Electroweak phase transition in the economical 3-3-1 model
We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that the EWPT in the model is a sequence of two first-order phase transitions, S U ( 3 ) → S U ( 2 ) at the TeV scale and S U ( 2 ) → U ( 1 ) at the 100 GeV scale. The EWPT S U ( 3 ) → S U ( 2 ) is triggered by the new bos...
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Published in | The European physical journal. C, Particles and fields Vol. 75; no. 7; pp. 1 - 13 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.07.2015
Springer Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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Summary: | We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that the EWPT in the model is a sequence of two first-order phase transitions,
S
U
(
3
)
→
S
U
(
2
)
at the TeV scale and
S
U
(
2
)
→
U
(
1
)
at the 100 GeV scale. The EWPT
S
U
(
3
)
→
S
U
(
2
)
is triggered by the new bosons and the exotic quarks; its strength is about 1–13 if the mass ranges of these new particles are 10
2
–10
3
GeV. The EWPT
S
U
(
2
)
→
U
(
1
)
is strengthened by only the new bosons; its strength is about 1–1.15 if the mass parts of
H
1
0
,
H
2
±
and
Y
±
are in the ranges 10–10
2
GeV. The contributions of
H
1
0
and
H
2
±
to the strengths of both EWPTs may make them sufficiently strong to provide large deviations from thermal equilibrium and B violation necessary for baryogenesis. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-015-3550-2 |