Abstract:Abstract. Our real universe is locally inhomogeneous. Dyer and Roeder introduced the smoothness parameter α to describe the influence of local inhomogeneity on angular diameter distance, and they obtained the angular diameter distance-redshift approximate relation (Dyer-Roeder equation) for locally inhomogeneous universe. Furthermore, the DistanceDuality (DD) relation, D L (z)(1 + z) −2 /D A (z) = 1, should be valid for all cosmological models that are described by Riemannian geometry, where D L and D A are, r… Show more
“…For a background concordance cosmology (i.e. w = −1), we confirm previous analyses [42,69] that find η = 0.81 ± 0.33 at the 68% C.L. However, we stress that we do not a priori fix the cosmological parameter values as in [42], but rather we constrain it with data complementary to SN Ia distances.…”
Constraints on models of the late time acceleration of the universe assume the cosmological principle of homogeneity and isotropy on large scales. However, small scale inhomogeneities can alter observational and dynamical relations, affecting the inferred cosmological parameters. For precision constraints on the properties of dark energy, it is important to assess the potential systematic effects arising from these inhomogeneities. In this study, we use the Type Ia supernova magnitude-redshift relation to constrain the inhomogeneities as described by the Dyer-Roeder distance relation and the effect they have on the dark energy equation of state (w), together with priors derived from the most recent results of the measurements of the power spectrum of the Cosmic Microwave Background and Baryon Acoustic Oscillations. We find that the parameter describing the inhomogeneities (η) is weakly correlated with w. The best fit values w = −0.933 ± 0.065 and η = 0.61 ± 0.37 are consistent with homogeneity at < 2σ level. Assuming homogeneity (η = 1), we find w = −0.961 ± 0.055, indicating only a small change in w. For a time-dependent dark energy equation of state, w 0 = −0.951 ± 0.112 and w a = 0.059 ± 0.418, to be compared with w 0 = −0.983 ± 0.127 and w a = 0.07 ± 0.432 in the homogeneous case, which is also a very small change. We do not obtain constraints on the fraction of dark matter in compact objects, f p , at the 95% C.L. with conservative corrections to the distance formalism. Future supernova surveys will improve the constraints on η, and hence, f p , by a factor of ∼ 10.
“…For a background concordance cosmology (i.e. w = −1), we confirm previous analyses [42,69] that find η = 0.81 ± 0.33 at the 68% C.L. However, we stress that we do not a priori fix the cosmological parameter values as in [42], but rather we constrain it with data complementary to SN Ia distances.…”
Constraints on models of the late time acceleration of the universe assume the cosmological principle of homogeneity and isotropy on large scales. However, small scale inhomogeneities can alter observational and dynamical relations, affecting the inferred cosmological parameters. For precision constraints on the properties of dark energy, it is important to assess the potential systematic effects arising from these inhomogeneities. In this study, we use the Type Ia supernova magnitude-redshift relation to constrain the inhomogeneities as described by the Dyer-Roeder distance relation and the effect they have on the dark energy equation of state (w), together with priors derived from the most recent results of the measurements of the power spectrum of the Cosmic Microwave Background and Baryon Acoustic Oscillations. We find that the parameter describing the inhomogeneities (η) is weakly correlated with w. The best fit values w = −0.933 ± 0.065 and η = 0.61 ± 0.37 are consistent with homogeneity at < 2σ level. Assuming homogeneity (η = 1), we find w = −0.961 ± 0.055, indicating only a small change in w. For a time-dependent dark energy equation of state, w 0 = −0.951 ± 0.112 and w a = 0.059 ± 0.418, to be compared with w 0 = −0.983 ± 0.127 and w a = 0.07 ± 0.432 in the homogeneous case, which is also a very small change. We do not obtain constraints on the fraction of dark matter in compact objects, f p , at the 95% C.L. with conservative corrections to the distance formalism. Future supernova surveys will improve the constraints on η, and hence, f p , by a factor of ∼ 10.
“…(While no useful constraints are possible, the global maximum likelihood in the λ 0 -Ω 0 -η cube also indicates a high value of η.) Unknown to me at the time, very similar results, based on the same data, were obtained by Yang et al (2013), Bréton & Montiel (2013), and, somewhat later, Li et al (2015) (the latter two restricted to a flat universe). While perhaps not surprising, it is of course important in science for results to be confirmed by others working independently.…”
Section: Relationsupporting
confidence: 74%
“…Busti et al (2013) compared the ZKDR distance to other approximations: the weak-lensing approximation with uncompensated density along the line of sight, the flux-averaging approximation, and a modified ZKDR distance which allows for a different expansion rate along the line of sight. This work is interesting for its analysis of the underlying issues (essentially assumptions about the mass distribution and how this affects light propagation, different approximations corresponding to different assumptions) and its combination of detailed theory and application to real data-the Union2.1 sample, also used by Helbig (2015a) and Yang et al (2013). 13.…”
The Universe is not completely homogeneous. Even if it is sufficiently so on large scales, it is very inhomogeneous at small scales, and this has an effect on light propagation, so that the distance as a function of redshift, which in many cases is defined via light propagation, can differ from the homogeneous case. Simple models can take this into account. I review the history of this idea, its generalization to a wide variety of cosmological models, analytic solutions of simple models, comparison of such solutions with exact solutions and numerical simulations, applications, simpler analytic approximations to the distance equations, and (for all of these aspects) the related concept of a 'Swiss-cheese' universe.
“…The ideal way to observationally test the CDDR is via independent measurements of intrinsic luminosities and sizes of the same object, without using a specific cosmological model [35]. We may quote approaches involving: measurements of the angular diameter distance (ADD) of galaxy clusters, observations of SNe Ia, estimates of the cosmic expansion H(z) from cosmic chronometers, measurements of the gas mass fraction in galaxy clusters and observations of strong gravitational lensing (SGL) [36,37,38,39,40,41,42,43,44,45]. All these tests were performed using different sources for D A and D L .…”
The cosmic distance duality relation (CDDR) has been test through several astronomical observations in the last years. This relation establishes a simple equation relating the angular diameter (DA) and luminosity (DL) distances at a redshift z, DLD −1 A (1 + z) −2 = η = 1. However, only very recently this relation has been observationally tested at high redshifts (z ≈ 3.6) by using luminosity distances from type Ia supernovae (SNe Ia) and gamma ray bursts (GRBs) plus angular diameter distances from strong gravitational lensing (SGL) observations. The results show that no significant deviation from the CDDR validity has been verified. In this work, we test the potentialities of future luminosity distances from gravitational waves (GWs) sources to impose limit on possible departures of CDDR jointly with current SGL observations. The basic advantage of DL from GWs is being insensitive to non-conservation of the number of photons. By simulating 600, 900 and 1200 data of GWs using the Einstein Telescope (ET) as reference, we derive limits on η(z) function and obtain that the results will be at least competitive with current limits from the SNe Ia + GRBs + SGLs analyses. *
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