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Autor principal: Matusch, Brendon
Formato: Preprint
Publicado: 2024
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Acceso en línea:https://arxiv.org/abs/2405.12233
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author Matusch, Brendon
author_facet Matusch, Brendon
contents The definition of thermodynamic entropy is dependent on one's assignment of physical microstates to observed macrostates. As a result, low entropy in the distant past could be equivalently explained by selection of a particular observer. In this paper, I make the case that because we observe a low-entropy past everywhere even as we look further and further away, anthropic selection over observers does not explain the non-equilibrium state of the observed cosmos. Under a uniform prior over possible world states, the probability of a non-equilibrium past, given our local observations, decreases to zero as the size of the world tends toward infinity. This claim is not dependent on choice of observer, unless the amount of information used to encode the observer's coarse-graining perception function scales linearly with the size of the world. As a result, for anthropic selection to choose a world like the one we live in, the initial state of a universe with size $N$ must be low-information, having Kolmogorov complexity that does not scale with $N$.
format Preprint
id arxiv_https___arxiv_org_abs_2405_12233
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Anthropic Selection for a Low-Entropy Past
Matusch, Brendon
High Energy Physics - Theory
Cosmology and Nongalactic Astrophysics
Statistical Mechanics
The definition of thermodynamic entropy is dependent on one's assignment of physical microstates to observed macrostates. As a result, low entropy in the distant past could be equivalently explained by selection of a particular observer. In this paper, I make the case that because we observe a low-entropy past everywhere even as we look further and further away, anthropic selection over observers does not explain the non-equilibrium state of the observed cosmos. Under a uniform prior over possible world states, the probability of a non-equilibrium past, given our local observations, decreases to zero as the size of the world tends toward infinity. This claim is not dependent on choice of observer, unless the amount of information used to encode the observer's coarse-graining perception function scales linearly with the size of the world. As a result, for anthropic selection to choose a world like the one we live in, the initial state of a universe with size $N$ must be low-information, having Kolmogorov complexity that does not scale with $N$.
title Anthropic Selection for a Low-Entropy Past
topic High Energy Physics - Theory
Cosmology and Nongalactic Astrophysics
Statistical Mechanics
url https://arxiv.org/abs/2405.12233