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 |
---|---|
Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.07.2015
Springer Springer Nature B.V |
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Abstract | 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. |
---|---|
AbstractList | (ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image).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, ... at the TeV scale and ... at the 100 GeV scale. The EWPT ... 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...-10... GeV. The EWPT ... is strengthened by only the new bosons; its strength is about 1-1.15 if the mass parts of ..., ... and ... are in the ranges 10-10... GeV. The contributions of ... and ... to the strengths of both EWPTs may make them sufficiently strong to provide large deviations from thermal equilibrium and B violation necessary for baryogenesis. 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, at the TeV scale and at the 100 GeV scale. The EWPT 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 [Formula omitted]-10 GeV. The EWPT is strengthened by only the new bosons; its strength is about 1-1.15 if the mass parts of , and are in the ranges 10-10 GeV. The contributions of and to the strengths of both EWPTs may make them sufficiently strong to provide large deviations from thermal equilibrium and B violation necessary for baryogenesis. 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. |
ArticleNumber | 342 |
Audience | Academic |
Author | Long, Hoang Ngoc Minh, Le Hoang Van, Vo Thanh Phong, Vo Quoc |
Author_xml | – sequence: 1 givenname: Vo Quoc surname: Phong fullname: Phong, Vo Quoc email: vo.quoc.phong.vl@gmail.com organization: Department of Theoretical Physics, Ho Chi Minh City University of Science – sequence: 2 givenname: Hoang Ngoc surname: Long fullname: Long, Hoang Ngoc organization: Institute of Physics, Vietnamese Academy of Science and Technology – sequence: 3 givenname: Vo Thanh surname: Van fullname: Van, Vo Thanh organization: Department of Theoretical Physics, Ho Chi Minh City University of Science – sequence: 4 givenname: Le Hoang surname: Minh fullname: Minh, Le Hoang organization: Department of Theoretical Physics, Ho Chi Minh City University of Science |
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Snippet | 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... 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, at... (ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image) We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that... (ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image).We consider the EWPT in the economical 3-3-1 (E331) model. Our analysis shows that... |
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SubjectTerms | Analysis Astronomy Astrophysics and Cosmology Bosons Cosmology Deviation Economics Electroweak model Elementary Particles Hadrons Heavy Ions Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Phase transformations Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quarks Regular Article - Theoretical Physics Strength String Theory Texts |
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Title | Electroweak phase transition in the economical 3-3-1 model |
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