<p>In the model based on gauge group symmetry <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="272" /> </InlineMediaObject> <EquationSource Format="TEX">\(SU(3)_C\times SU(2)_L\times SU(3)_R\times U(1)_X\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <mi>U</mi> <msub> <mrow> <mo stretchy="false">(</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> <mi>C</mi> </msub> <mo>×</mo> <mi>S</mi> <mi>U</mi> <msub> <mrow> <mo stretchy="false">(</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> <mi>L</mi> </msub> <mo>×</mo> <mi>S</mi> <mi>U</mi> <msub> <mrow> <mo stretchy="false">(</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> <mi>R</mi> </msub> <mo>×</mo> <mi>U</mi> <msub> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mi>X</mi> </msub> </mrow> </math></EquationSource> </InlineEquation> (3-2-3-1 model), we study the phenomenology of the standard model–like Higgs boson <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>, which was not considered in previous works (Dong et al., Phys. Rev. D <b>95</b>, 075034, <CitationRef CitationID="CR1">2017</CitationRef>, and Huong et al., Phys. Rev. D <b>98</b>, 055033, <CitationRef CitationID="CR2">2018</CitationRef>). Specifically, we study couplings of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>H</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> with pairs of charged fermions, gauge, charged scalar bosons, and trilinear Higgs boson self-coupling by employing the <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>κ</mi> </math></EquationSource> </InlineEquation>-framework. Based on these parameters, we explore the parameters <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\gamma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mi>γ</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{Z\gamma }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mrow> <mi>Z</mi> <mi>γ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> representing the <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_1\rightarrow \gamma \gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mn>1</mn> </msub> <mo stretchy="false">→</mo> <mi>γ</mi> <mi>γ</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq8.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="72" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_1\rightarrow Z\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mn>1</mn> </msub> <mo stretchy="false">→</mo> <mi>Z</mi> <mi>γ</mi> </mrow> </math></EquationSource> </InlineEquation> decays and find that the model can fulfill both 2<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq9.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sigma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>σ</mi> </math></EquationSource> </InlineEquation> ATLAS and CMS constraints. Besides, new physics effects to lepton flavor-violating (LFV) decays <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq10.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="85" /> </InlineMediaObject> <EquationSource Format="TEX">\(H_1\rightarrow e_a^{\pm }e_b^{\mp }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>H</mi> <mn>1</mn> </msub> <mo stretchy="false">→</mo> <msubsup> <mi>e</mi> <mi>a</mi> <mo>±</mo> </msubsup> <msubsup> <mi>e</mi> <mi>b</mi> <mo>∓</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq11.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(a\ne b\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>≠</mo> <mi>b</mi> </mrow> </math></EquationSource> </InlineEquation>) are also discussed. The result indicates that the lower bound of the new physics scale, <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq12.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \ge 10\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>≥</mo> <mn>10</mn> </mrow> </math></EquationSource> </InlineEquation> TeV, derived from LFV decay limits, is stronger than other constraints <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq13.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \ge 6.6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>≥</mo> <mn>6.6</mn> </mrow> </math></EquationSource> </InlineEquation> TeV (for charge parameter <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq14.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\(q=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>) and <InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq15.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="56" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Lambda \ge 4.6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>≥</mo> <mn>4.6</mn> </mrow> </math></EquationSource> </InlineEquation> TeV (for charge parameter <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1891_Article_IEq16.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(q=-1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>q</mi> <mo>=</mo> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) for electroweak precision tests and FCNCs obtained in Dong et al. (Phys. Rev. D <b>95</b>, 075034, <CitationRef CitationID="CR1">2017</CitationRef>) and Huong et al. (Phys. Rev. D <b>98</b>, 055033, <CitationRef CitationID="CR2">2018</CitationRef>).</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Investigation of Higgs Phenomenology in the 3-2-3-1 Model

  • P. N. Thu

摘要

In the model based on gauge group symmetry \(SU(3)_C\times SU(2)_L\times SU(3)_R\times U(1)_X\) S U ( 3 ) C × S U ( 2 ) L × S U ( 3 ) R × U ( 1 ) X (3-2-3-1 model), we study the phenomenology of the standard model–like Higgs boson \(H_1\) H 1 , which was not considered in previous works (Dong et al., Phys. Rev. D 95, 075034, 2017, and Huong et al., Phys. Rev. D 98, 055033, 2018). Specifically, we study couplings of \(H_1\) H 1 with pairs of charged fermions, gauge, charged scalar bosons, and trilinear Higgs boson self-coupling by employing the \(\kappa \) κ -framework. Based on these parameters, we explore the parameters \(\kappa _{\gamma }\) κ γ and \(\kappa _{Z\gamma }\) κ Z γ representing the \(H_1\rightarrow \gamma \gamma \) H 1 γ γ and \(H_1\rightarrow Z\gamma \) H 1 Z γ decays and find that the model can fulfill both 2 \(\sigma \) σ ATLAS and CMS constraints. Besides, new physics effects to lepton flavor-violating (LFV) decays \(H_1\rightarrow e_a^{\pm }e_b^{\mp }\) H 1 e a ± e b ( \(a\ne b\) a b ) are also discussed. The result indicates that the lower bound of the new physics scale, \(\Lambda \ge 10\) Λ 10 TeV, derived from LFV decay limits, is stronger than other constraints \(\Lambda \ge 6.6\) Λ 6.6 TeV (for charge parameter \(q=0\) q = 0 ) and \(\Lambda \ge 4.6\) Λ 4.6 TeV (for charge parameter \(q=-1\) q = - 1 ) for electroweak precision tests and FCNCs obtained in Dong et al. (Phys. Rev. D 95, 075034, 2017) and Huong et al. (Phys. Rev. D 98, 055033, 2018).