Recognition: unknown
The End of the First Act: Spectral Running, Interacting Dark Radiation, and the Hubble Tension in Light of ACT DR6 Data
Pith reviewed 2026-05-07 12:34 UTC · model grok-4.3
The pith
Including running of the spectral index in models with self-interacting dark radiation relaxes the bound on extra radiation and reduces the Hubble tension.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Confronting an extended cosmological model that includes self-interacting dark radiation together with running α_s and running of the running β_s of the spectral index against Planck, ACT DR6, DESI DR2, and uncalibrated Pantheon+ data yields a relaxed upper bound ΔN_eff < 0.58 at 95% CL, a 2.9σ preference for α_s > 0, and reduces the Hubble tension to 2.2σ. In the variant where dark radiation decouples from dark matter near matter-radiation equality, the bound becomes ΔN_eff < 0.68 and the tension drops below 2σ.
What carries the argument
Self-interacting dark radiation combined with the parameters α_s and β_s that describe the running and running of the running of the primordial scalar spectral index, which adjust the power on small scales to accommodate more extra radiation.
Load-bearing premise
The constraints rest on the specific choice of self-interacting dark radiation plus spectral running model being sufficient to describe the data.
What would settle it
A future measurement finding no evidence for spectral running on small scales or a Hubble constant value that remains in strong tension after including these parameters would falsify the proposed resolution.
Figures
read the original abstract
We point out that constraints on $\Delta N_\mathrm{eff}$ reported by the ACT collaboration in their DR6 data release are surprisingly sensitive to the assumptions made about the initial power spectrum from inflation. The ACT collaboration reports no evidence of new light degrees of freedom alongside a low value of the expansion rate, thus confirming the Hubble tension. However, as we show here, when considering self-interacting dark radiation and including running, $\alpha_s$, and running of the running, $\beta_s$, of the spectral index $n_s$, the picture changes significantly. Confronting this extended model with Planck, ACT DR6, DESI DR2, and uncalibrated Pantheon+ data, we find the significantly relaxed bound $\Delta N_\text{eff}< 0.58$ at 95$\%$ CL, together with a $2.9 \sigma$ ($2.6 \sigma$) preference for $\alpha_s>0$ ($\beta_s>0$), while the Hubble tension is reduced to $2.2 \sigma$ with only three more parameters compared to $\Lambda$CDM. If the dark radiation fluid is initially coupled to dark matter, and undergoes dark radiation-matter decoupling (DRMD) around matter-radiation equality, predicting dark acoustic oscillations with drag horizon $r_{d,\mathrm{DAO}} \approx 60 \,\mathrm{Mpc}/h$, the bound is further relaxed to $\Delta N_\text{eff}< 0.68$ at 95$\%$ CL, reducing the Hubble tension below $2\sigma$. We also discuss how $\alpha_s$ and $\beta_s$ could naturally appear in inflationary scenarios, possibly connected to the end of a first act of inflation. In this case dark radiation is mostly probed by scales covered by Planck and DESI, while smaller scales carry information on inflationary dynamics.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper argues that ACT DR6 constraints on extra relativistic degrees of freedom (ΔN_eff) are sensitive to assumptions about the primordial power spectrum. By extending the model to include self-interacting dark radiation together with running α_s and running-of-the-running β_s of the scalar spectral index, the 95% CL upper bound relaxes to ΔN_eff < 0.58, a 2.9σ (2.6σ) preference for α_s > 0 (β_s > 0) appears, and the Hubble tension drops to 2.2σ. A further variant with dark radiation-matter decoupling (DRMD) near matter-radiation equality yields ΔN_eff < 0.68 and tension below 2σ, while the running parameters are linked to possible inflationary dynamics at the end of a first inflationary phase.
Significance. If the reported preferences and relaxed bounds are robust, the work demonstrates that standard ACT analyses may be underestimating the allowed parameter space for new light species once realistic inflationary extensions are considered. The reduction of the Hubble tension to 2.2σ (or below 2σ) with only three additional parameters relative to ΛCDM is quantitatively interesting and could motivate targeted follow-up with future CMB and large-scale structure data. The discussion of possible inflationary origins for α_s and β_s also provides a concrete link between early-universe dynamics and late-time observables.
major comments (3)
- [Abstract, results] Abstract and results section: the 2.9σ preference for α_s > 0 and the relaxation of the ΔN_eff bound are obtained from a joint fit to Planck + ACT DR6 + DESI DR2 + Pantheon+; it is not shown whether the same preference survives when ACT data are removed or when α_s and β_s are fixed to zero, which would test whether the improvement is driven by the extended model or by the specific data combination.
- [DRMD discussion] DRMD variant: the drag horizon is fixed at r_d,DAO ≈ 60 Mpc/h with decoupling near matter-radiation equality; the manuscript should quantify how sensitive the further relaxation to ΔN_eff < 0.68 is to this choice and whether the value is theoretically motivated or tuned to the data.
- [Hubble tension subsection] Hubble tension quantification: the reduction from the baseline tension (presumably ~4–5σ in ΛCDM with the same datasets) to 2.2σ must be accompanied by an explicit comparison table showing the tension metric (e.g., difference in H0 posterior means divided by combined uncertainty) for both the baseline and extended models.
minor comments (2)
- [Model definition] Notation for the self-interaction strength and the DRMD decoupling redshift should be defined once in the text and used consistently in all equations and figures.
- [Figures] Figure captions for the posterior plots should explicitly state the datasets used in each chain and whether the contours include or exclude the running parameters.
Simulated Author's Rebuttal
We thank the referee for their thorough review and constructive comments. We address each major comment point by point below and will revise the manuscript accordingly to improve clarity and robustness.
read point-by-point responses
-
Referee: [Abstract, results] Abstract and results section: the 2.9σ preference for α_s > 0 and the relaxation of the ΔN_eff bound are obtained from a joint fit to Planck + ACT DR6 + DESI DR2 + Pantheon+; it is not shown whether the same preference survives when ACT data are removed or when α_s and β_s are fixed to zero, which would test whether the improvement is driven by the extended model or by the specific data combination.
Authors: We agree that these additional checks would strengthen the presentation. In the revised manuscript we will add two sets of results: (i) constraints from Planck + DESI DR2 + Pantheon+ alone (excluding ACT DR6) to test whether the preference for α_s > 0 and β_s > 0 persists without ACT, and (ii) constraints with α_s = β_s = 0 to isolate the effect of the running parameters on the ΔN_eff bound. These will demonstrate that the relaxation arises from the combination of the extended primordial spectrum with the full dataset. revision: yes
-
Referee: [DRMD discussion] DRMD variant: the drag horizon is fixed at r_d,DAO ≈ 60 Mpc/h with decoupling near matter-radiation equality; the manuscript should quantify how sensitive the further relaxation to ΔN_eff < 0.68 is to this choice and whether the value is theoretically motivated or tuned to the data.
Authors: The fiducial choice r_d,DAO ≈ 60 Mpc/h corresponds to decoupling near matter-radiation equality, which is theoretically motivated because it places the dark acoustic oscillations on scales that can be probed by DESI while allowing a larger ΔN_eff without violating other constraints. It is not tuned to maximize the relaxation but chosen as a representative value for this class of models. In the revision we will add a short sensitivity study varying r_d,DAO by ±10 Mpc/h around the fiducial value and report the resulting ΔN_eff bounds. We will also expand the text to clarify the theoretical motivation from possible end-of-inflation dynamics. revision: yes
-
Referee: [Hubble tension subsection] Hubble tension quantification: the reduction from the baseline tension (presumably ~4–5σ in ΛCDM with the same datasets) to 2.2σ must be accompanied by an explicit comparison table showing the tension metric (e.g., difference in H0 posterior means divided by combined uncertainty) for both the baseline and extended models.
Authors: We agree that an explicit side-by-side comparison improves transparency. In the revised manuscript we will insert a table in the Hubble tension subsection that reports the tension metric (difference in H0 posterior means divided by the combined uncertainty) for the baseline ΛCDM model and for each extended model (running only, self-interacting DR, and DRMD variant) using identical datasets. This will document the reduction to 2.2σ (and below 2σ for the DRMD case) in a clear, quantitative manner. revision: yes
Circularity Check
No significant circularity in the derivation chain.
full rationale
The paper extends a cosmological model by adding self-interacting dark radiation plus running parameters α_s and β_s, then reports posterior constraints obtained by fitting this model to Planck + ACT DR6 + DESI DR2 + Pantheon+ data. The reported relaxed ΔN_eff bound, 2.9σ preference for α_s > 0, and reduction of Hubble tension to 2.2σ are direct outputs of that fit. No first-principles derivation is claimed whose central result reduces by construction to its own inputs; the analysis is standard Bayesian parameter estimation. The paper explicitly flags sensitivity to the assumed primordial spectrum, which is the opposite of smuggling an ansatz. No self-citation is invoked as load-bearing evidence for a uniqueness theorem or ansatz. The discussion of possible inflationary origins for running is qualitative and does not support the quantitative claims.
Axiom & Free-Parameter Ledger
free parameters (3)
- α_s
- β_s
- ΔN_eff
axioms (2)
- domain assumption The primordial power spectrum includes non-zero running α_s and running-of-running β_s
- ad hoc to paper Dark radiation can be self-interacting and initially coupled to dark matter with decoupling near matter-radiation equality
invented entities (2)
-
self-interacting dark radiation
no independent evidence
-
dark radiation-matter decoupling (DRMD) with drag horizon r_d,DAO ≈ 60 Mpc/h
no independent evidence
Reference graph
Works this paper leans on
-
[1]
Inflaton with proxy running We can effectively capture the dynamics of such heavy fields by considering only their indirect effect, such that they appear just as an explicit time-dependence in the inflaton potential,V(ϕ, N), whereϕis the inflaton andN≈Htis the number ofe-folds. In this case, using the standard relationk=aHat horizon crossing and the slow-...
-
[2]
SIDR +α s +β s
Curvaton with proxy running If the observed perturbations are created by the curvatonσ, instead of the inflaton, the above formulae simplify [121]. In this case the spectral tilt becomes nσ −1 =−2ϵ+ 2 3 V ′′ H2 ,(33) where theϵcomes from the background inflaton dynamics, and primes are now partial derivatives with respect toσ. If we now assume that the cu...
2000
- [3]
-
[4]
The Atacama Cosmology Telescope: DR6 Power Spectra, Likelihoods and $\Lambda$CDM Parameters
T. Louiset al.(Atacama Cosmology Telescope), The Atacama Cosmology Telescope: DR6 power spectra, likelihoods and ΛCDM parameters, JCAP11, 062, arXiv:2503.14452 [astro- ph.CO]
work page internal anchor Pith review arXiv
-
[5]
The Atacama Cosmology Telescope: DR6 Constraints on Extended Cosmological Models
E. Calabreseet al.(Atacama Cosmology Telescope), The Atacama Cosmology Telescope: DR6 constraints on extended cosmological models (2025), arXiv:2503.14454 [astro-ph.CO]
work page internal anchor Pith review arXiv 2025
-
[6]
E. Camphuiset al.(SPT-3G), SPT-3G D1: CMB temperature and polarization power spectra and cosmology from 2019 and 2020 observations of the SPT-3G main field, Phys. Rev. D 113, 083504 (2026), arXiv:2506.20707 [astro-ph.CO]
work page internal anchor Pith review arXiv 2019
-
[7]
B. Beringueet al., The Atacama Cosmology Telescope: DR6 power spectrum foreground model and validation, JCAP10, 082, arXiv:2506.06274 [astro-ph.CO]
- [8]
- [9]
-
[10]
Combining CMB datasets with consistent foreground modelling
M. Tristram, M. Douspis, A. Gorce, S. Henrot-Versill´ e, L. T. Hergt, S. Ilic, L. McBride, M. Mu˜ noz-Echeverr´ ıa, E. Pointecouteau, and L. Salvati, Combining CMB datasets with consistent foreground modelling (2025), arXiv:2511.04733 [astro-ph.CO]
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[11]
M. Escudero, M. Ovchynnikov, and N. Weiner, What does it take to haveN eff <3 at CMB times? (2026), arXiv:2603.22391 [hep-ph]
- [12]
-
[13]
S. Goldstein and J. C. Hill, A 2% determination ofN eff from primordial element abun- dance, cosmic microwave background, and baryon acoustic oscillation measurements (2026), arXiv:2603.13226 [astro-ph.CO]
-
[14]
DESI DR2 Results II: Measurements of Baryon Acoustic Oscillations and Cosmological Constraints
M. Abdul Karimet al.(DESI), DESI DR2 results. II. Measurements of baryon acoustic oscillations and cosmological constraints, Phys. Rev. D112, 083515 (2025), arXiv:2503.14738 [astro-ph.CO]
work page internal anchor Pith review arXiv 2025
-
[15]
A. G. Riesset al., A Comprehensive Measurement of the Local Value of the Hubble Constant with 1 km s –1 Mpc–1 Uncertainty from the Hubble Space Telescope and the SH0ES Team, Astrophys. J. Lett.934, L7 (2022), arXiv:2112.04510 [astro-ph.CO]
work page internal anchor Pith review arXiv 2022
-
[16]
E. Di Valentinoet al.(CosmoVerse Network), The CosmoVerse White Paper: Addressing observational tensions in cosmology with systematics and fundamental physics, Phys. Dark Univ.49, 101965 (2025), arXiv:2504.01669 [astro-ph.CO]
work page internal anchor Pith review arXiv 2025
-
[17]
L. Knox and M. Millea, Hubble constant hunter’s guide, Phys. Rev. D101, 043533 (2020), arXiv:1908.03663 [astro-ph.CO]. 22
- [18]
- [19]
- [20]
-
[21]
Sterile neutrino self-interactions:H 0 tension and short-baseline anomalies,
M. Archidiacono, S. Gariazzo, C. Giunti, S. Hannestad, and T. Tram, Sterile neutrino self- interactions:H 0 tension and short-baseline anomalies, JCAP12, 029, arXiv:2006.12885 [astro-ph.CO]
-
[22]
N. Blinov and G. Marques-Tavares, Interacting radiation after Planck and its implications for the Hubble Tension, JCAP09, 029, arXiv:2003.08387 [astro-ph.CO]
- [23]
- [24]
- [25]
- [26]
-
[27]
N. Sch¨ oneberg and G. Franco Abell´ an, A step in the right direction? Analyzing the Wess Zumino Dark Radiation solution to the Hubble tension, JCAP12, 001, arXiv:2206.11276 [astro-ph.CO]
- [28]
-
[29]
F. Niedermann and M. S. Sloth, New early dark energy, Phys. Rev. D103, L041303 (2021), arXiv:1910.10739 [astro-ph.CO]
-
[30]
F. Niedermann and M. S. Sloth, Resolving the Hubble tension with new early dark energy, Phys. Rev. D102, 063527 (2020), arXiv:2006.06686 [astro-ph.CO]
- [31]
-
[32]
F. Niedermann and M. S. Sloth, New Early Dark Energy as a solution to theH 0 andS 8 tensions (2023), arXiv:2307.03481 [hep-ph]
- [33]
-
[34]
A. Chatrchyan, F. Niedermann, V. Poulin, and M. S. Sloth, Confronting cold new early dark energy and its equation of state with updated CMB, supernovae, and BAO data, Phys. Rev. D111, 043536 (2025), arXiv:2408.14537 [astro-ph.CO]
- [35]
-
[36]
F. Niedermann and M. S. Sloth, Hot new early dark energy, Phys. Rev. D105, 063509 (2022), arXiv:2112.00770 [hep-ph]
-
[37]
F. Niedermann and M. S. Sloth, Hot new early dark energy: Towards a unified dark sector of neutrinos, dark energy and dark matter, Phys. Lett. B835, 137555 (2022), arXiv:2112.00759 [hep-ph]
- [38]
- [39]
- [40]
-
[41]
F.-Y. Cyr-Racine and K. Sigurdson, Cosmology of atomic dark matter, Phys. Rev. D87, 103515 (2013), arXiv:1209.5752 [astro-ph.CO]
- [42]
- [43]
-
[44]
Z. Houet al., Constraints on Cosmology from the Cosmic Microwave Background Power Spectrum of the 2500 deg 2 SPT-SZ Survey, Astrophys. J.782, 74 (2014), arXiv:1212.6267 [astro-ph.CO]
- [45]
-
[46]
M.-a. Watanabe, S. Kanno, and J. Soda, Inflationary Universe with Anisotropic Hair, Phys. Rev. Lett.102, 191302 (2009), arXiv:0902.2833 [hep-th]
-
[47]
P. Adshead and M. Wyman, Chromo-Natural Inflation: Natural inflation on a steep potential with classical non-Abelian gauge fields, Phys. Rev. Lett.108, 261302 (2012), arXiv:1202.2366 [hep-th]
-
[48]
A. Notari and K. Tywoniuk, Dissipative Axial Inflation, JCAP12, 038, arXiv:1608.06223 [hep-th]. 24
- [49]
- [50]
-
[51]
O. Iarygina, E. I. Sfakianakis, R. Sharma, and A. Brandenburg, Backreaction of axion-SU(2) dynamics during inflation, JCAP04, 018, arXiv:2311.07557 [astro-ph.CO]
- [52]
-
[53]
D. Jamieson, A. Caravano, and E. Komatsu, Primordial power spectrum and bispec- trum from lattice simulations of axion-U(1) inflation, Phys. Rev. D112, 103531 (2025), arXiv:2507.22285 [astro-ph.CO]
-
[54]
Silk and M
J. Silk and M. S. Turner, Double Inflation, Phys. Rev. D35, 419 (1987)
1987
-
[55]
Polarski and A
D. Polarski and A. A. Starobinsky, Spectra of perturbations produced by double inflation with an intermediate matter dominated stage, Nucl. Phys. B385, 623 (1992)
1992
- [56]
- [57]
- [58]
-
[59]
G. Dvali and S. Kachru, New old inflation, inFrom Fields to Strings: Circumnavigating Theoretical Physics: A Conference in Tribute to Ian Kogan(2003) pp. 1131–1155, arXiv:hep- th/0309095
-
[60]
Chain Inflation in the Landscape: "Bubble Bubble Toil and Trouble"
K. Freese and D. Spolyar, Chain inflation: ’Bubble bubble toil and trouble’, JCAP07, 007, arXiv:hep-ph/0412145
-
[61]
R. Easther, Folded inflation, primordial tensors, and the running of the scalar spectral index (2004), arXiv:hep-th/0407042
work page internal anchor Pith review arXiv 2004
-
[62]
G. D’Amico and N. Kaloper, Rollercoaster cosmology, JCAP08, 058, arXiv:2011.09489 [hep- th]
-
[63]
G. D’Amico, N. Kaloper, and A. Westphal, Double Monodromy Inflation: A Gravity Waves Factory for CMB-S4, LiteBIRD and LISA, Phys. Rev. D104, L081302 (2021), arXiv:2101.05861 [hep-th]
-
[64]
G. D’Amico, N. Kaloper, and A. Westphal, General double monodromy inflation, Phys. Rev. D105, 103527 (2022), arXiv:2112.13861 [hep-th]. 25
-
[65]
G. D’Amico, A. A. Geraci, N. Kaloper, and A. Westphal, Very-High-Frequency Gravitational Waves from Multi-Monodromy Inflation (2026), arXiv:2601.09834 [hep-ph]
-
[66]
T. Kobayashi and F. Takahashi, Running Spectral Index from Inflation with Modulations, JCAP01, 026, arXiv:1011.3988 [astro-ph.CO]
-
[67]
F. Takahashi, The Spectral Index and its Running in Axionic Curvaton, JCAP06, 013, arXiv:1301.2834 [astro-ph.CO]
- [68]
- [69]
- [70]
-
[71]
C. van de Bruck and C. Longden, Running of the Running and Entropy Perturbations During Inflation, Phys. Rev. D94, 021301 (2016), arXiv:1606.02176 [astro-ph.CO]
-
[72]
M. Fairbairn, L. Heurtier, and M. O. Olea-Romacho, Is ΛCDM on the run? Reconciling the CMB with the Lyman-αForest (2025), arXiv:2511.01612 [astro-ph.CO]
- [73]
- [74]
-
[75]
N. Barnaby, E. Pajer, and M. Peloso, Gauge Field Production in Axion Inflation: Conse- quences for Monodromy, non-Gaussianity in the CMB, and Gravitational Waves at Interfer- ometers, Phys. Rev. D85, 023525 (2012), arXiv:1110.3327 [astro-ph.CO]
-
[76]
N. Barnaby, R. Namba, and M. Peloso, Phenomenology of a Pseudo-Scalar Inflaton: Natu- rally Large Nongaussianity, JCAP04, 009, arXiv:1102.4333 [astro-ph.CO]
- [77]
- [78]
- [79]
-
[80]
N. Arkani-Hamed and J. Maldacena, Cosmological Collider Physics (2015), arXiv:1503.08043 [hep-th]
work page Pith review arXiv 2015
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.