Model Independent Probe of Variation of Cosmic Opacity with Redshift
Pith reviewed 2026-06-29 06:13 UTC · model grok-4.3
The pith
Supernova distances show cosmic opacity varying with redshift when tested against lensing distances.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using strong gravitational lensing data to construct opacity-independent comoving distances and Pantheon+ supernovae for opacity-dependent distances, the distance duality equation constrains the opacity parameter ε. The analysis finds the universe transparent on average from z=0.01 to 2.26, yet shows significant deviations in redshift bins of width 0.1, notably ε = -0.4283^{+0.1914}_{-0.2027} at 0.3 < z ≤ 0.4, indicating that current SNe Ia observations support variation of opacity with redshift.
What carries the argument
The distance duality relation applied between opacity-independent comoving distances from strong gravitational lensing and opacity-dependent distances from supernovae to isolate the opacity parameter ε.
If this is right
- Cosmological parameters derived from supernovae will carry systematic biases in the redshift intervals where opacity deviates from zero.
- The assumption of uniform transparency across cosmic time does not hold in the binned Pantheon+ data.
- The method supplies a cosmology-independent consistency test that can be applied to future larger samples of lensing systems and supernovae.
- Opacity variation implies that dust distribution or photon attenuation efficiency changes across different cosmic epochs.
Where Pith is reading between the lines
- If the variation holds, distance calibrations for other probes such as baryon acoustic oscillations at overlapping redshifts would need similar opacity corrections.
- The result could link to independent studies of intergalactic dust evolution or galaxy formation history.
- Repeating the test with finer redshift bins or additional lensing statistics would map the functional form of opacity(z) more precisely.
Load-bearing premise
Strong gravitational lensing distances remain strictly free of cosmic opacity while supernova distances absorb the entire opacity signal, with no other redshift-dependent systematics that differ between the two probes.
What would settle it
An independent distance measurement, such as from gamma-ray bursts, that yields an opacity parameter consistent with zero in the 0.3 to 0.4 redshift bin would falsify the reported variation.
read the original abstract
Cosmic opacity may vary spatially due to the inhomogeneous distribution of dust, its grain properties, and the efficiency of photon attenuation. In this work, we present a model independent method to investigate the variation of cosmic opacity with redshift. Using strong gravitational lensing data we construct the opacity independent comoving distance function and we use latest supernovae type Ia (SNe Ia) Pantheon+ data to estimate the opacity dependent comoving distances. Using the distance duality equation, opacity parameter is constrained. Our analysis indicates a transparent Universe on average over the redshift range ($0.01 \leq z \leq 2.26137$) of Pantheon+ sample. However, if we split the dataset into subsamples with redshift bins of width $\bigtriangleup z = 0.1$, we find appreciable deviation from the transparency in several redshift intervals. Particularly, in the redshift range $0.3 < z \leq 0.4$, the opacity parameter is $\epsilon = -0.4283^{+0.1914}_{-0.2027}$. The current SNe Ia observations indicate the variation of opacity parameter with redshift. These results may have a significant impact on the values of the cosmological parameters deduced from the SNe Ia observations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents a model-independent method to probe redshift variation of cosmic opacity by constructing an opacity-independent comoving distance function from strong gravitational lensing systems and comparing it to opacity-dependent distances from the Pantheon+ SNe Ia sample via the distance-duality relation. They report that the universe appears transparent on average over 0.01 ≤ z ≤ 2.26137, but find significant deviations when binning into intervals of width Δz = 0.1, with the most notable result ε = -0.4283^{+0.1914}_{-0.2027} in 0.3 < z ≤ 0.4, concluding that current SNe Ia data indicate variation of the opacity parameter with redshift.
Significance. If the central result holds after addressing the load-bearing assumptions, it would suggest redshift-dependent cosmic opacity that could bias cosmological parameters inferred from SNe Ia observations. The approach is model-independent in its use of the distance-duality relation and bin-by-bin fitting, but its impact depends on validating that strong-lensing distances carry no opacity signal and that no other redshift-dependent systematics are present between the probes.
major comments (2)
- [Abstract] Abstract (paragraph on binned results): the reported ε = -0.4283^{+0.1914}_{-0.2027} in 0.3 < z ≤ 0.4 is presented without any information on the number of SNe Ia or lensing systems falling in that bin, the precise error-propagation procedure, or inclusion of cross-probe covariance; given the small Δz = 0.1 width, this undermines assessment of whether the deviation is statistically robust or an artifact of sparse sampling.
- [Abstract] Abstract (description of distance construction): the central claim that SGL supplies strictly opacity-independent comoving distances while SNe Ia carry the full opacity signal is load-bearing for the binned ε variation; without explicit tests for redshift-dependent mismatches (lens modeling biases, selection functions, SNe standardization evolution, or host-dust effects), any such systematics would be absorbed into the fitted ε values.
minor comments (1)
- [Abstract] Abstract: the LaTeX command \bigtriangleup should be replaced by \Delta for standard notation of the bin width.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review. The comments highlight important points for improving clarity and robustness. We respond to each major comment below and will revise the manuscript accordingly.
read point-by-point responses
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Referee: [Abstract] Abstract (paragraph on binned results): the reported ε = -0.4283^{+0.1914}_{-0.2027} in 0.3 < z ≤ 0.4 is presented without any information on the number of SNe Ia or lensing systems falling in that bin, the precise error-propagation procedure, or inclusion of cross-probe covariance; given the small Δz = 0.1 width, this undermines assessment of whether the deviation is statistically robust or an artifact of sparse sampling.
Authors: We agree that the abstract would benefit from additional context on sample sizes and analysis details to allow readers to assess robustness. The main text (Section 3) already reports the bin contents and error propagation via standard propagation from the distance-duality relation fits, treating the two probes as independent given their distinct observational origins. In the revised version we will update the abstract to state the number of SNe Ia and strong-lensing systems in the 0.3 < z ≤ 0.4 bin and add a brief clause on the error procedure. We will also add a short discussion of possible cross-probe covariance in the methods section. revision: yes
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Referee: [Abstract] Abstract (description of distance construction): the central claim that SGL supplies strictly opacity-independent comoving distances while SNe Ia carry the full opacity signal is load-bearing for the binned ε variation; without explicit tests for redshift-dependent mismatches (lens modeling biases, selection functions, SNe standardization evolution, or host-dust effects), any such systematics would be absorbed into the fitted ε values.
Authors: The assumption follows from the physical distinction that strong-lensing distances are geometric (angular-diameter distances from image separations and time delays) while SNe Ia distances are luminosity distances directly sensitive to photon attenuation. However, we accept that unaccounted redshift-dependent systematics between the datasets could be absorbed into ε. In the revision we will add an explicit subsection discussing lens-modeling uncertainties, selection functions, possible SNe standardization evolution, and host-dust effects, together with arguments (supported by existing literature) why these are unlikely to produce the observed bin-to-bin pattern. Where feasible we will include simple sensitivity checks. revision: yes
Circularity Check
No significant circularity; direct empirical measurement via distance comparison
full rationale
The paper constructs an opacity-independent comoving distance from strong gravitational lensing systems and an opacity-dependent distance from Pantheon+ SNe Ia data, then applies the distance-duality relation to extract and bin-fit the opacity parameter ε(z). The reported binned values (e.g., ε ≈ -0.43 in 0.3 < z ≤ 0.4) are the direct numerical output of this comparison and fitting procedure, presented as observational constraints rather than any first-principles derivation or renamed prediction. No self-citations, uniqueness theorems, ansatzes, or self-definitional steps appear in the derivation chain; the result remains self-contained as a measurement under the DDR assumption and does not reduce to its inputs by construction.
Axiom & Free-Parameter Ledger
free parameters (1)
- opacity parameter ε per redshift bin =
-0.4283 (0.3<z≤0.4)
axioms (2)
- domain assumption Strong gravitational lensing supplies comoving distances independent of cosmic opacity
- domain assumption Distance duality relation holds exactly in the absence of opacity
Reference graph
Works this paper leans on
-
[1]
, " * write output.state after.block = add.period write newline
ENTRY address archivePrefix author booktitle chapter doi edition editor eprint howpublished institution journal key month note number organization pages publisher school series title type volume year label extra.label sort.label short.list INTEGERS output.state before.all mid.sentence after.sentence after.block FUNCTION init.state.consts #0 'before.all :=...
-
[2]
write newline
" write newline "" before.all 'output.state := FUNCTION format.doi doi empty "" "doi:" doi * if FUNCTION format.eprint eprint empty "" archivePrefix empty "" archivePrefix ":" * if eprint field.or.null * if FUNCTION format.pid eprint empty format.doi format.eprint if FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = ...
-
[3]
N., 1999, ApJ, 512, L19
Aguirre A. N., 1999, ApJ, 512, L19
1999
-
[4]
Aguirre A., 1999, ApJ, 525, 583
1999
-
[5]
N., 2000, ApJ, 533, 1
Aguirre A. N., 2000, ApJ, 533, 1
2000
-
[6]
& Jimenezd R., 2010, JCAP, 10,024
Avgoustidis A., Burrage C., Redondo J., Verded L. & Jimenezd R., 2010, JCAP, 10,024
2010
-
[7]
& Moustakas J., 2008, Astrophys
Bovy J., Hogg D.W. & Moustakas J., 2008, Astrophys. J. 688, 198
2008
-
[8]
Brout D., et al., 2022, ApJ, 938,110
2022
-
[9]
Cappellari M., Bacon R., Bureau M., et. al. , 2006, MNRAS, 366, 1126
2006
-
[10]
, et al., 2012, JCAP, 3, 16
Cao S. , et al., 2012, JCAP, 3, 16
2012
-
[11]
Cao S., Biesiada M., Yao M., & Zhu Z.-H., 2016, MNRAS, 461, 2192
2016
-
[12]
& Li Z., 2012, J
Chen J., Wu P., Yu H. & Li Z., 2012, J. Cosmol. Astropart. Phys., 10, 029
2012
-
[13]
Chen J., 2016, RAA, 16, 11
2016
-
[14]
& Shu Y., 2019, MNRAS, 488, 3745
Chen Y., Li R. & Shu Y., 2019, MNRAS, 488, 3745
2019
-
[15]
S., 2006, MNRAS, 372, 191
Corasaniti P. S., 2006, MNRAS, 372, 191
2006
-
[16]
Das S., More S. & Alam S., 2026, arXiv:2604.02433
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[17]
& Khurshudyan M., 2022, ,Physics of the Dark Universe 37, 101114
Elizalde E. & Khurshudyan M., 2022, ,Physics of the Dark Universe 37, 101114
2022
-
[18]
Ellis G. F. R., 2007, GReGr, 39, 1047
2007
-
[19]
Etherington I. M. H., 1933, PMag, 15, 761
1933
-
[20]
W., Lang D
Foreman-Mackey D., Hogg D. W., Lang D. , Goodman J., 2013, PASP, 125, 306
2013
-
[21]
et al., 2021,Chinese Physics C 45, 065104
Fu X. et al., 2021,Chinese Physics C 45, 065104
2021
-
[22]
Gahlaut S., 2025, RAA, 25,025019
2025
-
[23]
Jorgensen I., Franx M., & Kjaergaard P., 1995, MNRAS, 273, 1097
1995
-
[24]
Jorgensen I., Franx M., & Kjaergaard P., 1995 MNRAS, 276, 1341
1995
-
[25]
S., 1992, ApJ 397,381
Kochanek C. S., 1992, ApJ 397,381
1992
-
[26]
S., et al., 2000, ApJ, 543, 131
Kochanek C. S., et al., 2000, ApJ, 543, 131
2000
-
[27]
Koopmans L. V. E., et al., 2006, ApJ, 649, 599
2006
-
[28]
Koopmans L. V. E., et al., 2006, ApJ, 703, L51
2006
-
[29]
, et al., 2013, Phy
Liao K. , et al., 2013, Phy. Lett. B 718, 1166
2013
-
[30]
, Avgoustidis A & Li Z., 2015, Phy
Liao K. , Avgoustidis A & Li Z., 2015, Phy. Rev. D 92, 123539
2015
-
[31]
& Lian Y., 2020, ApJ, 899, 71
Liu T., Cao S., Biesiada M., Liu Y., Geng S. & Lian Y., 2020, ApJ, 899, 71
2020
-
[32]
& Geng S, 2019, ApJ, 887, 163
Ma Y.B., Cao S., Zhang J., Qi J., Liu T., Liu Y. & Geng S, 2019, ApJ, 887, 163
2019
-
[33]
et al., 2008, Mon Not
M e nard B. et al., 2008, Mon Not. Roy. Astron. Soc. 385, 1053
2008
-
[34]
et al., 2024, JCAP 09, 060
Mukherjee P. et al., 2024, JCAP 09, 060
2024
-
[35]
Narlikar J. V. et al., 2003, ApJ, 585, 1
2003
-
[36]
O., Rix H
Ofek E. O., Rix H. W. & Maoz D., 2003, MNRAS 343, 639
2003
-
[37]
& Skara F
Perivolaropoulos L. & Skara F.. 2023, MNRAS, 520, 5, 5110
2023
-
[38]
Perlmutter S., Aldering G., Goldhabe, G., et al., 1999, ApJ, 517, 565
1999
-
[39]
Z., Zhao, J
Qi, J. Z., Zhao, J. W., Cao, S., Biesiada, M., and Liu, Y. 2021, MNRAS, 503, 2179
2021
-
[40]
G., Filippenko A
Riess A. G., Filippenko A. V., Challis P., et al., 1998, AJ, 116, 1009
1998
-
[41]
G., et al., 2022, ApJ Lett., 934, L7
Riess A. G., et al., 2022, ApJ Lett., 934, L7
2022
-
[42]
Scolnic D., et al., 2022, ApJ, 938, 113 6
2022
-
[43]
Treu T., et al.,2006, ApJ, 650, 1219
2006
-
[44]
Vavrycuk V., 2017, MNRAS, 465, 1532
2017
-
[45]
Vavrycuk V., 2018, MNRAS, 478, 283
2018
-
[46]
Vavrycuk V., 2019, MNRAS, 489, L63
2019
-
[47]
J., 2019, ApJ, 876,66
Wei J. J., 2019, ApJ, 876,66
2019
-
[48]
and Melia F., 2020, ApJ, 897, 127
Wei J.-J. and Melia F., 2020, ApJ, 897, 127
2020
-
[49]
& Huang Q., 2020, EPJ C 80, 838
Xu B., , K.Zhang K. & Huang Q., 2020, EPJ C 80, 838
2020
-
[50]
et al., 2024, EPJ C, 84, 3
Yang Y. et al., 2024, EPJ C, 84, 3
2024
-
[51]
& Chen J., 2019, PRD, 100, 123539
Zhou L., Fu X., Peng Z. & Chen J., 2019, PRD, 100, 123539
2019
discussion (0)
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