A Thermal Timeline Through a Bounce: When Each Epoch Occurs, Twice

In a bounce cosmology every thermal epoch of the early universe occurs twice, once during contraction and once during expansion. This paper tabulates the standard epochs with their temperatures and their times from the bounce in the symmetric approximation: the electroweak crossover at 100 GeV occurs 2.34e-11 seconds from the bounce, the QCD transition at 0.15 GeV at 1.37e-05 seconds, neutrino decoupling at 1 MeV at 7.37e-01 seconds, nucleosynthesis at 0.07 MeV at 1.50e+02 seconds, and recombination at 0.26 eV at 1.95e+13 seconds. The doubled timeline matters for baryogenesis because mechanisms keyed to a temperature window get two opportunities, separated by the bounce, but only the second opportunity is safe from later hot eras. The table also fixes the windows in which washout, sphaleron conversion and freeze-out must be scheduled in any bounce baryogenesis model. Computed from stated assumptions, not measured.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-11
DOI
https://doi.org/10.5281/zenodo.24142412
Primary Topic
Cosmology and Gravitation Theories
Type
article
Field-Weighted Citation Impact
0.00
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
article

A Thermal Timeline Through a Bounce: When Each Epoch Occurs, Twice

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

A Thermal Timeline Through a Bounce: When Each Epoch Occurs, Twice

William Alexander Aldred
article en

Abstract

In a bounce cosmology every thermal epoch of the early universe occurs twice, once during contraction and once during expansion. This paper tabulates the standard epochs with their temperatures and their times from the bounce in the symmetric approximation: the electroweak crossover at 100 GeV occurs 2.34e-11 seconds from the bounce, the QCD transition at 0.15 GeV at 1.37e-05 seconds, neutrino decoupling at 1 MeV at 7.37e-01 seconds, nucleosynthesis at 0.07 MeV at 1.50e+02 seconds, and recombination at 0.26 eV at 1.95e+13 seconds. The doubled timeline matters for baryogenesis because mechanisms keyed to a temperature window get two opportunities, separated by the bounce, but only the second opportunity is safe from later hot eras. The table also fixes the windows in which washout, sphaleron conversion and freeze-out must be scheduled in any bounce baryogenesis model. Computed from stated assumptions, not measured.

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

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.

Laika access coming soon