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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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arXiv ID2302.11551 (version 2)
Pith IDADJ7KBRB, Pith's permanent record of this paper and its review
CitationHiroto Shibuya, Mayumi Aoki. "Electroweak baryogenesis between broken phases in multi-step phase transition." arXiv:2302.11551 (2023). https://pith.science/paper/ADJ7KBRB
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.24 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.08 · compares with prior results 0.07 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

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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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 0.97 · evidence from simulation or computation 0.60.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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
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7 arXiv papers cite this in 8 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 3 sentences without a confident label

Cites it as background 5 papers

What it cites · 67 sentences without a confident label

Contests 8 papers
Builds on 1 paper
Uses the method or tool of 3 papers
  • 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

  • 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

  • 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
  • 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

  • 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
  • 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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