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arxiv: 2507.17095 · v2 · pith:4MDLAZ43new · submitted 2025-07-23 · 🌀 gr-qc · astro-ph.CO· hep-th

Connecting Early Dark Energy to Late Dark Energy by the Diluting Matter Potential

Pith reviewed 2026-05-21 23:52 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.COhep-th
keywords early dark energylate dark energyHubble tensionscale invariancetunnelingeffective potentialsound horizoncosmological constant
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The pith

A density-dependent effective potential in scale-invariant gravity connects early dark energy to late dark energy through matter dilution.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper proposes a scale-invariant theory with two scalar fields and a metric-independent measure that, after integrating out the measure degrees of freedom, produces an effective potential in the Einstein frame dependent on matter density. This potential features flat regions supporting inflation, an early dark energy phase, and a late dark energy phase. As the universe expands and matter dilutes, the system can tunnel from the early to the late dark energy state. This setup modifies the sound horizon at recombination to reduce the Hubble tension without disrupting the standard late-time expansion, and fits data from CMB, BAO, and local H0 measurements with an early dark energy fraction around 0.3 at redshift 5000.

Core claim

In this scale invariant gravity theory the spontaneous breaking of scale symmetry by integrating the measure degrees of freedom yields an effective potential that depends on the density of dust particles and possesses three flat regions corresponding to inflation, early dark energy and late dark energy; tunneling between the early and late dark energy minima becomes efficient once matter has diluted sufficiently, thereby altering the pre-recombination expansion history to ease the Hubble tension while leaving the post-recombination cosmology unchanged.

What carries the argument

The effective potential dependent on the density of the particles, which arises from integrating the measure degrees of freedom and contains three flat regions for different cosmological eras.

If this is right

  • Modifies the sound horizon prior to recombination to alleviate the Hubble tension.
  • Preserves the standard late-time cosmology consistent with BAO and local H0 measurements.
  • Provides a unified framework including inflation, early dark energy, and late dark energy phases.
  • Yields a best-fit early dark energy fraction of approximately 0.3 at redshift 5000 when fitted to reduced CMB data.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The density-dependent potential may offer a natural resolution to the coincidence problem of why dark energy dominates now.
  • Extending the model to include full CMB likelihood could provide stronger tests of the tunneling transition timing.
  • Similar mechanisms might apply to other early-universe transitions in modified gravity theories.

Load-bearing premise

Integrating the degrees of freedom that define the measure spontaneously breaks the scale symmetry, leaving an effective potential that is dependent on the density of the particles and contains three flat regions suitable for inflation, early dark energy, and late dark energy, with tunneling becoming efficient at a certain dilution point.

What would settle it

A precise measurement of the early dark energy fraction from full CMB likelihood data that deviates significantly from the predicted value around 0.3 at redshift 5000 would falsify the model.

Figures

Figures reproduced from arXiv: 2507.17095 by Eduardo I. Guendelman, Pedro Labrana, Ramon Herrera.

Figure 1
Figure 1. Figure 1: FIG. 1: Schematic representation the effective potential [PITH_FULL_IMAGE:figures/full_fig_p008_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Schematic representation of the total potential [PITH_FULL_IMAGE:figures/full_fig_p012_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: In this plot, the grey region is the 1 [PITH_FULL_IMAGE:figures/full_fig_p018_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: This plot shows the 1 [PITH_FULL_IMAGE:figures/full_fig_p019_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Evolution of the percolation parameter [PITH_FULL_IMAGE:figures/full_fig_p020_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Evolution of the different fluid components in terms of the scale factor. We have used logarithmic scales on both axes [PITH_FULL_IMAGE:figures/full_fig_p021_6.png] view at source ↗
read the original abstract

In this work we study a scale invariant gravity theory containing two scalar fields, dust particles and a measure defined from degrees of freedom independent of the metric. The integration of the degrees of freedom that define the measure spontaneously break the scale symmetry, leaving us in the Einstein frame with an effective potential that is dependent on the density of the particles. The potential contains three flat regions, one for inflation, another for early dark energy and the third for late dark energy. At a certain point, as the matter dilutes, tunneling from the early dark energy to the late dark energy can start efficiently. This mechanism naturally alleviated the observed Hubble tension by modifying the sound horizon prior to recombination while preserving late-time cosmology. Moreover, the model predictions are consistent with observations from the reduced CMB, BAO, and local measurement of $H_0$, providing a coherent and unified description of the universe. In this context, the Bayesian analysis of these datasets confirms the viability of our scenario, with the best-fit parameters indicating an early dark energy fraction of $f_{\rm NEDE}\approx 0.3$ at a redshift of $z^{\prime}=5000$. This preliminary estimate, obtained using the reduced CMB dataset, is expected to be tightened once the full CMB likelihood is considered.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript presents a scale-invariant gravitational theory involving two scalar fields, dust particles, and a measure constructed from metric-independent degrees of freedom. Integrating out the measure spontaneously breaks scale symmetry, producing an effective potential in the Einstein frame that depends on matter density and features three flat regions corresponding to inflation, early dark energy (EDE), and late dark energy (LDE). The central claim is that as matter dilutes, tunneling from the EDE minimum to the LDE minimum becomes efficient, reducing the sound horizon prior to recombination to alleviate the Hubble tension while preserving late-time cosmology. A Bayesian analysis of reduced CMB, BAO, and local H0 data yields a best-fit EDE fraction f_NEDE ≈ 0.3 at z' = 5000, presented as a preliminary result.

Significance. If the tunneling dynamics can be shown to activate at the appropriate epoch, the framework supplies a unified mechanism connecting EDE and LDE phases through a density-dependent potential generated by spontaneous scale-symmetry breaking. This offers a coherent approach to the Hubble tension that is in principle falsifiable with full CMB data. The explicit Bayesian fit with a quoted numerical value for f_NEDE is a constructive element, though the reduced dataset limits the robustness of the current constraints.

major comments (2)
  1. [Abstract and effective-potential derivation] The assertion that tunneling from the EDE to the LDE minimum 'can start efficiently' at a certain dilution point is load-bearing for the claim that the transition modifies the sound horizon at z ≳ 1100 while leaving late-time cosmology untouched. No explicit computation of the Euclidean bounce action, prefactor, or decay rate Γ(ρ_m) as a function of matter density appears in the manuscript (see the abstract and the discussion of the effective potential).
  2. [Section deriving the effective potential] The integration of the measure degrees of freedom is stated to produce an effective potential with three flat regions, yet the manuscript supplies no detailed derivation or explicit functional form of this potential (including its dependence on particle density). This omission prevents verification of the flatness conditions and the spontaneous symmetry-breaking step that underpins the entire scenario.
minor comments (2)
  1. The redshift notation z' = 5000 should be defined explicitly; it is unclear whether this marks the onset of efficient tunneling or the epoch at which f_NEDE is evaluated.
  2. [Bayesian analysis] The abstract refers to a 'reduced CMB dataset'; the manuscript should state precisely which likelihoods were omitted and how this choice affects the reported constraints.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed feedback on our manuscript. We have addressed each major comment point by point below. Where the comments identify areas needing additional detail or clarification, we have revised the manuscript accordingly to strengthen the presentation of the tunneling dynamics and the derivation of the effective potential.

read point-by-point responses
  1. Referee: [Abstract and effective-potential derivation] The assertion that tunneling from the EDE to the LDE minimum 'can start efficiently' at a certain dilution point is load-bearing for the claim that the transition modifies the sound horizon at z ≳ 1100 while leaving late-time cosmology untouched. No explicit computation of the Euclidean bounce action, prefactor, or decay rate Γ(ρ_m) as a function of matter density appears in the manuscript (see the abstract and the discussion of the effective potential).

    Authors: We thank the referee for identifying this key point. The original manuscript emphasized the qualitative features of the density-dependent potential and the resulting tunneling mechanism. To provide quantitative support, the revised manuscript includes a new subsection (and accompanying appendix) that computes the Euclidean bounce action in the thin-wall limit for the barrier separating the EDE and LDE minima. We also derive an estimate for the decay rate Γ(ρ_m), showing that tunneling becomes efficient once the matter density has diluted to the epoch corresponding to the best-fit z' ≈ 5000. This calculation confirms that the transition can occur prior to recombination while leaving the late-time cosmology unaffected. revision: yes

  2. Referee: [Section deriving the effective potential] The integration of the measure degrees of freedom is stated to produce an effective potential with three flat regions, yet the manuscript supplies no detailed derivation or explicit functional form of this potential (including its dependence on particle density). This omission prevents verification of the flatness conditions and the spontaneous symmetry-breaking step that underpins the entire scenario.

    Authors: We agree that a more explicit derivation improves verifiability. In the revised manuscript we have expanded the relevant section to include the full step-by-step integration of the measure degrees of freedom. This yields the spontaneous breaking of scale symmetry and produces the explicit functional form of the effective potential in the Einstein frame, V_eff(φ, χ, ρ_m), with its dependence on the matter density. We explicitly demonstrate the emergence of the three flat regions (inflation, EDE, LDE) and verify the flatness conditions that follow from the symmetry-breaking mechanism. revision: yes

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper derives an effective density-dependent potential by integrating out independent measure degrees of freedom from a scale-invariant action, yielding three flat regions and a dilution-triggered tunneling transition as a direct consequence of the spontaneous scale-symmetry breaking. This construction is presented as following from the equations of motion and the form of the measure; the subsequent Bayesian fit to CMB/BAO/H0 data then determines numerical values for the early-dark-energy fraction and transition redshift. Because the central mechanism (flat regions and tunneling threshold) is obtained from the action prior to any data fitting, and the fit is used only to extract parameter values rather than to define the functional form itself, the derivation chain remains self-contained and does not reduce any claimed result to its own inputs by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 1 invented entities

The central claim rests on spontaneous scale-symmetry breaking via integration of the measure and on the existence of three flat regions in the resulting density-dependent potential; one fitted parameter (early dark energy fraction) is extracted from data rather than derived.

free parameters (1)
  • f_NEDE = 0.3
    Early dark energy fraction at z'=5000 obtained from Bayesian fit to reduced CMB, BAO, and H0 data.
axioms (2)
  • domain assumption The gravity theory is scale-invariant and contains two scalar fields plus dust particles and a metric-independent measure.
    Invoked in the opening description of the model setup.
  • domain assumption Integration of the measure degrees of freedom spontaneously breaks scale symmetry and produces an effective potential dependent on particle density.
    Central step that generates the three-flat-region potential.
invented entities (1)
  • Diluting matter potential no independent evidence
    purpose: To create flat regions for early and late dark energy and to trigger tunneling as density drops.
    New effective potential introduced after symmetry breaking; no independent falsifiable signature outside the fit is provided.

pith-pipeline@v0.9.0 · 5765 in / 1706 out tokens · 61818 ms · 2026-05-21T23:52:40.973167+00:00 · methodology

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Forward citations

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Reference graph

Works this paper leans on

77 extracted references · 77 canonical work pages · cited by 2 Pith papers · 41 internal anchors

  1. [1]

    Connecting Early Dark Energy to Late Dark Energy by the Diluting Matter Potential

    and modifications to the cosmic expansion history [15]. For a general review of the solutions of the H0 problem, see [16, 17]. ∗ guendel@bgu.ac.il † ramon.herrera@pucv.cl ‡ plabrana@ubiobio.cl arXiv:2507.17095v1 [gr-qc] 23 Jul 2025 2 In this work, we investigate a potential mechanism to alleviate the Hubble tension within the framework of New Early Dark E...

  2. [2]

    Other ideas based on the so called α attractors [26], which uses non canonical kinetic terms have been studied

    and for extensive list of references to earlier work on the topic, see Ref.[25]. Other ideas based on the so called α attractors [26], which uses non canonical kinetic terms have been studied. Also, a quintessential inflation based on a Lorentzian slow-roll ansatz which automatically gives two flat regions was studied in Ref. [27]. In previous papers [28]...

  3. [3]

    So the energy density associated to the matter ρm depends only on ϕ1 and the scale factor, as it should be because ϕ2 transforms under a scale transformation, while ϕ1 does not

    Thus, when inserting back into the expression for F −2 we can see that the dependence of ϕ2 cancels out. So the energy density associated to the matter ρm depends only on ϕ1 and the scale factor, as it should be because ϕ2 transforms under a scale transformation, while ϕ1 does not. In this way, the final result for the function F as a function of the new ...

  4. [4]

    The divergent point is given by, see Eq

    = 0. The divergent point is given by, see Eq. (50) ϕ0 1 = log − f1 g1 p α2 1 + α2 2 . (53) Thus, the divergent barrier at ϕ1 = ϕ0 1 separates the false vacuum from the true vacuum. Initially, the field ϕ1 is in the false vacuum and then, through a tunneling effect, transitions to the true vacuum. We can note from Eq. (49), that VT (ϕ1, ¯a) depends on cosm...

  5. [5]

    The Early Universe

    E.W. Kolb and M.S. Turner, “The Early Universe”, Addison Wesley (1990); A. Linde, “Particle Physics and Inflationary Cosmology”, Harwood, Chur, Switzerland (1990); A. Guth, “The Inflationary Universe”, Vintage, Random House (1998); S. Dodelson, “Modern Cosmology”, Acad. Press (2003); S. Weinberg, “Cosmology”, Oxford Univ. Press (2008)

  6. [6]

    Physical Foundations of Cosmology

    V. Mukhanov, “Physical Foundations of Cosmology”, Cambride Univ. Press (2005)

  7. [7]

    The Galactic Halo

    M.S. Turner, in Third Stromle Symposium “The Galactic Halo” , ASP Conference Series Vol. 666, B.K. Gibson, T.S. Axelrod and M.E. Putman (eds.), (1999); N. Bahcall, J.P. Ostriker, S.J. Perlmutter and P.J. Steinhardt, Science 284, (1999) 1481; for a review, see P.J.E. Peebles and B. Ratra, Rev. Mod. Phys. 75, (2003) 559

  8. [8]

    Riess, et al., Astronomical Journal 116 (1998) 1009-1038; S

    A. Riess, et al., Astronomical Journal 116 (1998) 1009-1038; S. Perlmutter et al., Astrophysical Journal 517 (1999) 565-586

  9. [9]

    A New Cosmological Paradigm: the Cosmological Constant and Dark Matter

    A New cosmological paradigm: The Cosmological constant and dark matter Lawrence M. Krauss, AIP Conf.Proc. 444 (1998) 1, 59-69 • Contribution to: SILAFAE 98, 59-69, 5th International WEIN Symposium: A Conference on Physics Beyond the Standard Model (WEIN 98), Tropical Workshop on Particle Physics and Cosmology, PASCOS 1998 • e-Print: hep-ph/9807376 [hep-ph...

  10. [10]

    Jose Luis Bernal, Licia Verde, Adam G. Riess, JCAP10 (2016)019 DOI: 10.1088/1475-7516/2016/10/019, arXiv:1607.05617 [astro-ph.CO]; Jos´ e Luis Bernal, Licia Verde, Raul Jimenez, Marc Kamionkowski, David Valcin et al., Phys.Rev.D 103 (2021) 10, 103533 • e-Print: 2102.05066 [astro-ph.CO]; Leila L. Graef, Micol Benetti, Jailson S. Alcaniz, Phys.Rev.D 99 (201...

  11. [11]

    R. E. Keeley, S. Joudaki, M. Kaplinghat and D. Kirkby, JCAP 12 (2019), 035; K. L. Pandey, T. Karwal and S. Das, JCAP 07 (2020), 026; A. Quelle and A. L. Maroto, Eur. Phys. J. C 80 (2020) no.5, 369; A. Bhattacharyya, U. Alam, K. L. Pandey, S. Das, and S. Pal, Astrophys. J. 876, 143 (2019), arXiv:1805.04716 [astro-ph.CO]; G. Lambiase, S. Mohanty, A. Narang,...

  12. [12]

    see review in M Cortˆ es et. al. Interpreting DESI’s evidence for evolving dark energy, arXiv:2404.08056 (astro-ph)

  13. [13]

    Early Dark Energy Can Resolve The Hubble Tension

    Vivian Poulin, Tristan L. Smith, Tanvi Karwal, Marc Kamionkowski Phys.Rev.Lett. 122 (2019) 22, 221301, Early Dark Energy Can Resolve The Hubble Tension Published: Jun 5, 2019 e-Print: 1811.04083 [astro-ph.CO]

  14. [14]

    Niedermann and M

    F. Niedermann and M. S. Sloth, Phys. Rev. D 102 (2020) no.6, 063527 doi:10.1103/PhysRevD.102.063527 [arXiv:2006.06686 [astro-ph.CO]]

  15. [15]

    Planck 2018 results. VI. Cosmological parameters

    N. Aghanim et al. [Planck], Astron. Astrophys. 641 (2020), A6 [erratum: Astron. Astrophys. 652 (2021), C4] doi:10.1051/0004-6361/201833910 [arXiv:1807.06209 [astro-ph.CO]]

  16. [16]

    A. G. Riess, W. Yuan, L. M. Macri, D. Scolnic, D. Brout, S. Casertano, D. O. Jones, Y. Murakami, L. Breuval and T. G. Brink, et al. Astrophys. J. Lett. 934 (2022) no.1, L7 doi:10.3847/2041-8213/ac5c5b [arXiv:2112.04510 [astro-ph.CO]]. 23

  17. [17]

    A. G. Riess, G. S. Anand, W. Yuan, S. Casertano, A. Dolphin, L. M. Macri, L. Breuval, D. Scolnic, M. Perrin and R. I. Anderson, Astrophys. J. Lett. 956 (2023) no.1, L18 doi:10.3847/2041-8213/acf769 [arXiv:2307.15806 [astro-ph.CO]]

  18. [18]

    Poulin, T

    V. Poulin, T. L. Smith and T. Karwal, Phys. Dark Univ. 42 (2023), 101348 doi:10.1016/j.dark.2023.101348 [arXiv:2302.09032 [astro-ph.CO]]

  19. [19]

    A. R. Khalife, M. B. Zanjani, S. Galli, S. G¨ unther, J. Lesgourgues and K. Benabed, JCAP04 (2024), 059 doi:10.1088/1475- 7516/2024/04/059 [arXiv:2312.09814 [astro-ph.CO]]

  20. [20]

    In the Realm of the Hubble tension $-$ a Review of Solutions

    Eleonora Di Valentino, Olga Mena, Supriya Pan, Luca Visinelli, Weiqiang Yang, Alessandro Melchiorri, David F. Mota, Adam G. Riess, Joseph Silk, In the Realm of the Hubble tension a Review of Solutions , astro-ph arXiv:2103.01183

  21. [21]

    The CosmoVerse White Paper: Addressing observational tensions in cosmology with systematics and fundamental physics

    Eleonora Di Valentino, Jackson Levi Said Jackson , Adam RiessShow et. al., The CosmoVerse White Paper: Addressing observational tensions in cosmology with systematics and fundamental physics April 2025 DOI: 10.48550/ arXiv.2504.01669

  22. [22]

    Niedermann and M

    F. Niedermann and M. S. Sloth, Phys. Rev. D 103 (2021) no.4, L041303 doi:10.1103/PhysRevD.103.L041303 [arXiv:1910.10739 [astro-ph.CO]]

  23. [23]

    Linde, Phys

    A. Linde, Phys. Lett. 108B (1982) 389-393; A. Albrecht and P. Steinhardt, Phys. Rev. Lett. 48 (1982) 1220-1223

  24. [24]

    COBE, Gravitational Waves, Inflation and Extended Inflation

    A.R. Liddle and D.H. Lyth, Phys. Lett. 291B (1992) 391-398 ( arxiv:astro-ph/9208007); A.R. Liddle and D.H. Lyth, Phys. Reports 231 (1993) 1-105 ( arxiv:astro-ph/9303019)

  25. [25]

    Peebles and A.Vilenkin, Phys

    P.J.E. Peebles and A.Vilenkin, Phys. Rev. D59 (1999) 063505

  26. [26]

    Modified gravity with negative and positive powers of the curvature: unification of the inflation and of the cosmic acceleration

    S. Nojiri and S. Odintsov, Phys. Rev. D68 (2003) 123512 ( arxiv:hep-th/0307288); G. Cognola, E. Elizalde, S. Nojiri, S.D. Odintsov, L. Sebastiani and S. Zerbini, Phys. Rev. D77 (2008) 046009 ( 0712.4017 [hep-th]), and references therein; S.A. Appleby, R.A. Battye and A.A. Starobinsky, JCAP 1006 (2010) 005 ( arxiv:0909.1737 [astro-ph])

  27. [27]

    The unification of inflation and late-time acceleration in the frame of $k$-essence

    R. Saitou and S. Nojiri, Eur. Phys. J. C71 (2011) 1712 ( arxiv:1104.0558 [hep-th])

  28. [28]

    Variable gravity Universe

    C. Wetterich, Phys. Rev. D89 (2014) 024005 ( arxiv:1308.1019 [astro-ph])

  29. [29]

    Variable gravity: A suitable framework for quintessential inflation

    Md. Wali Hossain, R. Myrzakulov, M. Sami and E.N. Saridakis, Phys. Rev. D90 (2014) 023512 ( arxiv:1402.6661 [gr-qc])

  30. [30]

    Quintessential Inflation with $\alpha$-attractors

    Konstantinos Dimopoulos, Charlotte Owen, JCAP 06 (2017) 027 • e-Print: 1703.00305 [gr-qc]; Konstantinos Dimopoulos, Leonora Donaldson Wood, Charlotte, Phys.Rev.D 97 (2018) 6, 063525 • e-Print: 1712.01760 [astro-ph.CO];R. Herrera, Eur. Phys. J. C 78, no.3, 245 (2018); R. Herrera, Phys. Rev. D 98, no.2, 023542 (2018);R. Herrera, Phys. Rev. D 99, no.10, 1035...

  31. [31]

    David Benisty, Eduardo I. Guendelman, Eur.Phys.J.C 80 (2020) 6, 577 • e-Print: 2006.04129 [astro-ph.CO]; Lorentzian Quintessential Inflation, awarded 2nd prize in the 2020 Gravity Research Foundation Essays Competition, David Benisty, Eduardo I. Guendelman, Int.J.Mod.Phys.D 29 (2020) 14, 2042002 • e-Print: 2004.00339 [astro-ph.CO]

  32. [32]

    Emergent Cosmology, Inflation and Dark Energy

    Eduardo Guendelman, Ram´ on Herrera, Pedro Labrana, Emil Nissimov, Svetlana Pacheva, Gen.Rel.Grav.47 (2015) 2, 10 • e-Print: 1408.5344 [gr-qc]; Eduardo I. Guendelman, Ramon Herrera, Gen.Rel.Grav. 48 (2016) 1, 3 • e-Print: 1511.08645 [gr-qc]

  33. [33]

    Unification of Inflation and Dark Energy from Spontaneous Breaking of Scale Invariance

    E. Guendelman, E. Nissimov and S. Pacheva, arxiv:1407.6281 [hep-th]

  34. [34]

    Scale invariance, new inflation and decaying Lambda terms

    E.I. Guendelman, Mod. Phys. Lett. A14 (1999) 1043-1052 ( arxiv:gr-qc/9901017); E.I. Guendelman, in “Energy Densities in the Universe”, Proc. Rencontres de Moriond, Les Arcs (2000) ( arxiv:gr- qc/0004011)

  35. [35]

    Dynamical measure and field theory models free of the cosmological constant problem

    E.I. Guendelman and A. Kaganovich, Phys. Rev. D60 (1999) 065004 ( arxiv:gr-qc/9905029)

  36. [36]

    Inflation and Transition to a Slowly Accelerating Phase from S.S.B. of Scale Invariance

    E.I. Guendelman and O. Katz, Class. Quantum Grav. 20 (2003) 1715-1728 ( arxiv:gr-qc/0211095)

  37. [37]

    Emerging Universe from Scale Invariance

    S. del Campo. E. Guendelman, R. Herrera and P. Labrana, JCAP 1006 (2010) 026 ( arxiv:1006.5734 [astro-ph.CO])

  38. [38]

    Emergent Universe from Scale Invariant Two Measures Theory

    S. del Campo. E. Guendelman, A. Kaganovich, R. Herrera and P. Labrana, Phys. Lett. 699B (2011) 211 ( arxiv:1105.0651 [astro-ph.CO])

  39. [39]

    Connecting The Non-Singular Origin of the Universe, The Vacuum Structure and The Cosmological Constant Problem

    E.I. Guendelman and P. Labrana, Int. J. Mod. Phys. D22 (2013) 1330018 ( arxiv:1303.7267 [astro-ph.CO])

  40. [40]

    A two measure model of dark energy and dark matter

    E.I. Guendelman, D. Singleton and N. Yongram, JCAP 1211 (2012) 044 ( arxiv:1205.1056 [gr-qc]); E.I. Guendelman, H. Nishino and S. Rajpoot, Phys. Lett. 732B (2014) 156 ( arxiv:1403.4199 [hep-th])

  41. [41]

    Strings and branes with a modified measure

    E.I. Guendelman, Class.Quant.Grav. 17 (2000) 3673-3680 • e-Print: hep-th/0005041 [hep-th]; E.I. Guendelman, Phys.Rev.D 63 (2001) 046006 • e-Print: hep-th/0006079 [hep-th], E. Guendelman, A. Kaganovich, E. Nissimov and S. Pacheva, Phys. Rev. D66 (2002) 046003 ( arxiv:hep-th/0203024)

  42. [42]

    E. I. Guendelman, International Journal of Modern Physics, Implications of the spectrum of dynamically generated string tension theories https://doi.org/10.1142/S0218271821420281, e-Print: 2110.09199 [hep-th]

  43. [43]

    Eduardo Guendelman, Eur.Phys.J.C 81 (2021) 10, 886 • e-Print: 2107.08005 [hep-th]

  44. [44]

    Metric-Independent Measures for Supersymmetric Extended Object Theories on Curved Backgrounds

    H. Nishino and S. Rajpoot, Phys. Lett. 736B (2014) 350-355 ( arxiv:1411.3805 [hep-th])

  45. [45]

    Guendelman

    E.I. Guendelman. Dynamical string tension theories with target space scale invariance SSB and restoration, Eur. Phys. J. C (2025) 85: 276 https://doi.org/10.1140/epjc/s10052-025-13966-9

  46. [46]

    Isocurvature Perturbations in Multiple Inflationary Models

    David Polarski, Alexei A. Starobinsky, Phys.Rev.D 50 (1994) 6123-6129 • e-Print: astro-ph/9404061 [astro-ph]

  47. [47]

    Starobinsky, Nucl.Phys.B 385 (1992) 623-650

    David Polarski, Alexei A. Starobinsky, Nucl.Phys.B 385 (1992) 623-650

  48. [48]

    Langlois and S

    D. Langlois and S. Renaux-Petel, JCAP 0804 (2008) 017

  49. [49]

    David Benisty,, Eduardo I. Guendelman, Emil Nissimov,, Svetlana Pacheva, Nucl.Phys.B 951 (2020) 114907 • e-Print: 1907.07625 [astro-ph.CO]; David Benisty, Eduardo Guendelman, Emil Nissimov, Svetlana Pacheva, Eur.Phys.J.C79 (2019) 9, 806 • e-Print: 1906.06691 [gr-qc]; David Benisty, Eduardo I. Guendelman, Class.Quant.Grav. 36 (2019) 9, 095001 • 24 e-Print:...

  50. [50]

    Guendelman, R

    E. Guendelman, R. Herrera and D. Benisty, Phys. Rev. D 105 (2022) no.12, 124035 doi:10.1103/PhysRevD.105.124035 [arXiv:2201.06470 [gr-qc]]

  51. [51]

    Starobinsky, Phys

    A. Starobinsky, Phys. Lett. 91B (1980) 99-102

  52. [52]

    Adam et al

    R. Adam et al. [Planck], Astron. Astrophys. 586, A133 (2016)

  53. [53]

    Adam et al

    R. Adam et al. (Planck Collaboration), P. A. R. Ade et al. [Planck], Astron. Astrophys. 571, A22 (2014)

  54. [54]

    P. A. R. Ade et al. [BICEP and Keck], Phys. Rev. Lett. 127, no.15, 151301 (2021)

  55. [55]

    Guendelman, Ramon Herrera, Pedro Labrana, Phys.Rev.D 103 (2021) 123515 • e-Print: 2005.14151 [gr-qc] and references there

    Eduardo I. Guendelman, Ramon Herrera, Pedro Labrana, Phys.Rev.D 103 (2021) 123515 • e-Print: 2005.14151 [gr-qc] and references there

  56. [56]

    Absence of the Fifth Force Problem in a Model with Spontaneously Broken Dilatation Symmetry

    E. Guendelman, A. Kaganovich, Annals Phys. 323 (2008) 866-882 • e-Print: 0704.1998 [gr-qc]

  57. [57]

    Gravitational theory without the cosmological constant problem, symmetries of space-filling branes and higher dimensions

    E.I. Guendelman), A.B. Kaganovich, Gravitational theory without the cosmological constant problem, symmetries of space filling branes and higher dimensions, Published in: Phys.Rev.D 56 (1997) 3548-3554 • e-Print: gr-qc/9702058 [gr-qc]

  58. [58]

    Cosmological implications of ultra-light axion-like fields

    V. Poulin, T. L. Smith, D. Grin, T. Karwal and M. Kamionkowski, Phys. Rev. D 98 (2018) no.8, 083525 doi:10.1103/PhysRevD.98.083525 [arXiv:1806.10608 [astro-ph.CO]]

  59. [59]

    Early dark energy, the Hubble-parameter tension, and the string axiverse

    T. Karwal and M. Kamionkowski, Phys. Rev. D 94 (2016) no.10, 103523 doi:10.1103/PhysRevD.94.103523 [arXiv:1608.01309 [astro-ph.CO]]

  60. [60]

    Early Dark Energy Can Resolve The Hubble Tension

    V. Poulin, T. L. Smith, T. Karwal and M. Kamionkowski, Phys. Rev. Lett. 122 (2019) no.22, 221301 doi:10.1103/PhysRevLett.122.221301 [arXiv:1811.04083 [astro-ph.CO]]

  61. [61]

    S. R. Coleman, Phys. Rev. D 15 (1977), 2929-2936 [erratum: Phys. Rev. D 16 (1977), 1248] doi:10.1103/PhysRevD.16.1248

  62. [62]

    A. D. Linde, Nucl. Phys. B 216 (1983), 421 [erratum: Nucl. Phys. B 223 (1983), 544] doi:10.1016/0550-3213(83)90072-X

  63. [63]

    Wright Omega Function: Mathematics, Lambert W Function, Continuous Function, Analytic Function, Differential Equation, Separation or Variables

    L. Surhone, M. Timplendon and S. Marseken, “Wright Omega Function: Mathematics, Lambert W Function, Continuous Function, Analytic Function, Differential Equation, Separation or Variables”, Betascript Publishing (2010)

  64. [64]

    J. D. Barrow and M. S. Turner, Nature 292 (1981), 35-38 doi:10.1038/292035a0

  65. [65]

    Cosmological constant potential: A resolution to the Hubble tension via the cosmological sound horizon,

    N. Khosravi, “Cosmological constant potential: A resolution to the Hubble tension via the cosmological sound horizon,” Phys. Rev. D 110 (2024) no.6, 063507 doi:10.1103/PhysRevD.110.063507 [arXiv:2312.13886 [astro-ph.CO]]

  66. [66]

    Planck priors for dark energy surveys

    P. Mukherjee, M. Kunz, D. Parkinson, and Y. Wang, Phys. Rev. D 78, 083529 (2008), 0803.1616; I. Tutusaus, M. Kunz, and L. Favre (2023), 2311.16862

  67. [67]

    2011, MNRAS, 412, 1473, doi: 10.1111/j.1365-2966.2011.18162.x

    F. Beutler, C. Blake, M. Colless, D. H. Jones, L. Staveley-Smith, L. Campbell, Q. Parker, W. Saunders and F. Watson, “The 6dF Galaxy Survey: Baryon Acoustic Oscillations and the Local Hubble Constant,” Mon. Not. Roy. Astron. Soc. 416 (2011), 3017-3032 doi:10.1111/j.1365-2966.2011.19250.x [arXiv:1106.3366 [astro-ph.CO]]

  68. [68]

    The Clustering of the SDSS DR7 Main Galaxy Sample I: A 4 per cent Distance Measure at z=0.15

    A. J. Ross, L. Samushia, C. Howlett, W. J. Percival, A. Burden and M. Manera, “The clustering of the SDSS DR7 main Galaxy sample – I. A 4 per cent distance measure at z = 0.15,”doi:10.1093/mnras/stv154 [arXiv:1409.3242 [astro-ph.CO]]

  69. [69]

    The clustering of the SDSS-IV extended Baryon Oscillation Spectroscopic Survey DR14 quasar sample: First measurement of Baryon Acoustic Oscillations between redshift 0.8 and 2.2

    M. Ata et al. [eBOSS], “The clustering of the SDSS-IV extended Baryon Oscillation Spectroscopic Survey DR14 quasar sample: first measurement of baryon acoustic oscillations between redshift 0.8 and 2.2,” Mon. Not. Roy. Astron. Soc. 473 (2018) no.4, 4773-4794 doi:10.1093/mnras/stx2630 [arXiv:1705.06373 [astro-ph.CO]]. 422 citations counted in INSPIRE as of...

  70. [70]

    The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Survey: cosmological analysis of the DR12 galaxy sample

    S. Alam et al. [BOSS], “The clustering of galaxies in the completed SDSS-III Baryon Oscillation Spectroscopic Sur- vey: cosmological analysis of the DR12 galaxy sample,” Mon. Not. Roy. Astron. Soc. 470 (2017) no.3, 2617-2652 doi:10.1093/mnras/stx721 [arXiv:1607.03155 [astro-ph.CO]]

  71. [71]

    Baryon acoustic oscillations from the complete SDSS-III Ly$\alpha$-quasar cross-correlation function at $z=2.4$

    H. du Mas des Bourboux et al. [BOSS], “Baryon acoustic oscillations from the complete SDSS-III Ly α-quasar cross- correlation function at z = 2.4,” Astron. Astrophys. 608 (2017), A130 doi:10.1051/0004-6361/201731731 [arXiv:1708.02225 [astro-ph.CO]]

  72. [72]

    M. S. Turner, E. J. Weinberg and L. M. Widrow, Phys. Rev. D 46, 2384-2403 (1992) doi:10.1103/Phys Rev D.46.2384

  73. [73]

    The Price of Shifting the Hubble Constant

    J. Evslin, A. A. Sen and Ruchika, “Price of shifting the Hubble constant,” Phys. Rev. D 97 (2018) no.10, 103511 doi:10.1103/PhysRevD.97.103511 [arXiv:1711.01051 [astro-ph.CO]]

  74. [74]

    Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies

    “Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies,” Astro- phys. J. 633 (2005), 560-574 doi:10.1086/466512 [arXiv:astro-ph/0501171 [astro-ph]]. 4646 citations counted in INSPIRE as of 16 Apr 2025

  75. [75]

    Baryonic Features in the Matter Transfer Function

    D. J. Eisenstein and W. Hu, “Baryonic features in the matter transfer function,” Astrophys. J. 496 (1998), 605 doi:10.1086/305424 [arXiv:astro-ph/9709112 [astro-ph]]

  76. [76]

    Roberto Trotta, Bayes in the sky: Bayesian inference and model selection in cosmology, Contemp.Phys.49:71-104,2008, arXiv:0803.4089 [astro-ph]

  77. [77]

    Emanuel Parzen, Modern Probability Theory and Its Applications ISBN: 978-0-471-57278-7