Washout Survival of a Baryon Asymmetry Across the Hot Phase of a Bounce

An asymmetry produced before or during the hot phase of a bouncing cosmology is partially erased by the same interactions that created it, a process called washout. This paper computes the surviving fraction of an initial baryon yield as a function of a washout strength K and of the duration of the hot phase, which a bounce can lengthen. For weak washout, K = 0.1, the surviving fraction is 0.976; at K = 1 it is 0.785; at K = 10 it falls to 8.84e-02 for a standard hot phase and to 7.81e-03 when the bounce triples that phase; at K = 100 essentially nothing survives, with a fraction of 2.91e-11. The integrated washout at K = 10 is W = 2.43 e-foldings of depletion. The practical result is a survival boundary: production mechanisms operating in the strong-washout regime cannot rely on an asymmetry made before the bounce, whatever its initial size within reasonable bounds. 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.24142341
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

Washout Survival of a Baryon Asymmetry Across the Hot Phase of a Bounce

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

Washout Survival of a Baryon Asymmetry Across the Hot Phase of a Bounce

William Alexander Aldred
article en

Abstract

An asymmetry produced before or during the hot phase of a bouncing cosmology is partially erased by the same interactions that created it, a process called washout. This paper computes the surviving fraction of an initial baryon yield as a function of a washout strength K and of the duration of the hot phase, which a bounce can lengthen. For weak washout, K = 0.1, the surviving fraction is 0.976; at K = 1 it is 0.785; at K = 10 it falls to 8.84e-02 for a standard hot phase and to 7.81e-03 when the bounce triples that phase; at K = 100 essentially nothing survives, with a fraction of 2.91e-11. The integrated washout at K = 10 is W = 2.43 e-foldings of depletion. The practical result is a survival boundary: production mechanisms operating in the strong-washout regime cannot rely on an asymmetry made before the bounce, whatever its initial size within reasonable bounds. 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