Abstract

In standard Big Bang cosmology, the universe expanded from a very dense, hot and opaque initial state. The light that was last scattered about 380,000 years later, when the universe had become transparent, has been redshifted and is now seen as thermal radiation with a temperature of 2.7 K, the cosmic microwave background (CMB). However, since light escapes faster than matter can move, it is prudent to ask how we, made of matter from this very source, can still see the light. In order for this to be possible, the light must take a return path of the right length. A curved return path is possible in spatially closed, balloon-like models, but in standard cosmology, the universe is "flat" rather than balloon-like, and it lacks a boundary surface that might function as a reflector. Under these premises, radiation that once filled the universe homogeneously cannot do so permanently after expansion, and we cannot see the last scattering event. It is shown that the traditional calculation of the CMB temperature is flawed and that light emitted by any source inside the Big Bang universe earlier than half its "conformal age", also by distant galaxies, can only become visible to us via a return path. Although often advanced as the best evidence for a hot Big Bang, the CMB actually tells against a formerly smaller universe and so do the most distant galaxies. While standard cosmology has additional deficiencies, those disclosed here defy rationality and therefore make a more well-founded cosmology indispensable.

Highlights

  • In 1964, Penzias & Wilson (1965) serendipitously discovered the cosmic microwave background (CMB), a thermal radiation with a temperature of 2.7 K

  • Alpher & Herman (1948) and Alpher et al (1967), who were contemplating thermonuclear reactions in the expanding universe (for historical perspectives see Naselsky et al (2006) and Alpher (2012), expected a thermal radiation with about 5 K as a residual of a hot Big Bang. They built on Tolman’s studies (Tolman, 1931; Tolman, 1934) of model universes filled with blackbody radiation as a thermodynamic fluid, so that “The model of the expanding universe with which we deal, is one containing a homogeneous, isotropic mixture of matter and blackbody radiation” (Alpher & Herman, 1975)

  • Because of the inherent inconsistency of the standard ΛCDM concordance cosmology, here represented by model 4, it does not come as a surprise that “misconceptions and confusions have long been common in papers on cosmology, in many by renowned authors”, as reported by Davis & Lineweaver (2004)

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Summary

Indranil Banik Germany

Marcos C.D. Neves, State University of Maringá, Maringá, Brazil. Cosmology theory, concordance cosmology, big bang cosmology. This article is included in the Mathematical, Physical, and Computational Sciences collection

Louis Marmet Canada
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