1972
DOI: 10.1016/0370-2693(72)90109-8
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Macroscopic consequences of the Weinberg model

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Cited by 778 publications
(461 citation statements)
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“…It is well established after the pioneering work of Kirzhnits and Linde [9] that the electroweak SU(2)×U(1) gauge symmetry was unbroken in the early universe. As the universe cooled down to a temperature of order T ∼ 100 GeV, the thermal expectation value of the Higgs field developed a nonzero value, breaking the electroweak symmetry.…”
Section: The Electroweak Phase Transitionmentioning
confidence: 99%
“…It is well established after the pioneering work of Kirzhnits and Linde [9] that the electroweak SU(2)×U(1) gauge symmetry was unbroken in the early universe. As the universe cooled down to a temperature of order T ∼ 100 GeV, the thermal expectation value of the Higgs field developed a nonzero value, breaking the electroweak symmetry.…”
Section: The Electroweak Phase Transitionmentioning
confidence: 99%
“…Unfortunately the Ginzburg temperature T G of the potential (17) can not be expressed in a simple form, but we can find T G numerically directly from (17) and (22),…”
Section: Electroweak Phase Transitionmentioning
confidence: 99%
“…The φ 3 term arising from gauge boson loops is primarily responsible for the hump in the potential [1,4,25].…”
Section: The 1-loop Effective Potentialmentioning
confidence: 99%
“…In the tadpole method [25,28], V ′ (φ) is calculated from tadpole graphs using Feynman rules in the shifted theory φ =φ + φ ′ , dropping linear terms in …”
Section: The 1-loop Effective Potentialmentioning
confidence: 99%