel, K
Ward, S. M., Thorp, S., Mandel, K. S., et al. 2023, The Astrophysical Journal, 956, 111, doi: 10.3847/1538-4357/acf7bb
2023 doi
-
[69]
C., Oesch, P., Barrufet, L., et al
Williams, C. C., Oesch, P., Barrufet, L., et al. 2021, PANORAMIC - A Pure Parallel Wide Area Legacy Imaging Survey at 1-5 Micron
2021
-
[70]
E., Taam, R
Woosley, S. E., Taam, R. E., & Weaver, T. A. 1986, The Astrophysical Journal, 301, 601, doi: 10.1086/163926
1986 doi
-
[71]
B., Dessart, L., et al
Zenati, Y ., Perets, H. B., Dessart, L., et al. 2023, The Astrophysical Journal, 944, 22, doi: 10.3847/1538-4357/acaf65
2023 doi
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