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A non-perturbative analysis of the finite-T phase transition in SU (2) × U (1) electroweak theory

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Kajantie, K., Laine, M., Rummukainen, K., Shaposhnikov, M.·1997·Nuclear Physics B

Abstract

The continuum 3d SU(2)×U(1)+Higgs theory is an effective theory for a large class of 4d high-temperature gauge theories, including the minimal standard model and some of its supersymmetric extensions. We study the effects of the U(1) subgroup using lattice Monte Carlo techniques. When g ′2 /g 2 is increased from the zero corresponding to pure SU(2)+Higgs theory, the phase transition gets stronger. However, the increase in the strength is close to what is expected perturbatively, and the qualitative features of the phase diagram remain the same as for g ′2 = 0. In particular, the first order transition still disappears for mH > mH,c. We measure the photon mass and mixing angle, and find that the mass vanishes in both phases within the statistical errors.

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Metadata

Authors
Kajantie, K., Laine, M., Rummukainen, K., & Shaposhnikov, M.
Venue
Nuclear Physics B
Publisher
Elsevier BV
Published
1997-05
Volume
493
Issue
1-2
Pages
413-438
ISSN
0550-3213 (ISSN-L)
OpenAlex
W2131596340
Cited by
268
References
0
FWCI
11.75
Type
journal article
Language
en
Open access
green

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CoChat. (2026). Citation check: A non-perturbative analysis of the finite-T phase transition in SU (2) × U (1) electroweak theory. https://app.cochat.ai/papers/10.1016/s0550-3213(97)00164-8
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Kajantie, K., Laine, M., Rummukainen, K., & Shaposhnikov, M. (1997). A non-perturbative analysis of the finite-T phase transition in SU (2) × U (1) electroweak theory. Nuclear Physics B. https://doi.org/10.1016/s0550-3213(97)00164-8

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