Abstract:We use current measurements of the expansion rate H(z) and cosmic background radiation bounds on the spatial curvature of the Universe to impose cosmological model-independent constraints on cosmic opacity. To perform our analyses, we compare opacity-free distance modulus from H(z) data with those from two type Ia supernovae compilations, namely, the Union2.1 plus the most distant spectroscopically confirmed SNe Ia (SCP-0401 at z = 1.713) and two Sloan Digital Sky Survey (SDSS) subsamples. We find that a co… Show more
“…Based on previous works [28,29], we introduce an improved method to get luminosity distances that are not affected by cosmic opacity and are also independent of any specific cosmological model. We consider constructing 19 luminosity distances D H L (z n ), n = 1, 2...19, from the H(z) data at the corresponding redshifts by:…”
Section: Methodsmentioning
confidence: 99%
“…On the other hand, in Refs. [24,[28][29][30], distances derived from other opacity-independent probes, e.g. observational determinations of the Hubble parameter H(z) based on differential ageing of passively evolving galaxies (also dubbed "cosmic chronometers") [31], were proposed to test or even quantify cosmic opacity by comparing these distances with those from SN Ia observations.…”
Section: Introductionmentioning
confidence: 99%
“…What is more, in Refs. [28,29], the authors constructed luminosity distances from H(z) data but did not take the correlations between different redshifts into account. This treatment would lead to inaccurate estimations of the errors.…”
We present our study on cosmic opacity, which relates to changes in photon number as photons travel from the source to the observer. Cosmic opacity may be caused by absorption/scattering due to matter in the universe, or by extragalactic magnetic fields that can turn photons into unobserved particles (e.g. light axions, chameleons, gravitons, Kaluza-Klein modes), and it is crucial to correctly interpret astronomical photometric measurements like type Ia supernovae observations. On the other hand, the expansion rate at different epochs, i.e. the observational Hubble parameter data H(z), are obtained from differential ageing of passively evolving galaxies or from baryon acoustic oscillations and thus are not affected by cosmic opacity. In this work, we first construct opacity-free luminosity distances from H(z) determinations, taking correlations between different redshifts into consideration for our error analysis. Moreover, we let the light-curve fitting parameters, accounting for distance estimation in type Ia supernovae observations, free to ensure that our analysis is authentically cosmological-model-independent and gives a robust result. Any non-zero residuals between these two kinds of luminosity distances can be deemed as an indication of the existence of cosmic opacity. While a transparent universe is currently consistent with the data, our results show that strong constraints on opacity (and consequently on physical mechanisms that could cause it) can be obtained in a cosmological-model-independent fashion.PACS numbers: 98.80.-k, 98.80.Es
“…Based on previous works [28,29], we introduce an improved method to get luminosity distances that are not affected by cosmic opacity and are also independent of any specific cosmological model. We consider constructing 19 luminosity distances D H L (z n ), n = 1, 2...19, from the H(z) data at the corresponding redshifts by:…”
Section: Methodsmentioning
confidence: 99%
“…On the other hand, in Refs. [24,[28][29][30], distances derived from other opacity-independent probes, e.g. observational determinations of the Hubble parameter H(z) based on differential ageing of passively evolving galaxies (also dubbed "cosmic chronometers") [31], were proposed to test or even quantify cosmic opacity by comparing these distances with those from SN Ia observations.…”
Section: Introductionmentioning
confidence: 99%
“…What is more, in Refs. [28,29], the authors constructed luminosity distances from H(z) data but did not take the correlations between different redshifts into account. This treatment would lead to inaccurate estimations of the errors.…”
We present our study on cosmic opacity, which relates to changes in photon number as photons travel from the source to the observer. Cosmic opacity may be caused by absorption/scattering due to matter in the universe, or by extragalactic magnetic fields that can turn photons into unobserved particles (e.g. light axions, chameleons, gravitons, Kaluza-Klein modes), and it is crucial to correctly interpret astronomical photometric measurements like type Ia supernovae observations. On the other hand, the expansion rate at different epochs, i.e. the observational Hubble parameter data H(z), are obtained from differential ageing of passively evolving galaxies or from baryon acoustic oscillations and thus are not affected by cosmic opacity. In this work, we first construct opacity-free luminosity distances from H(z) determinations, taking correlations between different redshifts into consideration for our error analysis. Moreover, we let the light-curve fitting parameters, accounting for distance estimation in type Ia supernovae observations, free to ensure that our analysis is authentically cosmological-model-independent and gives a robust result. Any non-zero residuals between these two kinds of luminosity distances can be deemed as an indication of the existence of cosmic opacity. While a transparent universe is currently consistent with the data, our results show that strong constraints on opacity (and consequently on physical mechanisms that could cause it) can be obtained in a cosmological-model-independent fashion.PACS numbers: 98.80.-k, 98.80.Es
“…We follow the methodology firstly presented by [30] where one transforms H(z) measurements into cosmological distance estimates by solving numerically the comoving distance integral for non-uniformly spaced data, i.e.,…”
Section: Distances From H(z) Measurementsmentioning
The cosmic distance duality relation is a milestone of cosmology involving the luminosity and angular diameter distances. Any departure of the relation points to new physics or systematic errors in the observations, therefore tests of the relation are extremely important to build a consistent cosmological framework. Here, two new tests are proposed based on galaxy clusters observations (angular diameter distance and gas mass fraction) and H(z) measurements. By applying Gaussian Processes, a non-parametric method, we are able to derive constraints on departures of the relation where no evidence of deviation is found in both methods, reinforcing the cosmological and astrophysical hypotheses adopted so far.
“…Holanda et al [85] parametrized the redshift dependence of η(z) in two distinct forms, η(z) = 1 + η 0 z(P1) and η(z) = 1 + η 0 z/(1 + z)(P2) and investigated the η 0 parameter by employing the luminosity distance D L measurements from Type Ia supernovae (SNe Ia) and diameter distance D A from galaxy clusters [86,87]. Several other authors have also tested the DDR relation using different observations: SNe Ia plus cosmic microwave background (CMB) and barion acoustic oscillations (BAO) [88], SNe Ia plus H(z) data [77,[89][90][91], gas mass fraction of galaxy clusters and SNe Ia [92,93], CMB spectrum [94], gammaray burst (GRB) plus H(z) [95], SNe Ia plus BAO [96], gas mass fraction plus H(z) [97], gravitational lensing plus SNe Ia [98], SNe Ia and radio galaxy plus CMB [99]. Most of the above authors obtain no significant deviation in DDR relation, although, roughly the scatter in η 0 parameter is observed as ±0.1 to ±0.…”
One of the fundamental results used in observational cosmology is the distance duality relation (DDR), which relates the luminosity distance, DL, with angular diameter distance, DA, at a given redshift z. We employ the observed limits of this relation to constrain the coupling of axion like particles (ALPs) with photons. With our detailed 3D ALP-photon mixing simulation in standard ΛCDM universe and latest DDR limits observed in Holand & Barros (2016) we limit the coupling constant g φ ≤ 6 × 10 −13 GeV −1 nG B Mpc for ALPs of mass ≤ 10 −15 eV. The DDR observations can provide very stringent constraint on ALPs mixing in future. Also any deviation in DDR can be conventionally explained as photons decaying to axions or vice-versa.
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