Abstract

In the late 1990’s, observations of two directionally-skewed samples of, in total, 93 Type Ia supernovae were analysed in the framework of the Friedmann–Lemaître–Robertson–Walker (FLRW) cosmology. Assuming these to be ‘standard(isable) candles’ it was inferred that the Hubble expansion rate is accelerating as if driven by a positive Cosmological Constant varLambda in Einstein’s theory of gravity. This is still the only direct evidence for the ‘dark energy’ that is the dominant component of today’s standard varLambda CDM cosmological model. Other data such as baryon acoustic oscillations (BAO) in the large-scale distribution of galaxies, temperature fluctuations in the cosmic microwave background (CMB), measurement of stellar ages, the rate of growth of structure, etc are all ‘concordant’ with this model but do not provide independent evidence for accelerated expansion. The recent discussions about whether the inferred acceleration is real rests on analysis of a larger sample of 740 SNe Ia which shows that these are not quite standard candles, and more importantly highlights the ‘corrections’ that are applied to analyse the data in the FLRW framework. The latter holds in the reference frame in which the CMB is isotropic, whereas observations are carried out in our heliocentric frame in which the CMB has a large dipole anisotropy. This is assumed to be of kinematic origin i.e. due to our non-Hubble motion driven by local inhomogeneity in the matter distribution which has grown under gravity from primordial density perturbations traced by the CMB fluctuations. The varLambda CDM model predicts how this peculiar velocity should fall off as the averaging scale is raised and the universe becomes sensibly homogeneous. However observations of the local ‘bulk flow’ are inconsistent with this expectation and convergence to the CMB frame is not seen. Moreover, the kinematic interpretation implies a corresponding dipole in the sky distribution of high redshift quasars, which is rejected by observations at 4.9sigma . Hence the peculiar velocity corrections employed in supernova cosmology are inconsistent and discontinuous within the data. The acceleration of the Hubble expansion rate is in fact anisotropic at 3.9sigma and aligned with the bulk flow. Thus dark energy could be an artefact of analysing data assuming that we are idealised observers in an FLRW universe, when in fact the real universe is inhomogeneous and anisotropic out to distances large enough to impact on cosmological analyses.

Highlights

  • The Cosmological Constant can be interpreted as the energy density of fluctuations of the vacuum in the quantum field theories that describe the energymomentum tensor

  • It was argued [13] that doing the analysis differently, and in particular taking into account other cosmological data such as on baryon acoustic oscillations (BAO) and cosmic microwave background (CMB) anisotropies analysed in the FLRW framework, firmly reinstates the acceleration of the universe

  • Since the CMB exhibits a large dipole anisotropy, this is assumed to be due to our motion with respect to the cosmic rest frame in which the Universe looks FLRW, and data can be analysed according to the Friedman–Lemaıtre equations

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Summary

Introduction

The Cosmological Constant can be interpreted as the energy density of fluctuations of the vacuum in the quantum field theories that describe the energymomentum tensor. H0 ≡ expansion rate and the only dimensionful parameter in the model.2 It was not until observations of 93 Type Ia supernova in the late 1990s claimed direct evidence for an accelerating Universe [9,10], that Λ was taken seriously and ΛCDM came to be canonised as the ‘standard model’ of cosmology. While any volume element in the FLRW model expands at the same rate as all others, as described by a single scale factor a, the expansion of the real Universe in GR is an average effect arising from the coarse-graining of small scales and is locally different everywhere [23] This is properly described by the Raychaudhury equation— which reduces to the Friedmann-Lemaıtre equation as a limiting case [24].3.

The universe is anisotropic
Supernova cosmology
Standardisable candles?
The statistical method
The accelerated expansion of the Universe
Peculiar velocity corrections and the ‘fitting problem’
Findings
Conclusions
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