The Trapped False-Vacuum Fraction at Percolation and the Energy It Withholds From the Plasma

At percolation the false-vacuum fraction is 0.712, and even at the late stage I = 2 more than thirteen percent of space remains unconverted; genuine completion to the one-percent level requires I = 4.5, where the fraction is 0.0111. The withheld shares at percolation are 0.065 of the total energy for a strength of 0.1 and 0.356 for a strength of unity. In other words, an estimate that spends the whole latent heat at percolation overstates the immediately available fluid energy by roughly a third of the latent component in the strong case. The withheld energy is not lost; it arrives as the pockets collapse, which stretches the effective source duration while lowering its early amplitude, a trade that simple one-number amplitude formulae do not represent. This study is simulated and computed from stated assumptions; it is not a measurement.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-11
DOI
https://doi.org/10.5281/zenodo.24145482
Primary Topic
Cosmology and Gravitation Theories
Type
article
Field-Weighted Citation Impact
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article

The Trapped False-Vacuum Fraction at Percolation and the Energy It Withholds From the Plasma

William Alexander Aldred
Zenodo (CERN European Organization for Nuclear Research)
Cosmology and Gravitation Theories
article

The Trapped False-Vacuum Fraction at Percolation and the Energy It Withholds From the Plasma

William Alexander Aldred
article en

Abstract

At percolation the false-vacuum fraction is 0.712, and even at the late stage I = 2 more than thirteen percent of space remains unconverted; genuine completion to the one-percent level requires I = 4.5, where the fraction is 0.0111. The withheld shares at percolation are 0.065 of the total energy for a strength of 0.1 and 0.356 for a strength of unity. In other words, an estimate that spends the whole latent heat at percolation overstates the immediately available fluid energy by roughly a third of the latent component in the strong case. The withheld energy is not lost; it arrives as the pockets collapse, which stretches the effective source duration while lowering its early amplitude, a trade that simple one-number amplitude formulae do not represent. This study is simulated and computed from stated assumptions; it is not a measurement.

Zenodo (CERN European Organization for Nuclear Research)
Cosmology and Gravitation Theories
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