Models of exponential and power-law acceleration of the Universe in Horndeski theory without ghosts and Laplace instabilities
Pith reviewed 2026-06-28 09:07 UTC · model grok-4.3
The pith
Designer method finds Horndeski subclasses for stable exponential and power-law cosmic acceleration.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors introduce a designer method within Horndeski's scalar-tensor theory for flat FRW spacetimes. This allows selection of theory functions such that cosmological solutions for exponential and power-law inflation exist without ghosts and Laplace instabilities, providing explicit subclasses of the theory free from these pathologies.
What carries the argument
The designer method applied to flat FRW spacetimes to select Horndeski functions ensuring no ghosts or Laplace instabilities for target expansion histories.
If this is right
- Subclasses of Horndeski theory support exponential inflation without ghosts or Laplace instabilities.
- Subclasses support power-law inflation models without these instabilities.
- The method provides a systematic way to build stable cosmological solutions in Horndeski theory for flat universes.
Where Pith is reading between the lines
- The derived models may be used to study how scalar field dynamics affects the duration of inflation.
- Similar designer techniques could be applied to other spacetime symmetries beyond flat FRW.
- Observational constraints on the expansion history could further restrict the allowed Horndeski functions.
Load-bearing premise
The designer method succeeds in selecting Horndeski functions that eliminate ghosts and Laplace instabilities for the desired flat FRW expansion histories.
What would settle it
An explicit computation for one of the constructed models showing that the no-ghost condition fails or that the Laplacian instability appears at some epoch during the expansion.
read the original abstract
We present a designer method for flat Friedman-Robertson-Walker space-times within the framework of Horndeski's scalar-tensor theory. As a result, one can find subclasses of Horndeski's scalar-tensor theory within which cosmological solutions exist without ghosts and Laplace instabilities. As an example, we found subclasses of Horndeski's theory for exponential and power-law inflation models of the Universe without pathologies.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a designer method to construct subclasses of Horndeski scalar-tensor theory supporting flat FRW solutions with prescribed exponential or power-law expansion histories that are free of ghosts and Laplace instabilities, and supplies explicit examples of such subclasses for inflation models.
Significance. If the constructions are verified to satisfy the no-ghost and no-gradient conditions along the target trajectories, the work supplies concrete, stable Horndeski models for cosmic acceleration. The designer approach itself is a reproducible tool for generating healthy modified-gravity cosmologies, which strengthens its utility beyond the specific exponential and power-law cases presented.
minor comments (1)
- The abstract is terse; a brief statement in the introduction or conclusion summarizing the explicit G_i(φ,X) forms obtained would improve accessibility.
Simulated Author's Rebuttal
We thank the referee for their positive assessment of the manuscript, accurate summary of the designer method, and recommendation to accept. No major comments were raised that require addressing.
Circularity Check
No significant circularity; designer construction is self-contained
full rationale
The paper applies the standard designer approach: prescribe a(t) for exponential or power-law expansion, solve the background equations for the Horndeski G_i(φ,X) functions, then impose the independent no-ghost and no-Laplace-instability conditions on the quadratic action for perturbations. This is a constructive existence proof with external stability criteria that do not reduce to the input a(t) by definition. No self-citations, fitted parameters renamed as predictions, or ansatz smuggling are indicated in the provided text. The derivation chain remains independent of its own outputs.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
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the inverse problem
authors presented constraints on HG from a cosmic shear analysis of the final data release of the Kilo-Degree Survey in combination with DESI measurements of baryon acoustic oscillations, eBOSS observations of redshift space distortions, and cosmic microwave background anisotropies from Planck. In papers [14, 15], the subclasses of HG, which are called No...
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In works [33], [34] the authors started from the anisotropic properties of space-time
used the growth factor of inhomogeneities in model with a scalar field, baryons and dark matter; Huterer and Turner (1999)[24], Nakamura and Chiba (1999) [25] used the luminosity data. In works [33], [34] the authors started from the anisotropic properties of space-time. The designer method has found wide application in HG [26–36]. The rich phenomenology ...
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the inverse problem
≥0,(7) c2 T ≡ w4 w1 ≥0.(8) To exclude ghosts, the following inequalities must be satisfied: QS ≡ w1(4w1w3 + 9w2 2) 3w2 2 >0,(9) QT ≡ w1 4 >0,(10) where w1 ≡2 (G 4 −2XG 4X )−2X(G 5X ˙ϕH−G 5ϕ),(11) w2 ≡ −2G 3X X ˙ϕ+ 4G 4H−16X 2G4XX H+ 4( ˙ϕG4ϕX −4H G 4X )X+ +2G 4ϕ ˙ϕ+ 8X 2HG 5ϕX + 2H X(6G 5ϕ −5G 5X ˙ϕH)−4G 5XX ˙ϕX 2H 2,(12) w3 ≡3X(G 2X + 2XG 2XX ) + 6X(3X ˙...
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there are no pathologies:QT ≈µ/4>0,Q S =rQ T /4>0
In casec 2 S · r 16 ≫1−c 2 T >0, we get the approximation QT µ ≈ 1 4 − 1 4 · c2 S 1 +c 2 S · r 16 1 +c 2 S 5 + 2c2 S · r 16 (1−c 2 T )>0,(50) 8 i.e. there are no pathologies:QT ≈µ/4>0,Q S =rQ T /4>0. The parameterβhas a negative value: β≈ − 1 +c 2 S 6 + 3c2 S · r 16 c2 S 1 +c 2 S · r 16 <0,(51) then the scalar field does not have the initial singularity (...
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In casec 2 S · r 16 =k 2(1−c 2 T )≪1(k̸= 1) from equality (48) and (49) it follows β= 3 (1−k 2)(1−c 2 T )(1 + (k 2 −1)(1−c 2 T )) × × r/48 + 2(1−k 2)(1−c 2 T ) + (k 2 −1) 2(1−c 2 T )2 ,(52) 1− µ 4QT = (1−k 2)(1−c 2 T )2(1 + (k 2 −1)(1−c 2 T )) r/16 + (k 2 −1)(1−c 2 T )(5 + 2(k 2 −1)(1−c 2 T )) .(53) Assuming|1−k 2|(1−c 2 T )≪rand (25), we get QT µ ≈ 1 4 +...
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The conditions for the absence of ghosts are met:Q T ≈µ/4>0, QS =rQ T /4>0
In casec 2 S · r 16 ≫1−c 2 T, we get the approximation QT µ ≈ 1 4 + 1 + (c2 S −1)r/64 4(1 +c 2 Sr/16) ·(1−c 2 T ),(76) β≈ (3c2 S + 1)r/16 4 + (c2 S −1)r/16 .(77) Condition of accelerated mode (74) is rewritten as follows −1/3< c 2 S <32/r−1.(78) It is fulfilled becausec 2 S ≥0,r < r 0 = 0.1. The conditions for the absence of ghosts are met:Q T ≈µ/4>0, QS ...
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[7]
The conditions for the absence of ghosts are confirmed: QT ≈µ/4>0,Q S =rQ T /4>0
In casec 2 S · r 16 =k 2(1−c 2 T )≪1(k̸= 1) from equalities (73) and (75) it follows β= r/16 + 3(k 2 −1)(1−c 2 T ) 4−r/16 + (k 2 −1)(1−c 2 T ) ≈ ≈ r/16 4−r/16 < r/16<0.00625,(79) QT µ = 1 4 1− 4−r/16 + (k 2 −1)(1−c 2 T ) 4(1 + (k 2 −1)(1−c 2 T )) ·(1−c 2 T ) −1 ≈ ≈ 1 4 + 1 4 (1−r/64)(1−c 2 T ).(80) The condition of accelerated expansion0< β <1is satisfied...
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discussion (0)
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