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Electroweak baryogenesis between broken phases in multi-step phase transition
High Energy Physics - Phenomenology · Submitted 22 Feb 2023
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the second step PTs where the sphaleron rate is possible to be un-suppressed before the PTs, which can reproduce the sufficient baryon number asymmetry.
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The abstract, sentence by sentence
Possibility of electroweak baryogenesis (EWBG) via multi-step phase transition (PT) is considered. We investigate the EWBG between $SU(2)$ broken phases in the second step PT of the two-step PT. The produced baryon number asymmetry is evaluated using a prototypical model with a $SU(2)$ charged CP-odd scalar field. We show that the second step PTs where the sphaleron rate is possible to be un-suppressed before the PTs, which can reproduce the sufficient baryon number asymmetry. Our studies can be adapted to models with extra $SU(2)$ scalar fields. We discuss specific models suitable for our scenario.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Possibility of electroweak baryogenesis (EWBG) via multi-step phase transition (PT) is considered. | background 0.73 | 0.34 | 0.05 | hedged possibility 0.94 |
| s1 | We investigate the EWBG between $SU(2)$ broken phases in the second step PT of the two-step PT. | contribution 0.99 | 0.89 | 0.06 | asserted 0.83 |
| s2 | The produced baryon number asymmetry is evaluated using a prototypical model with a $SU(2)$ charged CP-odd scalar field. | method 0.99 | 0.90 | 0.04 | asserted 0.98 |
| s3 | We show that the second step PTs where the sphaleron rate is possible to be un-suppressed before the PTs, which can reproduce the sufficient baryon number asymmetry. | result 0.98 | 0.89 | 0.80 | asserted 0.94 |
| s4 | Our studies can be adapted to models with extra $SU(2)$ scalar fields. | future work 0.75 | 0.45 | 0.04 | hedged possibility 0.63 |
| s5 | We discuss specific models suitable for our scenario. | contribution 0.90 | 0.72 | 0.04 | asserted 0.62 |
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The paper
Original abstract
Possibility of electroweak baryogenesis (EWBG) via multi-step phase transition (PT) is considered. We investigate the EWBG between $SU(2)$ broken phases in the second step PT of the two-step PT. The produced baryon number asymmetry is evaluated using a prototypical model with a $SU(2)$ charged CP-odd scalar field. We show that the second step PTs where the sphaleron rate is possible to be un-suppressed before the PTs, which can reproduce the sufficient baryon number asymmetry. Our studies can be adapted to models with extra $SU(2)$ scalar fields. We discuss specific models suitable for our scenario.
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References
How the literature uses it
7 arXiv papers cite this in 8 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 5 papers
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The two Higgs doublet model (2HDM) is one of the most straightforward extensions of the Higgs sector, in which EWBG has been studied for a long time [ref] .
Electroweak baryogenesis in 2HDM without EDM cancellation · Introduction · 0.93
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In the past few years, multi-step phase transitions were studied in many papers within the loop-corrected effective potential, with a focus on baryogenesis and generation of non-standard spectra of gravitational waves, see for example [ref] and references therein.
Charge-breaking domain walls separating neutral vacua in multi-Higgs models · Phase transitions in multi-Higgs models · 0.80
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The simplest extensions introduce additional scalar fields, such as the real/complex singlet extension [ref] , the two-Higgs-doublet model (2HDM) [ref] , or the $SU(2)$ dark sector [ref] .
Electroweak First-Order Phase Transition Triggered by Non-Gaussian Fluctuations of a $\mathbb{Z}_2$-Symmetric Spectator Scalar · Introduction · 0.96
What it cites · 67 sentences without a confident label
Contests 8 papers
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In contrast to Ref. [ref] , using CosmoTransitions [ref] , we find the PTs where the sphaleron rates before the second step PT would be hardly suppressed.
CosmoTransitions: Computing Cosmological Phase Transition Temperatures and Bubble Profiles with Multiple Fields · Discussions and conclusion · contest 0.75
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In contrast to Ref. [ref] , using CosmoTransitions [ref] , we find the PTs where the sphaleron rates before the second step PT would be hardly suppressed.
Baryon Asymmetry from a Two Stage Electroweak Phase Transition ? · Discussions and conclusion · contest 0.75
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However, Ref. [ref] shows the inaccuracy of the method.] To obtain enough BAU in one-step PT in 2HDMs, a cancellation mechanism for suppressing the electron EDM is necessary [ref] .
Aligned CP-violating Higgs sector canceling the electric dipole moment · Discussions and conclusion · contest 0.77
Builds on 1 paper
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Although Ref. [ref] used the simplified model and PT calculation, we investigate two-step PT in a more general model called the inert doublet model, including loop contributions for the scalar potential.
Baryon Asymmetry from a Two Stage Electroweak Phase Transition ? · Introduction · 0.93
Uses the method or tool of 3 papers
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In order to treat a region where the calculation of $Γ_sph^br$ is not reliable, Ref. [ref] suggested treating the overall sphaleron by introducing the suppression factor $f_sph$ as $Γ_sph^sym f_sph$, where the factor is given by [equation] In this letter, we call the method the CKT prescription.
Electroweak Baryogenesis in Two Higgs Doublet Models and B meson anomalies · Sphaleron rates and baryon asymmetry · 0.99
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The transport equations for the chemical potentials of the top quarks $μ_t$ and $μ_t^c$, left-handed bottom quarks $μ_b$, Higgs doublets $μ_h$, and the relevant plasma velocities $u_k$ ($k=t,b,t^c,h$) in the CK scheme are [ref] [equation]
Electroweak baryogenesis at high wall velocities · Transport equations · 0.94
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The transport equations for the chemical potentials of the top quarks $μ_t$ and $μ_t^c$, left-handed bottom quarks $μ_b$, Higgs doublets $μ_h$, and the relevant plasma velocities $u_k$ ($k=t,b,t^c,h$) in the CK scheme are [ref] [equation]
New benchmark scenarios of electroweak baryogenesis in aligned two Higgs double models · Transport equations · 0.94
Uses data or values from 2 papers
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The sphaleron energy $E_sph$ is given by [ref] [equation] where the constant $B$ is evaluated as the function of $x=m_h/m__W$, [equation] In the SM, the value of $B$ is $B≃1.96$.
Finite temperature field theory and phase transitions · Sphaleron rates and baryon asymmetry · 0.89
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The value of the BAU $η_B≡(n_B-n_B̅)/s$ is observed by the Planck satellite as [ref] [equation] where $n_B (n_B̅)$ is the number density of (anti-)baryon number $n_B (n_B̅)$ and $s$ is the entropy density.
Planck 2018 results. VI. Cosmological parameters · Introduction · 1.00
Compares with 1 paper
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The differences between the schemes are consistent with Ref. [ref] . ] The colors in the plane indicate the produced baryon asymmetries when the second step PT occurs from the point $(w_h, w__CP)$ to the EW vacuum.
Electroweak baryogenesis at high wall velocities · Numerical results · 0.89
Cites as background 42 papers
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Refs. [ref] consider the two-step PT where the second step occurs from the point on the $ϕ_2$ axis to that on the $ϕ_1$ axis.
Two Stage Phase Transition in Two Higgs Models · Discussions and conclusion · 0.87
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Refs. [ref] consider the two-step PT where the second step occurs from the point on the $ϕ_2$ axis to that on the $ϕ_1$ axis.
Baryon Asymmetry from a Two Stage Electroweak Phase Transition ? · Discussions and conclusion · 0.87
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The features of the multi-step PTs are investigated in Refs. [ref] .
Possibility of multi-step electroweak phase transition in the two Higgs doublet models · Introduction · 0.94
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