Cosmology Concepts Codexery

Electroweak epoch

Epoch when electromagnetism and weak force were unified.

Electroweak epoch

The electroweak epoch was a period in the early universe when the temperature was high enough that electromagnetism and the weak interaction remained unified as a single electroweak interaction, while the strong force had already separated. This epoch is significant because it marks the stage when exotic particles such as W and Z bosons and Higgs bosons were abundantly created, and it ended with an electroweak phase transition whose nature has been clarified by measurements of the Higgs boson mass.

field
Physical cosmology
start_time_disputed
10⁻³⁶ seconds or 10⁻³² seconds after the Big Bang
end_time
Approximately 10⁻¹² seconds after the Big Bang
associated_particles
W and Z bosons, Higgs bosons

Lore & Background

In physical cosmology, the electroweak epoch occurred after the strong force separated from the electronuclear interaction, but while the universe remained hot enough for the electroweak interaction to persist. Some cosmologists place its start at the beginning of the inflationary epoch, about 10⁻³⁶ seconds after the Big Bang; others place it at about 10⁻³² seconds, when the inflaton field's energy was released, creating a dense quark–gluon plasma. During this phase, particle interactions were energetic enough to produce large numbers of W and Z bosons and Higgs bosons.

Reader's Guide

The electroweak epoch is a critical transitional period in the early universe's thermal history. Its significance lies in the fact that it directly preceded the quark epoch and involved the last unification of two fundamental forces—electromagnetism and the weak interaction—before they separated. This means no observable gravitational wave background peaking in the mHz range or electroweak baryogenesis occurs within the Standard Model, though extensions such as supersymmetry may still allow a first-order transition. The epoch thus constrains models of baryogenesis and early-universe physics.

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