The Heisenberg limit at cosmological scales
arXiv:2112.07359 · doi:10.1007/s10701-021-00531-z
Abstract
For an observation time {equal to} the universe age, the Heisenberg principle fixes the value of the smallest measurable mass at kg and prevents to probe the masslessness for any particle using a balance. The corresponding reduced Compton length to is $\lambdabar_{\rm H}$, and represents the length limit beyond which masslessness cannot be proved using a metre ruler. In turns, $\lambdabar_{\rm H}$ is equated to the luminosity distance which corresponds to a red shift . When using the Concordance-Model parameters, we get Gpc and . Remarkably, falls quite short to the radius of the {\it observable} universe. According to this result, tensions in cosmological parameters could be nothing else but due to comparing data inside and beyond . Finally, in terms of quantum quantities, the expansion constant reveals to be one order of magnitude above the smallest measurable energy, divided by the Planck constant
arXiv commentA different view on the Hubble tension. To appear in final form on Foundations of Physics by Springer, as follow-on of Capozziello S., Benetti M., Spallicci A.D.A.M., 2020, Found. Phys., 50, 893
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