REVIEW 1 minor 1 cited by
Modified gravity with a linear potential and single phantom crossing struggles to match current data.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.3
2026-06-29 20:28 UTC pith:HSLBVF3S
load-bearing objection Shift-symmetric Horndeski with linear potential identifies three phantom-crossing channels but none fit current data well due to the restricted setup.
Charging Across the Phantom Divide with Modified Gravity
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In shift-symmetric Horndeski gravity plus a linear potential, the nearly conserved scalar charge produces early phantom behavior and permits three routes for the effective equation of state to cross w equals negative one; when the potential lacks a cosmological constant and the crossing occurs only once, none of the routes matches current cosmological observations well.
What carries the argument
The nearly conserved scalar charge, which controls the three possible crossings of w equals negative one in the shift-symmetric Horndeski theory with linear potential.
Load-bearing premise
The models rely on a linear potential without an added cosmological-constant term and assume the equation-of-state crossing occurs only once.
What would settle it
A data set that clearly requires either a non-linear potential or multiple crossings of w equals negative one to match the observed expansion history would falsify the claim that these simpler models have difficulty fitting the data.
If this is right
- Simpler modified-gravity models without a cosmological-constant term cannot easily reproduce the observed late-time acceleration.
- A single crossing of the phantom divide is disfavored by existing measurements of the expansion rate.
- More elaborate scalar potentials or extra terms become necessary for consistency with data.
- Early-universe dynamics remain tightly constrained by the near-conservation of the scalar charge.
Where Pith is reading between the lines
- The same fitting tension may appear in other modified-gravity setups that attempt phantom crossing without extra constant terms.
- High-precision future surveys measuring the dark-energy equation of state at multiple redshifts could directly test the three crossing mechanisms.
- Introducing a cosmological-constant term might ease the data tension but would reduce the model's predictive simplicity.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript analyzes crossing the phantom divide (w=-1) in shift-symmetric Horndeski gravity with a linear potential and no added cosmological constant term. It highlights the role of the nearly conserved scalar charge, identifies three distinct crossing mechanisms, and concludes that none reproduce conditions favored by current data. The central lesson is that such models, restricted to a single crossing, have difficulty fitting observations. An online interactive application solving the evolution equations is provided.
Significance. If the classification of mechanisms and data mismatch hold, the result usefully constrains the viability of simple shift-symmetric Horndeski models without a cosmological constant for late-time cosmology. The emphasis on the conserved charge and the provision of a reproducible interactive tool are strengths that enhance the paper's utility beyond a standard theoretical analysis.
minor comments (1)
- Abstract: the three crossing mechanisms are referenced but not briefly characterized; adding one sentence describing each would improve accessibility without lengthening the abstract unduly.
Simulated Author's Rebuttal
We thank the referee for their positive assessment of the manuscript, accurate summary of our results on the three crossing mechanisms in shift-symmetric Horndeski gravity with linear potential, and recommendation for minor revision. The emphasis on the conserved scalar charge and the interactive tool is appreciated.
Circularity Check
No significant circularity; derivation self-contained
full rationale
The paper derives predictions for phantom crossing in shift-symmetric Horndeski gravity with linear potential by solving the evolution equations and classifying three mechanisms, then comparing outcomes to data. No load-bearing step reduces by construction to a fitted input, self-citation, or renamed ansatz; the central lesson follows from explicit integration of the system rather than definitional equivalence. The provided abstract and context show independent content in the analysis.
Axiom & Free-Parameter Ledger
read the original abstract
Cosmology where the effective dark energy crosses $w=-1$ can be realized in Horndeski gravity with shift symmetric terms plus a linear potential. We highlight the special role of the nearly conserved scalar charge. The theory is highly predictive for the early phantom behavior and we identify three ways to cross $w=-1$. None of them recreate conditions indicated by current data very well. The major lesson is that such modified gravity with a potential lacking a cosmological constant and only crossing $w=-1$ once (hence the less elaborate models) has difficulty fitting current data. We provide an online interactive application solving the system of evolution equations, for the reader to explore various scenarios at will.
Forward citations
Cited by 1 Pith paper
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Constraints on Horndeski Gravity with Phantom Crossing
ACG models embed the observationally preferred phantom-crossing dark energy behavior inside a consistent Horndeski Lagrangian and achieve data fits of similar quality to w0waCDM while being narrowed by perturbative probes.
Reference graph
Works this paper leans on
-
[1]
Linder,Uplifting, Depressing, and Tilting Dark Energy,2506.02122
E. Linder,Uplifting, Depressing, and Tilting Dark Energy,2506.02122
-
[2]
A. Chudaykin and M. Kunz,Modified gravity interpretation of the evolving dark energy in light of DESI data,Phys. Rev. D110(2024) 123524 [2407.02558]. [6]DESIcollaboration,Modified gravity constraints from the full shape modeling of clustering measurements from DESI 2024,JCAP09(2025) 053 [2411.12026]
- [3]
-
[4]
G. Ye, A. Chudaykin, C. Bonvin and M. Kunz,Late-time reconstruction of non-minimally coupled gravity with a smoothness prior,2605.12415
work page internal anchor Pith review Pith/arXiv arXiv
-
[5]
S. Tsujikawa,Crossing the phantom divide in scalar-tensor and vector-tensor theories,Phys. Rev. D113(2026) L041301 [2508.17231]
-
[6]
W. Wolf, P. Ferreira and C. Garc´ ıa-Garc´ ıa,Cosmological constraints on Galileon dark energy with broken shift symmetry,Phys. Rev. D113(2026) 023551 [2509.17586]
work page internal anchor Pith review Pith/arXiv arXiv 2026
-
[7]
M. Cataneo and K. Koyama,Non-parametric exploration of minimally coupled gravity with phantom crossing,2512.13691
-
[8]
Linder,Cosmology after Phantom Crossing by Horndeski Gravity,2512.03139
E. Linder,Cosmology after Phantom Crossing by Horndeski Gravity,2512.03139
-
[9]
Y. Cai, X. Ren, T. Qiu, M. Li and X. Zhang,Quintom theory of dark energy after DESI DR2, Nat. Sci. Rev.(2026) nwag115 [2505.24732]
work page internal anchor Pith review Pith/arXiv arXiv 2026
- [10]
- [11]
-
[12]
Null energy condition violation and beyond Horndeski physics in light of DESI DR2 data,
G. Ye and Y. Cai,Null energy condition violation and beyond Horndeski physics in light of DESI DR2 data,Phys. Rev. D112(2025) L121301 [2503.22515]
-
[13]
Theoretical priors in scalar-tensor cosmologies: Shift-symmetric Horndeski models,
D. Traykova, E. Bellini, P. Ferreira, C. Garc´ ıa-Garc´ ıa, J. Noller and M. Zumalac´ arregui, Theoretical priors in scalar-tensor cosmologies: Shift-symmetric Horndeski models,Phys. Rev. D104(2021) 083502 [2103.11195]
-
[14]
Imperfect Dark Energy from Kinetic Gravity Braiding
C. Deffayet, O. Pujolas, I. Sawicki and A. Vikman,Imperfect Dark Energy from Kinetic Gravity Braiding,JCAP10(2010) 026 [1008.0048]
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[15]
Can dark energy evolve to the Phantom?
A. Vikman,Can dark energy evolve to the Phantom?,Phys. Rev. D71(2005) 023515 [astro-ph/0407107]
work page internal anchor Pith review Pith/arXiv arXiv 2005
-
[16]
E. Bellini and I. Sawicki,Maximal freedom at minimum cost: linear large-scale structure in general modifications of gravity,JCAP07(2014) 050 [1404.3711]
work page internal anchor Pith review Pith/arXiv arXiv 2014
-
[17]
E. Copeland, M. Sami and S. Tsujikawa,Dynamics of dark energy,Int. J. Mod. Phys. D15 (2006) 1753 [hep-th/0603057]
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[18]
Dynamical systems applied to cosmology: dark energy and modified gravity
S. Bahamonde, C. Boehmer, S. Carloni, E. Copeland, W. Fang and N. Tamanini,Dynamical systems applied to cosmology: Dark energy and modified gravity,Phys. Rept.775(2018) 1 [1712.03107]. A Initial conditions The initial conditions are very important to treat consistently. Due to the rapid variation of X(a)∼a −6/(2n−1) from Eq. (3.15), or equivalentlyx ϕ ≈ −...
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[19]
We vary this in order to obtain the desired Ω de,0
Set Ω de,i ≈a −3/(2n−1) i =a 6 i . We vary this in order to obtain the desired Ω de,0
-
[20]
This comes from Eq
Next, we setx g,i =α B = (3/5)Ωde. This comes from Eq. (3.20) and Eq. (3.26) with fi =f early = 3/5 (fi will lie in a different range for othern)
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[21]
(3.3),x k,i is given by xk,i = 1−f i 2n−1 Ωde,i.(A.2) This will also work withα K to guarantee a ghost free initial condition
Using Eq. (3.3),x k,i is given by xk,i = 1−f i 2n−1 Ωde,i.(A.2) This will also work withα K to guarantee a ghost free initial condition
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[22]
(3.15) we getx ϕ,i =−1/(2n−1) = 2
From Eq. (3.15) we getx ϕ,i =−1/(2n−1) = 2
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[23]
This arises from Eq
Setx f,i = 3xϕ,i + 3/2 = 15/2. This arises from Eq. (A.1) in the matter dominated era. – 15 –
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[24]
This comes from Eq
Finally we setx λ,i = Ω7/4 de,i. This comes from Eq. (4.21) and the early time scaling of Ωde(a). We can vary this in order to obtain different late time behavior. Note that since Ω7/4 de,i ≈a 21/2 i the numerical precision ata i = 10−2 must be treated carefully. Values of the quantities at successive timesteps are determined by the evolution equations (f...
discussion (0)
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