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Vacuum Energy, Black Holes and the Cosmological Constant
General Physics · Submitted 6 Feb 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Using the recently proposed thermodynamical equation of state obeyed by the cosmological constant we indicate, how this idea might explain the smallness of the cosmological constant, if the vacuum energy is the source of the cosmological constant.
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We consider a possibility that the formally infinite vacuum energy of the quantized matter fields could be stored into Planck-size quantum black holes acting as the fundamental constituents of space and time. Using the recently proposed thermodynamical equation of state obeyed by the cosmological constant we indicate, how this idea might explain the smallness of the cosmological constant, if the vacuum energy is the source of the cosmological constant.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider a possibility that the formally infinite vacuum energy of the quantized matter fields could be stored into Planck-size quantum black holes acting as the fundamental constituents of space and time. | contribution 0.90 | 0.26 | 0.16 | hedged possibility 0.92 |
| s1 | Using the recently proposed thermodynamical equation of state obeyed by the cosmological constant we indicate, how this idea might explain the smallness of the cosmological constant, if the vacuum energy is the source of the cosmological constant. | interpretation 0.43 | 0.66 | 0.47 | hedged possibility 0.64 |
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Original abstract
We consider a possibility that the formally infinite vacuum energy of the quantized matter fields could be stored into Planck-size quantum black holes acting as the fundamental constituents of space and time. Using the recently proposed thermodynamical equation of state obeyed by the cosmological constant we indicate, how this idea might explain the smallness of the cosmological constant, if the vacuum energy is the source of the cosmological constant.
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When the static coordinates, together with the natural units, where $ħ= c = G = k_B = 1$ are used, the line element of the de Sitter spacetime may be written as: [ref] [equation] The de Sitter spacetime has the cosmological horizon, where [equation] Unfortunately, the de Sitter metric is singular at the cosmological horizon, and therefore we shall consider, instead of the cosmological horizon itself, a sort of "shrinked horizon", which is a spacelike two-sphere with constant $r$ and $t$ just inside of the cosmological horizon, where $r=r_C$.
Adventures in de Sitter space · Introduction · 0.83
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