Lepton number violation Higgs decay at muon collider

A bstract In this paper, we consider the scalar singlet extension of type-I seesaw, where a scalar singlet S and a heavy neutral lepton N are further introduced. The Majorana mass term of heavy neutral lepton is generated through the Yukawa interaction with the scalar singlet, which then induces the lepton number violation decays of SM Higgs h and heavy Higgs H via mixing of scalars. As a pathway to probe the origin of heavy neutral lepton mass, we investigate the lepton number violation Higgs decay signature at the TeV- scale muon collider. The dominant production channel of Higgs bosons at the TeV-scale muon collider is via vector boson fusion. So we perform a detailed analysis of the signal process μ + μ − → $$ {\nu}_{\mu }{\overline{\nu}}_{\mu }h/H $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ν</mml:mi> <mml:mi>μ</mml:mi> </mml:msub> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>μ</mml:mi> </mml:msub> <mml:mi>h</mml:mi> <mml:mo>/</mml:mo> <mml:mi>H</mml:mi> </mml:math> → $$ {\nu}_{\mu }{\overline{\nu}}_{\mu } NN $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ν</mml:mi> <mml:mi>μ</mml:mi> </mml:msub> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>μ</mml:mi> </mml:msub> <mml:mi>NN</mml:mi> </mml:math> followed by N → μ ± jj , where the two jets from W boson decay are treated as one fat-jet J . With an integrated luminosity of 1(10) ab −1 , the 3 (10) TeV muon collider could discover the lepton number violation SM Higgs decay h → μ ± μ ± JJ signature for the Higgs mixing parameter sin α &gt; 0 . 05(0 . 009). Meanwhile, a large parameter space can be detected by the lepton number violation heavy Higgs decay H → μ ± μ ± JJ signature for m H ≲ 1(3) TeV and sin α ≳ 0 . 03(0 . 005) at the 3 (10) TeV muon collider. Therefore, the lepton number violation SM and heavy Higgs decay signatures are both promising at the TeV scale muon collider.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-09-24
DOI
https://doi.org/10.1007/jhep09(2025)200
Citations
1
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.87

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article

Lepton number violation Higgs decay at muon collider

Feng-lan Shao, Zhi-Long Han, Fei Huang, Y. Jin et al.
1 citations
Journal of High Energy Physics
Particle physics theoretical and experimental studies
1.87
article

Lepton number violation Higgs decay at muon collider

Feng-lan Shao, Zhi-Long Han, Fei Huang, Y. Jin, F. Yang, Honglei Li
article en
1 citations

Abstract

A bstract In this paper, we consider the scalar singlet extension of type-I seesaw, where a scalar singlet S and a heavy neutral lepton N are further introduced. The Majorana mass term of heavy neutral lepton is generated through the Yukawa interaction with the scalar singlet, which then induces the lepton number violation decays of SM Higgs h and heavy Higgs H via mixing of scalars. As a pathway to probe the origin of heavy neutral lepton mass, we investigate the lepton number violation Higgs decay signature at the TeV- scale muon collider. The dominant production channel of Higgs bosons at the TeV-scale muon collider is via vector boson fusion. So we perform a detailed analysis of the signal process μ + μ − → $$ {\nu}_{\mu }{\overline{\nu}}_{\mu }h/H $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ν</mml:mi> <mml:mi>μ</mml:mi> </mml:msub> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>μ</mml:mi> </mml:msub> <mml:mi>h</mml:mi> <mml:mo>/</mml:mo> <mml:mi>H</mml:mi> </mml:math> → $$ {\nu}_{\mu }{\overline{\nu}}_{\mu } NN $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>ν</mml:mi> <mml:mi>μ</mml:mi> </mml:msub> <mml:msub> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>μ</mml:mi> </mml:msub> <mml:mi>NN</mml:mi> </mml:math> followed by N → μ ± jj , where the two jets from W boson decay are treated as one fat-jet J . With an integrated luminosity of 1(10) ab −1 , the 3 (10) TeV muon collider could discover the lepton number violation SM Higgs decay h → μ ± μ ± JJ signature for the Higgs mixing parameter sin α &gt; 0 . 05(0 . 009). Meanwhile, a large parameter space can be detected by the lepton number violation heavy Higgs decay H → μ ± μ ± JJ signature for m H ≲ 1(3) TeV and sin α ≳ 0 . 03(0 . 005) at the 3 (10) TeV muon collider. Therefore, the lepton number violation SM and heavy Higgs decay signatures are both promising at the TeV scale muon collider.

Journal of High Energy PhysicsVol. 2025(9)
Qufu Normal University (CN), Guangxi Normal University (CN), University of Jinan (CN)
National Natural Science Foundation of China, University of Jinan, Natural Science Foundation of Shandong Province, Nuclear Physics
Openalex Percentile: Top 12%
Particle physics theoretical and experimental studies
1.87
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