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Journal ArticleDOI

Perturbative Calculations of Symmetry Breaking

Steven Weinberg
- 15 May 1973 - 
- Vol. 7, Iss: 10, pp 2887-2910
TLDR
In this article, the one-loop contributions to fermion and pseudo-Goldstone masses are calculated for the general class of renormalizable guage theories, and it is shown explicitly that when the masses are subject to any type of zeroth-order symmetry.
Abstract
The one-loop contributions to fermion and pseudo-Goldstone masses are calculated for the general class of renormalizable guage theories. It is shown explicitly that when the masses are subject to any type of zeroth-order symmetry. relation for all values of the parameters in the Lagrangian, the divergences in the one-loop corrections to these symmetry relations cancel. The finite parts of these corrections are evaluated and discussed. Other topics considered include the connection of this work with that of Coleman and E. Weinberg, the constraints obeyed by scalar coupling constants, and the path-integral derivation of the Feynman rules for general renormalizable gauge theories.

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Radiative corrections to the masses of supersymmetric Higgs bosons

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Gauge and Global Symmetries at High Temperature

TL;DR: In this paper, it was shown that a symmetry which is unbroken at low temperature can be broken by raising the temperature above a critical value, which is known as critical temperature.
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Proton stability in grand unified theories, in strings and in branes

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Finite Temperature Quantum Field Theory in Minkowski Space

TL;DR: In this paper, the authors formulate finite-temperature quantum field theories in Minkowski space (real time) using Feynman path integrals and show that at non-zero temperature a new field arises which plays the role of a ghost field and is necessary for unambiguous Feynmann rules.
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Baryon Washout, Electroweak Phase Transition, and Perturbation Theory

TL;DR: In this article, a gauge-independent criterion for baryon number preservation was proposed for electroweak baryogenesis, which is not gauge independent due to the failure of consistently implementing the Nielsen identities order-by-order in perturbation theory.
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