Grand-Unified Baryogenesis Checked Against Proton Stability

Grand-unified theories violate baryon number through heavy gauge bosons, and their decays are a classic baryogenesis channel, but the same bosons mediate proton decay, which has never been observed. This paper computes both sides of that tension on one page. The proton lifetime scales as the fourth power of the heavy boson mass: at M_X = 1e15 GeV the estimate is 4.60e+31 years, excluded by the experimental bound of 2.4e34 years; at 1e16 GeV it is 4.60e+35 years, and at 1e17 GeV, 4.60e+39 years. Meeting the bound requires M_X above 4.78e+15 GeV. At an efficiency of 0.1 the decays must carry a CP asymmetry of 9.28e-08 to produce the observed baryon yield. In a bounce history the high production temperature is available on both sides of the bounce, but only expanding-side production escapes subsequent washout and dilution. 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.24142437
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
0.00
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
NOV
article

Grand-Unified Baryogenesis Checked Against Proton Stability

William Alexander Aldred
Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
article

Grand-Unified Baryogenesis Checked Against Proton Stability

William Alexander Aldred
article en

Abstract

Grand-unified theories violate baryon number through heavy gauge bosons, and their decays are a classic baryogenesis channel, but the same bosons mediate proton decay, which has never been observed. This paper computes both sides of that tension on one page. The proton lifetime scales as the fourth power of the heavy boson mass: at M_X = 1e15 GeV the estimate is 4.60e+31 years, excluded by the experimental bound of 2.4e34 years; at 1e16 GeV it is 4.60e+35 years, and at 1e17 GeV, 4.60e+39 years. Meeting the bound requires M_X above 4.78e+15 GeV. At an efficiency of 0.1 the decays must carry a CP asymmetry of 9.28e-08 to produce the observed baryon yield. In a bounce history the high production temperature is available on both sides of the bounce, but only expanding-side production escapes subsequent washout and dilution. Computed from stated assumptions, not measured.

Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
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