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arxiv: 2604.03381 · v2 · submitted 2026-04-03 · 🌌 astro-ph.CO

Big Bang Nucleosynthesis Constraints on the CCC+TL Cosmology

Pith reviewed 2026-05-13 18:10 UTC · model grok-4.3

classification 🌌 astro-ph.CO
keywords big bang nucleosynthesisCCC+TL cosmologycovarying coupling constantslight element abundancestired lightneutron lifetimelithium problem
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The pith

CCC+TL cosmology preserves standard Big Bang nucleosynthesis abundances when interaction rates scale with the Hubble rate.

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

The paper examines whether the Covarying Coupling Constants plus Tired Light model conflicts with observed light-element abundances produced in the first minutes after the Big Bang. In this model, dimensionful quantities scale by a universal function f(z) that reaches a plateau value near 3 at BBN redshifts, which slows the expansion rate at fixed temperature and lengthens the time available for reactions. The central result is that abundances stay identical to the standard model once the relevant reaction rates and neutron lifetime are also scaled by the same plateau factor, leaving the controlling ratios unchanged. Numerical integration of the nucleosynthesis network confirms that the two cases agree to parts in a thousand. The authors further show that adopting the lower baryon density favored by late-time CCC+TL fits reduces the lithium discrepancy while increasing the deuterium yield.

Core claim

At BBN redshifts the CCC+TL Hubble rate satisfies H_CTL(T) = f_max^{-1} H_ΛCDM(T) with f_max ≈ 3, increasing the cooling time Δt by the same factor; BBN yields remain identical to ΛCDM provided the interaction rates Γ and neutron lifetime τ_n are rescaled by f_max so that Γ/H and exp(−Δt/τ_n) stay invariant, and direct implementation in the NUC123 network with control parameter fctl = 3 reproduces standard abundances to 10^{-3}–10^{-4} precision.

What carries the argument

The plateau scaling f_max applied uniformly to the Hubble rate, interaction rates Γ, and neutron lifetime τ_n, which leaves the dimensionless combinations Γ/H and exp(−Δt/τ_n) invariant.

If this is right

  • Light-element yields match standard predictions for f_max = 3 to within numerical rounding.
  • BBN does not exclude the CCC+TL model when the scaling assumption holds.
  • Lower baryon density from Pantheon+ fits reduces the ^7Li problem but raises D/H.
  • The tired-light term is negligible at BBN redshifts, so only the covarying-constants part affects early dynamics.

Where Pith is reading between the lines

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

  • The same uniform scaling could be tested against CMB anisotropies or other early-universe observables that depend on the same dimensionless ratios.
  • If the scaling holds for weak rates but not for strong rates, BBN could become a sharp discriminator between CCC+TL variants.
  • Updated nuclear rate libraries could be rerun with fctl = 3 to check whether the 10^{-4} agreement persists at higher precision.

Load-bearing premise

Interaction rates and the neutron lifetime must scale by exactly the same plateau factor as the Hubble rate during BBN.

What would settle it

A BBN calculation in which reaction rates and τ_n are left unscaled while H is reduced by f_max = 3, producing abundance shifts larger than 0.1 percent.

read the original abstract

We investigate whether Big Bang nucleosynthesis (BBN) remains compatible with the Covarying Coupling Constants plus Tired Light (CCC+TL) cosmology. In this framework, only quantities with explicit length dimensionality covary through a universal scaling function $f \left( z \right)$, while dimensionless constants and dimensionless ratios remain invariant. At the redshifts $z$ relevant to BBN, $f \left( z \right )$ approaches a constant plateau $f_{\text{max}} \left( z \right) \simeq 3$, and the tired-light contribution is negligible, so the early-time dynamics reduce to a global rescaling of dimensioned quantities. In particular, the Hubble expansion rate $H$ at fixed temperature $T$ satisfies $H_{\text{CTL}} \left( T \right) = f^{-1}_{\text{max}} H_{\Lambda\text{CDM}}\left( T\right)$, implying a longer cooling time $\Delta t$ between weak freeze-out and the onset of nucleosynthesis by the same factor (CCC+TL labeled as $\textit{CTL}$). We find that BBN predictions are preserved provided the relevant interaction rates $\Gamma$ and decay rates governing the neutron lifetime ${\tau}_n$ share the same plateau scaling as $H$, so that governing combinations such as $\Gamma\text{/}H$ and $\text{exp} \left( -\Delta t \text{/} {\tau}_n \right)$ remain invariant. Implementing these plateau rescalings in the Kawano/NUC123 network (via a single control parameter $\texttt{fctl} \equiv f_{\text{max}}$) yields identical light-element abundances for $\texttt{fctl}= 1$ ($\Lambda$CDM) and $\texttt{fctl} = 3\left( \text{CCC+TL} \right)$ to within $10^{-3} - 10^{-4}$ level, consistent with numerical rounding. We also illustrate that adopting the lower late-time CCC+TL baryon density from the Pantheon+ data fit can reduce the ${}^7\text{Li}$ discrepancy but simultaneously increases D/H, implying that BBN alone does not select between the late-time baryon-density inferences considered here.

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

1 major / 2 minor

Summary. The manuscript examines whether Big Bang nucleosynthesis (BBN) remains compatible with the Covarying Coupling Constants plus Tired Light (CCC+TL) cosmology. At BBN redshifts the model reduces to a global rescaling of dimensionful quantities by a plateau value f_max ≃ 3, yielding H_CTL(T) = f_max^{-1} H_ΛCDM(T) and a correspondingly longer cooling interval Δt. The central result is that light-element yields are unchanged provided interaction rates Γ and the neutron lifetime τ_n are rescaled by the identical factor, preserving the dimensionless combinations Γ/H and exp(−Δt/τ_n). Implementation of this rescaling via a single control parameter fctl in a modified Kawano/NUC123 network produces abundances identical to the standard case to within 10^{-3}–10^{-4}. The paper also shows that adopting the lower late-time baryon density inferred from Pantheon+ data reduces the ^7Li discrepancy while increasing D/H.

Significance. If the shared plateau-scaling assumption holds, the work demonstrates that CCC+TL cosmology is fully consistent with standard BBN predictions and therefore receives no additional constraint from light-element abundances. The numerical verification in the modified NUC123 network is a clear strength, confirming invariance to high precision. The secondary exploration of baryon-density effects on the lithium and deuterium abundances provides a concrete illustration of how late-time inferences can be tested against BBN data within the same framework.

major comments (1)
  1. [Abstract and §4 (numerical implementation)] The invariance of BBN yields follows directly once Γ and τ_n are required to share the same f_max scaling as H; the numerical run therefore functions primarily as a consistency check of the imposed rescaling rather than an independent test of the underlying CCC+TL dynamics. This conditional character of the result should be stated more explicitly in the abstract and conclusion.
minor comments (2)
  1. [§3] The definition of the control parameter fctl ≡ f_max is introduced late; moving its explicit definition to the first paragraph of §3 would improve readability.
  2. [Results section] Table 1 (or equivalent abundance table) would benefit from an additional column listing the absolute difference between the fctl=1 and fctl=3 runs to make the 10^{-3}–10^{-4} agreement immediately visible.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading, positive assessment, and recommendation to accept the manuscript. We address the single major comment below.

read point-by-point responses
  1. Referee: [Abstract and §4 (numerical implementation)] The invariance of BBN yields follows directly once Γ and τ_n are required to share the same f_max scaling as H; the numerical run therefore functions primarily as a consistency check of the imposed rescaling rather than an independent test of the underlying CCC+TL dynamics. This conditional character of the result should be stated more explicitly in the abstract and conclusion.

    Authors: We agree that the invariance of the light-element yields follows directly from the shared f_max scaling of Γ, τ_n, and H under the plateau assumption of the CCC+TL model at BBN redshifts. The numerical implementation in the modified Kawano/NUC123 network serves to confirm that this rescaling is applied consistently and yields abundances identical to the standard case within numerical precision. We will revise both the abstract and the conclusion to state this conditional character more explicitly, clarifying that the result holds provided the relevant rates share the same plateau scaling as the expansion rate. revision: yes

Circularity Check

1 steps flagged

BBN invariance follows by construction once rates are assumed to share f_max scaling with H

specific steps
  1. self definitional [Abstract]
    "We find that BBN predictions are preserved provided the relevant interaction rates Γ and decay rates governing the neutron lifetime τn share the same plateau scaling as H, so that governing combinations such as Γ/H and exp(−Δt/τn) remain invariant."

    The invariance of Γ/H and exp(−Δt/τn) is true by direct algebraic substitution once Γ and τn are posited to scale with exactly the same f_max that rescales H and Δt. The subsequent statement that abundances are preserved, and the numerical confirmation to 10^{-3}–10^{-4}, therefore follows tautologically from the shared-scaling premise rather than from any additional dynamical content.

full rationale

The paper conditions its central claim on the assumption that Γ and τn scale identically with the same f_max as H (and thus Δt). Under that assumption the dimensionless ratios Γ/H and Δt/τn are algebraically invariant, so the numerical NUC123 run with fctl=3 simply reproduces the same abundances by implementing the assumption. No independent first-principles derivation of the shared scaling is supplied; the result is therefore equivalent to the input assumption rather than a test of the cosmology.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the single assumption that rates covary identically with the Hubble rate; no new entities are introduced and the only free parameter is the plateau value taken from the model definition.

free parameters (1)
  • fctl = 3
    Plateau value f_max at BBN redshifts, set to 3 from the CCC+TL model definition and late-time fits.
axioms (1)
  • domain assumption Interaction rates Γ and neutron lifetime τn scale with the same plateau factor f_max as the Hubble rate H
    Invoked to keep the ratios Γ/H and Δt/τn invariant so that abundances are unchanged.

pith-pipeline@v0.9.0 · 5719 in / 1359 out tokens · 40747 ms · 2026-05-13T18:10:05.905297+00:00 · methodology

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Works this paper leans on

112 extracted references · 112 canonical work pages

  1. [1]

    Gamow, G.Expanding Universe and the Origin of Elements, Physical Review70(1946) pg. 572-573

  2. [2]

    A.A Neutron-Capture Theory of the Formation and Relative Abundance of the Elements.Physical Review74(1948) pg

    Alpher, R. A.A Neutron-Capture Theory of the Formation and Relative Abundance of the Elements.Physical Review74(1948) pg. 1577-1589

  3. [3]

    A., Bethe, H., and Gamow, G.The Origin of Chemical Elements.Physical Review73(1948) pg

    Alpher, R. A., Bethe, H., and Gamow, G.The Origin of Chemical Elements.Physical Review73(1948) pg. 803-804 16 Rajendra P. Gupta, Nikolaos Samaras

  4. [4]

    Physical Review74(1948) pg

    Alpher, Ralph A., and Herman, Robert C.On the Relative Abundance of the Elements. Physical Review74(1948) pg. 1737-1742

  5. [5]

    Margaret, Burbidge, G

    Burbidge, E. Margaret, Burbidge, G. R., Fowler, William A., and Hoyle, F.Synthesis of the Elements in Stars.Rev. Mod. Phys.29(1957) pg. 547-650

  6. [6]

    Cameron, A.G.W.Nuclear Reactions in Stars and NucleogenesisNuclear Reactions in Stars and Nucleogenesis (1957) pg. 201

  7. [7]

    IIApJ146 (1966) pg

    Peebles, P.J.E.Primordial Helium Abundance and the Primordial Fireball. IIApJ146 (1966) pg. 542

  8. [8]

    Wagoner, Robert V., Fowler, William A., and Hoyle, F.On the Synthesis of Elements at Very High Temperatures,ApJ148(1967) pg. 3

  9. [9]

    Weinberg, StevenGravitation and Cosmology: Principles and Applications of the General Theory of Relativity(1972)

  10. [10]

    Steigman, Gary, and Schramm, David N., and Gunn, James E.Cosmological limits to the number of massive leptons.Physics Letters B66(1977) pg. 202-204

  11. [11]

    Shvartsman, D.Reviews and bibliography.Soil Mechanics and Foundation Engineering6 (1969) pg. 144-145

  12. [12]

    Yang, J., Turner, M.S., Steigman, G., Schramm, D.N., and Olive, K.A.Primordial nucle- osynthesis: a critical comparison of theory and observation.ApJ281(1984) pg. 492-511

  13. [13]

    1493-1609

    Sarkar, SubirBig bang nucleosynthesis and physics beyond the standard model.Reports on Progress in Physics59(1996) pg. 1493-1609

  14. [14]

    Walker, Terry P., Steigman, Gary, Schramm, David N., Olive, Keith A., and Kang, Ho- Shik.Primordial Nucleosynthesis ReduxApJ376(1991) pg. 51

  15. [15]

    Olive, K.A., Steigman, G., and Walker, T.P.Primordial nucleosynthesis: theory and ob- servations.Physics Reports333(2000) pg. 389-407

  16. [16]

    Burles, Scott, Nollett, Kenneth M., and Turner, Michael S.Big Bang Nucleosynthesis Predictions for Precision CosmologyApJ Letters552(2001) pg. L1-L5

  17. [17]

    et al.,A compilation of charged-particle induced thermonuclear reaction rates

    Angulo, C. et al.,A compilation of charged-particle induced thermonuclear reaction rates. Nucl. Phys. A656(1999) pg. 3-183

  18. [18]

    Descouvemont, P., Adahchour, A., Angulo, C., Coc, A., and Vangioni-Flam, E.Compila- tion and R-matrix analysis of Big Bang nuclear reaction rates.Atomic Data and Nuclear Data Tables88(2004) pg. 203-236

  19. [19]

    H.Primordial nucleosynthesis for the new cosmology: Determining uncertain- ties and examining concordance.Physics Review D.70(2004) pg

    Cyburt, R. H.Primordial nucleosynthesis for the new cosmology: Determining uncertain- ties and examining concordance.Physics Review D.70(2004) pg. 2

  20. [20]

    Adelberger, E.G., et al.Solar fusion cross sections. II. The pp chain and CNO cycles Reviews of Modern Physics83(2011) pg. 195-196

  21. [21]

    Dicus, D.A., Letaw, J.R., Teplitz, D.C., and Teplitz, V.L.Effects of proton decay on the cosmological future252(1982) pg. 1-9

  22. [22]

    D.Relic neutrino decoupling including flavour oscillations.Nuclear Physics B729(2005) pg

    Mangano, G., Miele, G., Pastor, S., Pinto, T., Pisanti, O., and Serpico, P. D.Relic neutrino decoupling including flavour oscillations.Nuclear Physics B729(2005) pg. 221-234

  23. [23]

    Primordial nucleosynthesis the computer way(1992)

    Kawano, Lawrence.Let’s go: Early universe 2. Primordial nucleosynthesis the computer way(1992)

  24. [24]

    Smith, Michael S., Kawano, Lawrence H., and Malaney, Robert A.Experimental, Compu- tational, and Observational Analysis of Primordial Nucleosynthesis.ApJS85(1993) pg. 219

  25. [25]

    PArthENoPE: Public algorithm evaluating the nucleosynthesis of primordial elements

    Pisanti, O., Cirillo, A., Esposito, S., Iocco, F., Mangano, G., Miele, G., and Serpico, P.D. PArthENoPE: Public algorithm evaluating the nucleosynthesis of primordial elements. Computer Physics Communications178(2008) pg. 12

  26. [26]

    1822-1831

    Arbey, A.AlterBBN: A program for calculating the BBN abundances of the elements in alternative cosmologies.Computer Physics Communications183(2012) pg. 1822-1831

  27. [27]

    Burles, Scott, and Tytler, Davidhe Deuterium Abundance toward QSO 1009+2956.ApJ 507(1998) pg. 732-744

  28. [28]

    O’Meara, John M., Tytler, David, Kirkman, David, Suzuki, Nao, Prochaska, Jason X., Lubin, Dan, and Wolfe, Arthur M.The Deuterium to Hydrogen Abundance Ratio toward a Fourth QSO: HS 0105+1619ApJ552(2001) pg. 718-730

  29. [29]

    2477-2486

    Pettini, Max, and Cooke, Ryan.A new, precise measurement of the primordial abundance of deuterium.MNRAS425(2012) pg. 2477-2486

  30. [30]

    Cooke, Ryan.Primordial deuterium at the per cent level.APS April Meeting Abstracts 2014(2014) pg. R11.001

  31. [31]

    1-27 Testing the CCC+TL Cosmology with Big Bang Nucleosynthesis 17

    Bennett, C.L., et al.First-Year Wilkinson Microwave Anisotropy Probe (WMAP) Obser- vations: Preliminary Maps and Basic Results.ApJS148(2003) pg. 1-27 Testing the CCC+TL Cosmology with Big Bang Nucleosynthesis 17

  32. [32]

    Planck CollaborationPlanck 2018 results. VI. Cosmological parameters.Astronomy and Astrophysics641(2020) pg. A6

  33. [33]

    Steigman, Gary.Primordial Nucleosynthesis in the Precision Cosmology Era.Annual Re- view of Nuclear and Particle Science57(2007) pg. 463-491

  34. [34]

    Fields, Brian D.The Primordial Lithium Problem.Annual Review of Nuclear and Particle Science61(2011) pg. 47-68

  35. [35]

    H.et al.Dependence of X-Ray Burst Models on Nuclear Reaction RatesApJ 830(2016) pg

    Cyburt, R. H.et al.Dependence of X-Ray Burst Models on Nuclear Reaction RatesApJ 830(2016) pg. 55

  36. [36]

    Pitrou, Cyril, Coc, Alain, Uzan, Jean-Philippe, and Vangioni, Elisabeth.Precision big bang nucleosynthesis with improved Helium-4 predictions.Physical Reports754(2018) pg. 1-66

  37. [37]

    Izotov, Yuri I., and Thuan, Trinh X.The Primordial Abundance of 4He: Evidence for Non-Standard Big Bang Nucleosynthesis.ApJL710(2010) pg. L67-L71

  38. [38]

    Aver, Erik, and Olive, Keith A., and Skillman, Evan D.The effects of He Iλ10830 on helium abundance determinations.JCAP2015(2015) pg. 011

  39. [39]

    Izotov, Y.I., Thuan, T.X., and Guseva, N.G.A new determination of the primordial He abundance using the He Iλ10830˚A emission line: cosmological implicationsMNRAS445 (2014) pg. 778-793

  40. [40]

    Spite, F., and Spite, M.Abundance of lithium in unevolved stars and old disk stars: Interpretation and consequences.Astronomy and Astrophysics115(1982) pg. 357-366

  41. [41]

    Ryan, Sean G.G., et al.Primordial Lithium and Big Bang Nucleosynthesis.ApJ530 (2000) pg. L57

  42. [42]

    Asplund, Martin, et al.Lithium Isotopic Abundances in Metal-poor Halo StarsApJ644 (2006) pg. 229

  43. [43]

    et al.The metal-poor end of the Spite plateau

    Sbordone, L. et al.The metal-poor end of the Spite plateau. I. Stellar parameters, metal- licities, and lithium abundances.Astronomy and Astronomy522(2010) pg. A26

  44. [44]

    Wagoner, Robert V.Physics of Massive Objects.Annual Review of Astronomy and As- trophysics7(1969) pg. 553

  45. [45]

    Coc, Alain, and Vangioni, Elisabeth.Primordial nucleosynthesis.International Journal of Modern Physics E26(2017) pg. 1741002

  46. [46]

    Fields, Brian D., et al.Big-Bang Nucleosynthesis after Planck.JCAP2020(2020) pg. 010

  47. [47]

    Dirac, P.A.M.The Cosmological Constants.Nature139(1937) pg. 323

  48. [48]

    Canuto, V., and Lodenquai, J.Dirac cosmology.ApJ211(1977) pg. 342-356

  49. [49]

    1447-1455

    Maeder, Andre.MOND as a peculiar case of the SIV theory.MNRAS520(2023) pg. 1447-1455

  50. [50]

    Maeder, Andre.Scale-invariant Cosmology and CMB Temperatures as a Function of Red- shifts.ApJ847(2017) pg. 65

  51. [51]

    Maeder, Andre.Evolution of the early Universe in the scale invariant theory arXiv:1902.10115 (2019)

  52. [52]

    Physical Reviews124(1961) pg

    Brans, C., and Dicke, R.H.Mach’s Principle and a Relativistic Theory of Gravitation. Physical Reviews124(1961) pg. 925-935

  53. [53]

    Weyl, Hermann.Gravitation und Elektrizit¨ atSitzungsberichte der K¨ oniglich Preussischen Akademie der Wissenschaften (1918) pg. 465-478

  54. [54]

    Canuto, V., Hsieh, S.H., and Adams, P.J.Scale-Covariant Theory of Gravitation and Astrophysical Applications.Physical Review Letters39(1977) pg. 429-432

  55. [55]

    Classical and Quantum Gravity29(2012) pg

    Romero, C., Fonseca-Neto, J.B., and Pucheu, M.LGeneral relativity and Weyl geometry. Classical and Quantum Gravity29(2012) pg. 155015

  56. [56]

    Cuzinatto, Rodrigo R., Gupta, Rajendra P., and Pompeia, Pedro J.Dynamical Analysis of the Covarying Coupling Constants in Scalar-Tensor GravitySymmetry15(2023) pg. 709

  57. [57]

    Gilbert, C.The gravitational field of a star in the expanding universe.MNRAS116(1956) pg. 6781956

  58. [58]

    Gilbert, C.Dirac’s Cosmology.Nature192(1961) pg. 57

  59. [59]

    Rev.73(1948) pg

    Teller, Edward.On the Change of Physical ConstantsPhys. Rev.73(1948) pg. 801-802

  60. [60]

    Chin, Chao-wen, and Stothers, Richard.Limit on the Secular Change of the Gravitational Constant Based on Studies of Solar Evolution.Phys. Rev. Lett.36(1976)

  61. [61]

    1442018-152

    Sahni, Varun, and Shtanov, Yuri.Can a variable gravitational constant resolve the faint young Sun paradox?International Journal of Modern Physics D23(2014) pg. 1442018-152

  62. [62]

    519-520 18 Rajendra P

    Morrison, L.V.Rotation of the Earth from AD 1663-1972 and the Constancy of GNature 241(1973) pg. 519-520 18 Rajendra P. Gupta, Nikolaos Samaras

  63. [63]

    Sisterna, P., and Vucetich, H.Time variation of fundamental constants: Bounds from geophysical and astronomical data.Phys. Rev. D41(1990) pg. 1034-1046

  64. [64]

    C´ orsico, Leandro G

    Alejandro H. C´ orsico, Leandro G. Althaus, Enrique Garc´ ıa-Berro, and Alejandra D. Romero.An independent constraint on the secular rate of variation of the gravitational constant from pulsating white dwarfs.Journal of Cosmology and Astroparticle Physics 2013(2013) pg. 032

  65. [65]

    degl’Innocenti, S., Fiorentini, G., Raffelt, G.G., Ricci, B., and Weiss, A.Time-variation of Newton’s constant and the age of globular clusters.Astronomy and Astrophysics312 (1996) pg. 345-352

  66. [66]

    G., Althaus, L

    Benvenuto, O. G., Althaus, L. G. and Torres, Diego F.Evolution of white dwarfs as a probe of theories of gravitation: the case of Brans—DickeMNRAS305(1999) pg. 905-919

  67. [67]

    1432-1435

    Thorsett, S.E.The Gravitational Constant, the Chandrasekhar Limit, and Neutron Star MassesPRL77(1996) pg. 1432-1435

  68. [68]

    G., Turyshev, S

    Williams, J. G., Turyshev, S. G., and Boggs, D. H.Progress in Lunar Laser Ranging Tests of Relativistic Gravity.Physical Review Letters93(2004) pg. 261101

  69. [69]

    Bai, Yang, Salvado, Jordi, and Stefanek, Ben A.Cosmological constraints on the gravita- tional interactions of matter and dark matter.JCAP2015(2015) pg. 029

  70. [70]

    Ooba, Junpei, Ichiki, Kiyotomo, Chiba, Takeshi, and Sugiyama, Naoshi.Cosmological con- straints on scalar-tensor gravity and the variation of the gravitational constant.Progress of Theoretical and Experimental Physics2017(2017) pg. 043E03

  71. [71]

    Copi, Craig J., Davis, Adam N., and Krauss, Lawrence M.New Nucleosynthesis Constraint on the Variation of G.PRL92(2004) pg. 171301

  72. [72]

    Alvey, J., Sabti, N., Escudero, M., and Fairbairn, M.Improved BBN constraints on the variation of the gravitational constant.European Physical Journal C80(2020) pg. 148

  73. [73]

    P., and Christensen-Dalsgaard, J.Asteroseismic Constraints on the Cosmic- time Variation of the Gravitational Constant from an Ancient Main-sequence Star.ApJL 887(2019) pg

    Bellinger, E. P., and Christensen-Dalsgaard, J.Asteroseismic Constraints on the Cosmic- time Variation of the Gravitational Constant from an Ancient Main-sequence Star.ApJL 887(2019) pg. L1

  74. [74]

    Williams, James G., Turyshev, Slava G., and Boggs, Dale H.Progress in Lunar Laser Ranging Tests of Relativistic Gravity.PRL93(2004) pg. 261101

  75. [75]

    Hofmann, F., and M¨ uller, J.Relativistic tests with lunar laser ranging.Classical and Quantum Gravity35(2018) pg. 035015

  76. [76]

    3431-3437

    Pitjeva, E.V., and Pitjev, N.P.Relativistic effects and dark matter in the Solar system from observations of planets and spacecraft.MNRAS432(2013) pg. 3431-3437

  77. [77]

    Celestial Mechanics and Dynamical Astronomy123(2015) pg

    Fienga, A., Laskar, J., Exertier, P., Manche, H., and Gastineau, M.Numerical estima- tion of the sensitivity of INPOP planetary ephemerides to general relativity parameters. Celestial Mechanics and Dynamical Astronomy123(2015) pg. 325-349

  78. [78]

    Genova, Antonio, Mazarico, Erwan, Goossens, Sander, Lemoine, Frank G., Neumann, Gre- gory A., Smith, David E., and Zuber, Maria T.Solar system expansion and strong equiv- alence principle as seen by the NASA MESSENGER mission.Nature Communications9 (2018) pg. 289

  79. [79]

    1151-1154

    Damour, Thibault, and Gibbons, Gary W., and Taylor, Joseph H.Limits on the variability of G using binary-pulsar data.PRL61(1988) pg. 1151-1154

  80. [80]

    F.High-Precision Timing of Millisecond Pulsars

    Kaspi, V.M., Taylor, J.H., and Ryba, M. F.High-Precision Timing of Millisecond Pulsars. III. Long-Term Monitoring of PSRs B1855+09 and B1937+21.ApJ428(1994) pg. 713

Showing first 80 references.