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New analysis of SNeIa Pantheon Catalog: Variable speed of light as an alternative to dark energy

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Abstract

In A&A 412, 35 (2003) Blanchard, Douspis, Rowan-Robinson, and Sarkar (BDRS) slightly modified the primordial fluctuation spectrum and produced an excellent fit to WMAP's CMB power spectrum for an Einstein-de Sitter (EdS) universe, bypassing dark energy. Curiously, they obtained a Hubble value of H046H_0\approx46, in sharp conflict with the canonical range H06773H_0\sim67-73. However, we will demonstrate that the reduced value of H046H_0\approx46 achieved by BDRS is fully compatible with the use of variable speed of light in analyzing the late-time cosmic acceleration observed in Type Ia supernovae (SNeIa). In arXiv:2412.04257 [gr-qc] we uncovered a hidden aspect in a generic class of scale-invariant actions: the dynamics of the dilaton can induce a variation in the speed of light as cχ1/2c\propto\chi^{1/2}, causing c to vary alongside χ\chi across spacetime. For an EdS universe with varying c, besides the effects of cosmic expansion, light waves emitted from distant SNeIa are further subject to a refraction effect, which alters the Lemaitre redshift relation to 1+z=a3/21+z=a^{-3/2}. Based on this new formula, we achieve a fit to the SNeIa Pantheon Catalog exceeding the quality of the Λ\LambdaCDM model. Crucially, our approach does not require dark energy and produces H0=47.2H_0=47.2 in strong alignment with the BDRS finding of H046H_0\approx46. Hence, BDRS's analysis of the (early-time) CMB power spectrum and our variable-c analysis of the (late-time) Hubble diagram of SNeIa fully agree on two counts: (i) the dark energy hypothesis is avoided, and (ii) H0H_0 is reduced to 47\sim47, which also yields an age t0=2/(3H0)=13.8t_0=2/(3H_0)=13.8 Gy for an EdS universe, without requiring dark energy. Most importantly, we will demonstrate that the late-time acceleration can be attributed to the declining speed of light in an expanding EdS universe, rather than to a dark energy component.

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The varying speed of light (VSL) theory is controversial. It succeeds in explaining some cosmological problems, but on the other hand it is excluded by mainstream physics because it will shake the foundation of physics. In the present paper, we devote ourselves to test whether the speed of light is varying from the observational data of the type Ia Supernova, Baryon Acoustic Oscillation, Observational H(z) data and Cosmic Microwave Background (CMB). We select the common form c(t)=c0an(t)c(t)=c_0a^n(t) with the contribution of dark energy and matter, where c0c_0 is the current value of speed of light, n is a constant, and consequently construct a varying speed of light dark energy model (VSLDE). The combined observational data show a much trivial constraint n=0.0033±0.0045n=-0.0033 \pm 0.0045 at 68.3\% confidence level, which indicates that the speed of light may be a constant with high significance. By reconstructing the time-variable c(t), we find that the speed of light almost has no variation for redshift z<101z < 10^{-1}. For high-z observations, they are more sensitive to the VSLDE model, but the variation of speed of light is only in order of 10210^{-2}. We also introduce the geometrical diagnostic Om(z)Om (z) to show the difference between the VSLDE and Λ\LambdaCDM model. The result shows that the current data are difficult to differentiate them. All the results show that the observational data favor the constant speed of light.
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The varying speed of light (VSL) model describes how the speed of light in a vacuum changes with cosmological redshift. Despite numerous models, there is little observational evidence for this variation. While the speed of light can be accurately measured by physical means, cosmological methods are rarely used. Previous studies quantified the speed of light at specific redshifts using Gaussian processes and reconstructed the redshift-dependent function c(z). It is crucial to quantify the speed of light across varying redshifts. We use the latest data on angular diameter distances DA(z)D_\mathrm{ A}(z) and Hubble parameters H(z) from baryon acoustic oscillation and cosmic chronometer measurements in the redshift interval z[0.07,1.965]z\in [0.07,1.965]. The speed of light c(z) is determined using Gaussian and deep Gaussian processes to reconstruct H(z), DA(z)D_\mathrm{ A}(z), and DA(z)D^{\prime }_\mathrm{ A}(z). Furthermore, we conduct comparisons across three distinct models, encompassing two renowned VSL models. We get the result of the parameters constraints in the models (1) for the ‘c-c’ model, c0=29492.6±5.36.2 km s1c_0=29\,492.6 \pm ^{6.2}_{5.3} \mathrm{~km} \mathrm{~s}^{-1}. (2) For the ‘c-cl’ model, c0=29665.5±11.411.2 km s1c_0=29\,665.5 \pm ^{11.2}_{11.4}\mathrm{~km} \mathrm{~s}^{-1} and n=0.05535 \pm\, ^{0.00008}_{0.00007}. (3) For the ‘c-CPL’ model, c0=29555.7±13.213.3 km s1c_0=29\,555.7 \pm ^{13.3}_{13.2} \mathrm{~km} \mathrm{~s}^{-1} and n=0.0607±0.0001n=-0.0607 \pm 0.0001. Based on our findings, it may be inferred that Barrow’s classical VSL model is not a suitable fit for our data. In contrast, the widely recognized Chevallier–Polarski–Linder (CPL) VSL model, under some circumstances, as well as the universal ‘c is constant’ model, demonstrate a satisfactory ability to account for our findings.
Article
The Friedmann-Lemaître-Robertson-Walker model establishes the correlation between redshifts and distances. It has a metric expansion of space. As a result, the wavelength of photons propagating through the expanding space is stretched, creating the cosmological redshift, z. It also relates the frequency of light detected by a local observer to that emitted from a distant source. In standard cosmology (i.e., a constant speed light model), this relation is given by a factor 1/(1 + z). However, this ratio is modified in the minimally extended varying speed of light model (meVSL, c = c0ab/4) as 1/(1 + z)1 − b/4. This time dilation effect is detected as the observed rate of the time variation in the intensity of emitted radiation. The spectra of type Ia supernovae (SNe Ia) provide a reliable way to measure the apparent aging rate of distant objects. We use data on 13 high-redshift (0.28 ≤ z ≤ 0.62) SNe Ia to obtain b = 0.198 ± 0.415 at the 1-σ confidence interval. The current data is too sparse to give meaningful constrain on the meVSL and cannot distinguish the meVSL model from the standard model.
Article
At least one dimensionless physical constant (i.e., a physically observable) must change for the cosmic time to make the varying speed of light (VSL) models phenomenologically feasible. Various physical constants and quantities also should be functions of cosmic time to satisfy all known local laws of physics, including special relativity, thermodynamics, and electromagnetism. Adiabaticity is another necessary condition to keep the homogeneity and isotropy of three-dimensional space. To be a self-consistent theory, one should consider cosmic evolutions of physical constants and quantities when one derives Einstein’s field equations and their solutions. All these conditions are well satisfied in the so-called minimally extended varying speed of light (meVSL) model. Unlike other VSL models, we show that the redshift-drift formula of the meVSL model is the same as a standard model. Therefore, we cannot use this as an experimental tool to verify the meVSL. Instead, one can still use the cosmological chronometers (CC) as a model-independent test of the meVSL. The current CC data cannot distinguish meVSL from the standard model (SM) when we adopt the best-fit values (or Gaussian prior) of H0 and Ωm0 from the Planck mission. However, the CC data prefer the meVSL when we choose Pantheon22 data.
Article
In standard cosmology, redshift is related to scale factor by z = a−1 − 1. Varying speed of light cosmologies also have applied this relationship, in which c does not explicitly appear, with the assumption that ℏ∝c. Measured redshift is not a comparison of an observed spectrum with the spectrum as it was emitted at a distant location, but a comparison with a reference spectrum generated more locally. This distinction suggests decomposition into two parts: (a) change during the flight of a photon, and (b) difference in physics at the time of emission and at the time of observation of a photon associated with an electron transition between specific bound states of an atom. Based on atomic units consistent with data and a relativistic atomic model, redshift is given by z = β(θ)θa−1 − 1, where θ = c/c0, with c0 the present value of c, and β is a function of the atomic parameters describing the transition. The modified form appears to have a modest effect (a difference in scale factor < 2 %) for redshifts that are not much greater than 10. However, the modification can have a major effect for an early universe with c significantly larger than the present. The simplified form z = θa−1 − 1, which results from a non-relativistic model, provides an approximation for redshift that is not transition-specific.
Article
The Co-varying Physical Couplings (CPC) framework is a modified gravity set up assuming Einstein Field Equations wherein the quantities {G, c, Λ} are promoted to spacetime functions. Bianchi identity and the requirement of stress-energy tensor conservation entangle the possible variations of the couplings {G, c, Λ}, which are forced to co-vary as dictated by the General Constraint (GC). In this paper we explore a cosmological model wherein G, c and Λ are functions of the redshift respecting the GC of the CPC framework. We assume a linear parameterization of Λ in terms of the scale factor a. We use the ansatz G˙/G=σ(c˙/c)\dot{G}/G = \sigma \left( \dot{c}/c \right) with σ = constant to deduce the functional forms of c = c(z) and G = G(z). We show that this varying-{G, c, Λ} model fits SNe Ia data and H(z) data with σ = 3. The model parameters can be constrained to describe dark energy at the background level.
Article
Previous researches on high-energy photon events from gamma-ray bursts (GRBs) suggest a light speed variation v(E)=c(1−E/ELV) with ELV=3.6×1017 GeV, together with a pre-burst scenario that hight-energy photons come out about 10 seconds earlier than low-energy photons at the GRB source. However, in the Lorentz symmetry violating scenario with an energy dependent light speed considered here, high-energy photons travel slower than low-energy photons due to the light speed variation, so that they are usually detected after low-energy photons in observed GRB data. Here we find three high-energy photon events which were observed earlier than low-energy photons from Fermi Gamma-ray Space Telescope (FGST), and analysis on these photon events supports the pre-burst scenario of high energy photons from GRBs and the energy dependence of light speed listed above.
Article
The invariance of the speed of light in the distant universe has profound significance for fundamental physics. In this paper, we propose a new model-independent method to test the invariance of the speed of light c at different redshifts by combining the strong gravitational lensing (SGL) systems and the observations of type-Ia supernovae (SNe Ia). All the quantities used to test the deviation of c come from the direct observations, and the absolute magnitudes of SNe Ia need not to be calibrated. Our results show that the speed of light in the distant universe is no obvious deviation from the constant value c0 within the uncertainty based on current observations. Moreover, we conclude that the currently compiled SGL and SNe Ia Pantheon samples may achieve much higher precision Δc/c ∼ 10−2 for the deviation of c than all previously considered approaches. The forthcoming data from the Legacy Survey of Space and Time and Wide-Field InfraRed Space Telescope will achieve more stringent testing for deviation of the SOL (at the level of Δc/c ∼ 10−3) by using our model-independent method. Finally, we discuss the potential ways in which our technique might be improved, focusing on the treatment of possible sources of systematic uncertainties.
Article
We have used the recently published varying physical constants (VPC) approach in an attempt to resolve the primordial lithium abundance problem. The value of the ratio of ⁷Li to hydrogen ⁷Li/H = 1.400 ( ± 0.023) × 10⁻¹⁰ we have calculated using this approach is about four times lower than that estimated using the standard lambda cold dark matter (ΛCDM) cosmological model, and is consistent with the most agreed observational value of 1.6 ( ± 0.3) × 10⁻¹⁰. In the VPC approach Einstein equations are modified to include the variation of the speed of light c, gravitational constant G and cosmological constant Λ using the Einstein-Hilbert action. Application of this approach to cosmology naturally leads to the variation of the Plank constant ℏ and the Boltzmann constant kB as well. They approach fixed values at the scale factor a ≪ 1: c = c0/e, G = G0/e³, ℏ = ℏ0/e and kB = kB0/e5/4, where e is the Euler's number (= 2.7183). Since the VPC cosmology reduces to the same form as the ΛCDM cosmology at very small scale factors, we could use an existing Big-Bang nucleosynthesis (BBN) code AlterBBN with the above changes to calculate the light element abundances under the VPC cosmology. Among other abundances we have calculated at baryon to photon ratio η = 6.1 × 10⁻¹⁰ are: ⁴He/H = 0.2478 ( ± 0.0041), D/H = 2.453 ( ± 0.041) × 10⁻⁵, ³He/H = 2.940 ( ± 0.049) × 10⁻⁵.
Article
We have shown that the varying physical constant model is consistent with the recently published variational approach wherein Einstein equations are modified to include the variation of the speed of light c, gravitational constant G, and cosmological constant Λ using the Einstein–Hilbert action. The general constraint resulting from satisfying the local conservation laws and contracted Bianchi identities provides the freedom to choose the form of the variation of the constants as well as how their variations are related. When we choose {\dot{G}}/G = 3\,\underset{\raise0.3em\hbox{\smash{\scriptscriptstyle\cdot}}}{\dot{c}} /c,\,c = {c_0}\,{\rm{exp}}\,[({a^\alpha} - 1)],\,G = {G_0}\,{\rm{exp}}\,[3({a^\alpha} - 1)], and Λ=Λ0 exp[(aα1)]{\rm{\Lambda }} = {{\rm{\Lambda }}_0}\ \exp [ {( {{a^{ - \alpha }} - 1} )} ], where a is the scale factor and α = 1.8, we are able to show that the resulting model: (a) fits the supernova 1a observational data marginally better than the Lambda cold dark matter (ΛCDM) model; (b) determines the first peak in the power spectrum of the cosmic microwave background temperature anisotropies at a multipole value of l=217.3l = 217.3; (c) calculates the age of the Universe as 14.1 Gyr; and (d) finds the BAO acoustic scale to be 145.2 Mpc. These numbers are within less than 3 per cent of the values derived using the ΛCDM model. Surprisingly, we find that the dark-energy density is negative in a Universe that has significant negative curvature and whose expansion is accelerating at a faster rate than that predicted by the ΛCDM model.
Article
We develop an action principle to construct the dynamics that gives rise to a minimal generalization of Einstein’s equations, where the speed of light ([Formula: see text]), the gravitational constant ([Formula: see text]) and the cosmological constant ([Formula: see text]) are allowed to vary. Our construction preserves general covariance of the theory, which yields a general dynamical constraint on [Formula: see text], [Formula: see text] and [Formula: see text]. This action is general and can be applied to describe different cosmological solutions. We apply this formulation to the initial condition puzzles of the early universe and show that it generates a dynamical mechanism to obtain the homogeneous and flat universe we observe today. We rewrite the conditions necessary to solve the horizon and flatness problems in this framework, which does not necessarily lead to an accelerated expansion as in inflation. Then, we show how the dynamics of the scalar field that represents [Formula: see text] or [Formula: see text] (and [Formula: see text]) can be used to solve the problems of the early universe cosmology by means of different ways to [Formula: see text]-inflate the horizon in the early universe. By taking [Formula: see text], we show that the dynamics of the scalar field representing [Formula: see text] can be described once a potential is given.
Article
Phantom dark energy (w<−1) can produce amplified cosmic acceleration at late times, thus increasing the value of H0 favored by CMB data and releasing the tension with local measurements of H0. We show that the best fit value of H0 in the context of the CMB power spectrum is degenerate with a constant equation-of-state parameter w, in accordance with the approximate effective linear equation H0+30.93w−36.47=0 (H0 in km sec−1 Mpc−1). This equation is derived by assuming that both Ω0mh2 and dA=∫0zrecdzH(z) remain constant (for an invariant CMB spectrum) and equal to their best fit Planck/ΛCDM values as H0, Ω0m, and w vary. For w=−1, this linear degeneracy equation leads to the best fit H0=67.4 km sec−1 Mpc−1 as expected. For w=−1.22, the corresponding predicted CMB best fit Hubble constant is H0=74 km sec−1 Mpc−1, which is identical with the value obtained by local-distance ladder measurements, while the best fit matter density parameter is predicted to decrease, since Ω0mh2 is fixed. We verify the above H0−w degeneracy equation by fitting a wCDM model with fixed values of w to the Planck TT spectrum, showing also that the quality of fit (χ2) is similar to that of ΛCDM. However, when including SnIa, baryon acoustic oscillation, or growth data, the quality of fit becomes worse than ΛCDM when w<−1. Finally, we generalize the H0−w(z) degeneracy equation for the parametrization w(z)=w0+w1z/(1+z) and identify analytically the full w0−w1 parameter region (straight line) that leads to a best fit H0=74 km sec−1 Mpc−1 in the context of the Planck CMB spectrum. This exploitation of H0−w(z) degeneracy can lead to immediate identification of all parameter values of a given w(z) parametrization that can potentially resolve the H0 tension.
Article
Because of the high energies and long distances to the sources, astrophysical observations provide a unique opportunity to test possible signatures of Lorentz invariance violation (LIV). Superluminal LIV enables the decay of photons at high energy. The high altitude water Cherenkov (HAWC) observatory is among the most sensitive gamma-ray instruments currently operating above 10 TeV. HAWC finds evidence of 100 TeV photon emission from at least four astrophysical sources. These observations exclude, for the strongest of the limits set, the LIV energy scale to 2.2×1031 eV, over 1800 times the Planck energy and an improvement of 1 to 2 orders of magnitude over previous limits.
Article
We present a novel method to reconstruct the temporal evolution of the speed of light c ( z ) in a flat Friedmann-Robertson-Walker (FRW) Universe using astronomical observations. After validating our pipeline with mock datasets, we apply our method to the latest baryon acoustic oscillations (BAO) and supernovae observations, and reconstruct c ( z ) in the redshift range of z ∈ [0,1.5]. We find no evidence of a varying speed of light, although we see some interesting features of Δ c ( z ), the fractional difference between c ( z ) and c 0 (the speed of light in the International System of Units), eg, Δ c ( z ) < 0 and Δ c ( z ) > 0 at 0.2 ≲ z ≲ 0.5 and 0.8 ≲ z ≲ 1.3, respectively, although the significance of these features is currently far below statistical importance.
Article
In this paper, the Lorentz invariance violation (LIV) is introduced in the calculations of photon propagation in the universe. LIV is considered in the photon sector, and the mean-free path of the γγ → e⁺e⁻ interaction is calculated. The corresponding photon horizon, including LIV effects, is used to predict major changes in the propagation of photons with energy above 10¹⁸ eV. The flux of GZK photons on Earth, considering LIV, is calculated for several source models of ultra-high-energy cosmic rays (UHECRs). The predicted flux of GZK gamma-rays is compared to the new upper limits on the photon flux obtained by the Pierre Auger Observatory in order to impose upper limits on the LIV coefficients of order n = 0, 1, and 2. The limits on the LIV coefficients derived here are more realistic than previous works and in some cases more restrictive. The analysis resulted in LIV upper limits in the photon sector of δγ,0limit ∼ -10⁻²⁰,δγ,1limit ∼ -10⁻³⁸eV⁻², δγ,2limit ∼ -10⁻⁵⁶eV⁻²in the astrophysical scenario, which best describes UHECR data. © 2018. The American Astronomical Society. All rights reserved.
Article
Many varying speed of light (VSL) theories have been developed recently. Here we address the issue of their observational verification in a fully comprehensive way. By using the most updated cosmological probes, we test three different candidates for a VSL theory (Barrow & Magueijo, Avelino & Martins, and Moffat). We consider many different Ansätze for both the functional form of c(z) and the dark energy dynamics. We compare these results using a reliable statistical tool such as the Bayesian evidence. We find that the present cosmological data are perfectly compatible with any of these VSL scenarios, but for the Moffat model there is a higher Bayesian evidence ratio in favor of VSL rather than the c = constant ΛCDM scenario. Moreover, in such a scenario, the VSL signal can help to strengthen constraints on the spatial curvature (with indication toward an open universe), to clarify some properties of dark energy (exclusion of a cosmological constant at 2σ level), and is also falsifiable in the near future owing to peculiar issues that differentiate this model from the standard one. Finally, we apply an information prior and entropy prior in order to put physical constraints on the models, though still in favor Moffat's proposal. © 2017. The American Astronomical Society. All rights reserved.
Article
We investigate a new method to recover (if any) a possible varying speed of light (VSL) signal from cosmological data. It comes as an upgrade by Salzano, Dąbrowski, and Lazkoz [Phys. Rev. Lett.114, 101304 (2015); Phys. Rev. D 93, 063521 (2016)], where it was argued that such a signal could be detected at a single redshift location only. Here, we show how it is possible to extract information on a VSL signal on an extended redshift range. We use mock cosmological data from future galaxy surveys (BOSS, DESI, WFirst-2.4 and SKA): the sound horizon at decoupling imprinted in the clustering of galaxies (baryon acoustic oscillations) as an angular diameter distance, and the expansion rate derived from those galaxies recognized as cosmic chronometers. We find that, given the forecast sensitivities of such surveys, a ∼1% VSL signal can be detected at 3σ confidence level in the redshift interval z∈[0.,1.55]. Smaller signals (∼0.1%) will be hardly detected (even if some lower possibility for a 1σ detection is still possible). Finally, we discuss the degeneration between a VSL signal and a non-null spatial curvature; we show that, given present bounds on curvature, any signal, if detected, can be attributed to a VSL signal with a very high confidence. On the other hand, our method turns out to be useful even in the classical scenario of a constant speed of light: in this case, the signal we reconstruct can be totally ascribed to spatial curvature and, thus, we might have a method to detect a 0.01-order curvature in the same redshift range with a very high confidence.
Article
The varying speed of light (VSL) has been used in cosmological models in which the physical constants vary over time. On the other hand, the Dvali, Gabadadze and Porrati (DGP) brane world model, especially its normal branch has been extensively discussed to justify the current cosmic acceleration. In this article we show that the normal branch of DGP in VSL cosmology leads to a self-accelerating behavior and therefore can interpret cosmic acceleration. Applying statefinder diagnostics demonstrate that our result slightly deviates {\Lambda}CDM model.
Article
We revisit the possibility that the Planck mass is spontaneously generated in scale invariant scalar-tensor theories of gravity, typically leading to a "dilaton." The fifth force, arising from the dilaton, is severely constrained by astrophysical measurements. We explore the possibility that nature is fundamentally Weyl-scale invariant and argue that, as a consequence, the fifth force effects are dramatically suppressed and such models are viable. We discuss possible obstructions to maintaining scale invariance and how these might be resolved.
Article
In this paper we extend a new method to measure possible variation of the speed of light by using Baryon Acoustic Oscillations and the Hubble function presented in our earlier paper [V. Salzano, M. P. D\c{a}browski, and R. Lazkoz, Phys. Rev. D93, 063521 (2016)] onto an inhomogeneous model of the universe. The method relies on the fact that there is a simple relation between the angular diameter distance (DA)(D_{A}) maximum and the Hubble function (H) evaluated at the same maximum-condition redshift, which includes speed of light c. One limit of such method was the assumption of null spatial curvature (even if we showed that even a non-zero curvature would have negligible effects). Here, we move one step further: we explicitly assume a model with intrinsic non-null curvature, and calculate the exact relation between DAD_{A} and H in this case. Then, we evaluate if current or future missions such as SKA can be sensitive enough to detect any such kind of spatial variation of c which can perhaps be related to the recently observed spatial variation of the fine structure constant (an effect known as α\alpha-dipole).
Article
Big Bang models of the Universe predict rapid domination by curvature, a paradox known as the flatness problem. Solutions to this problem usually leave the Universe exactly flat for every practical purpose. Explaining a nearly but not exactly flat current Universe is a new problem, which we label the quasi-flatness problem. We show how theories incorporating time-varying coupling constants could drive the Universe to a late-time near-flat attractor. A similar problem may be posed with regards to the cosmological constant Λ, the quasi-lambda problem, and we exhibit a solution to this problem as well.