Aspects of Domain-Wall Standard Model

Desmond Villalba; Digesh Raut; Nobuchika Okada

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Aspects of Domain-Wall Standard Model

Nobuchika Okada, Digesh Raut, Desmond Villalba

High Energy Physics - Phenomenology · Submitted 8 Jan 2018

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We also propose a simple unified picture of localizing all the SM fields.

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What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.13 · human participants 0.02 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.14 · mentions code or data availability 0.02.

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We have recently proposed a setup of the "Domain-Wall Standard Model" in a non-compact 5-dimensional space-time, where all the Standard Model (SM) fields are localized in certain domains of the 5th dimension. While the SM is realized as a 4-dimensional effective theory at low energies, the model involves Kaluza-Klein (KK) modes of the SM particles. In this paper we introduce two simple solvable examples which lead to domain-wall configurations for the SM particles and their KK-modes. Based on the examples, we address a variety of phenomenologies of the Domain-Wall SM, such as the KK-mode gauge boson phenomenology at the Large Hadron Collider (LHC), the effect of the KK-mode SM fermions on Higgs boson phenomenology, and the KK-mode fermion search at the LHC with its decay into a corresponding SM fermion and a Nambu-Goldstone boson associated with a spontaneous breaking of the translational invariance in the 5th dimension. We also propose a simple unified picture of localizing all the SM fields.

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#	sentence	role	the authors' own work	states the main conclusion	strength
s0	We have recently proposed a setup of the "Domain-Wall Standard Model" in a non-compact 5-dimensional space-time, where all the Standard Model (SM) fields are localized in certain domains of the 5th dimension.	background 0.83	0.71	0.10	asserted 1.00
s1	While the SM is realized as a 4-dimensional effective theory at low energies, the model involves Kaluza-Klein (KK) modes of the SM particles.	background 0.98	0.21	0.06	asserted 1.00
s2	In this paper we introduce two simple solvable examples which lead to domain-wall configurations for the SM particles and their KK-modes.	contribution 0.87	0.91	0.11	asserted 1.00
s3	Based on the examples, we address a variety of phenomenologies of the Domain-Wall SM, such as the KK-mode gauge boson phenomenology at the Large Hadron Collider (LHC), the effect of the KK-mode SM fermions on Higgs boson phenomenology, and the KK-mode fermion search at the LHC with its decay into a corresponding SM fermion and a Nambu-Goldstone boson associated with a spontaneous breaking of the translational invariance in the 5th dimension.	contribution 0.97	0.80	0.26	asserted 0.95
s4	We also propose a simple unified picture of localizing all the SM fields.	contribution 1.00	0.88	0.21	asserted 0.90

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.95.

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The paper

Original abstract

We have recently proposed a setup of the "Domain-Wall Standard Model" in a non-compact 5-dimensional space-time, where all the Standard Model (SM) fields are localized in certain domains of the 5th dimension. While the SM is realized as a 4-dimensional effective theory at low energies, the model involves Kaluza-Klein (KK) modes of the SM particles. In this paper we introduce two simple solvable examples which lead to domain-wall configurations for the SM particles and their KK-modes. Based on the examples, we address a variety of phenomenologies of the Domain-Wall SM, such as the KK-mode gauge boson phenomenology at the Large Hadron Collider (LHC), the effect of the KK-mode SM fermions on Higgs boson phenomenology, and the KK-mode fermion search at the LHC with its decay into a corresponding SM fermion and a Nambu-Goldstone boson associated with a spontaneous breaking of the translational invariance in the 5th dimension. We also propose a simple unified picture of localizing all the SM fields.

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6 arXiv papers cite this in 22 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 · 15 sentences without a confident label

Compares with it 1 paper

This is a result of a selection rule in our model.[ Note that a non-derivative coupling $Yψ̅_L^(0) ψ_R^(1)$ from $TΨ̅Ψ$ was recently studied in Ref. [ref] .

Localization of the Standard Model via Higgs mechanism and a finite electroweak monopole from non-compact five dimensions · Translational zero mode · 0.84

Cites it as background 5 papers

Next we briefly review the 5D extension of the Higgs mechanism which is proposed in Refs. [ref] .

Fermion Mass Hierarchy and Phenomenology in the 5D Domain Wall Standard Model · Domain-Wall Higgs Field and Higgs Mechanism · 0.96
A supersymmetric model has been constructed in five spacetime dimensions [ref] , and further developments into unified theories beyond the Standard Model followed [ref] , see also [ref] .

Massless bosons on domain walls: Jackiw-Rebbi-like mechanism for bosonic fields · Introduction · 0.87
Recently, it was proposed that another interesting signature from the localized heavy KK modes of gauge bosons and fermions [ref] , although the presence and/or the number of localized KK modes is more dependent on details of models.

Localization of the Standard Model via Higgs mechanism and a finite electroweak monopole from non-compact five dimensions · Generalized models · 0.80

What it cites · 8 sentences without a confident label

Uses the method or tool of 2 papers

For localizing the gauge field, we adopt a simple way proposed in Ref. [ref] [ We can find that the same idea was discussed elsewhere before Ref. [ref] .

Non-Abelian Gauge Field Localized on Walls with Four-Dimensional World Volume · The gauge sector · 1.00
Note that this structure is analogous to that in spontaneously broken gauge theories, and suggests us to eliminate it by adding a gauge fixing term, which is a 5D analog to the $R_ξ$ gauge [ref] : ℒ_GF=-s/2 ξ(∂_μA^μ- ξ/s ∂_y(s A_y))^2 , where $ξ$ is a gauge parameter.

Domain-Wall Standard Model in non-compact 5D and LHC phenomenology · The gauge sector · 0.84

Uses data or values from 4 papers

The right panel in Figure [ref] shows the signal strength as a function of $m_KK$, along with the LHC constraint of $0.96 ≤μ^γγ ≤1.33$, from the ATLAS and CMS combined analysis [ref] .

Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC $pp$ collision data at $\sqrt{s}=$ 7 and 8 TeV · Higgs boson phenomenology · 0.87
For $m_t=173.34$ GeV [ref] , $m_W=80.4$, and $m_h=125.09$ GeV [ref] , we find $F_1/2(τ_t) ≃1.38$ and $F_1(τ_W) ≃-8.33$.

First combination of Tevatron and LHC measurements of the top-quark mass · Higgs boson phenomenology · 1.00
According to a recent report by the ATLAS collaboration on their search results with luminosities of about 36 fb$^-1$, the lower mass bound on the sequential SM $Z^'$ boson is $m_Z^' ≥4.5$ TeV, which is obtained by the search with dilepton final states [ref] .

Search for new high-mass phenomena in the dilepton final state using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV with the ATLAS detector · Phenomenology of KK-mode gauge bosons · 0.99

Cites as background 1 paper

See, for example, Ref. [ref] , for a pioneering work of this direction.

Gauge-Higgs Unification at LHC · Higgs boson phenomenology · 0.90

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