<p>We study light neutralinos <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq1.gif" Format="GIF" Height="33" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mfenced close=")" open="("> <msubsup> <mover accent="true"> <mi>χ</mi> <mo stretchy="true">~</mo> </mover> <mn>1</mn> <mn>0</mn> </msubsup> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \left({\overset{\sim }{\chi}}_1^0\right) \)</EquationSource> </InlineEquation> with masses ranging from 10 GeV to several hundred GeV within the framework of R-parity-violating (RPV) supersymmetry. These light neutralinos can be long-lived, decaying with a macroscopic displacement (order cm) inside the LHC main detectors. Complementing previous works on the subject, here we focus on their production through the electroweak pair production of left-chiral sleptons <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="30" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mfenced close=")" open="("> <msub> <mover accent="true"> <mi>e</mi> <mo stretchy="true">~</mo> </mover> <mi>L</mi> </msub> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \left({\tilde{e}}_L\right) \)</EquationSource> </InlineEquation>, with the signal process <i>pp</i> → <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mover accent="true"> <mi>e</mi> <mo stretchy="true">~</mo> </mover> <mi>L</mi> <mo>+</mo> </msubsup> <msubsup> <mover accent="true"> <mi>e</mi> <mo stretchy="true">~</mo> </mover> <mi>L</mi> <mo>−</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\tilde{e}}_L^{+}{\tilde{e}}_L^{-} \)</EquationSource> </InlineEquation> → <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq4.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="70" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>e</mi> <mo>+</mo> </msup> <msubsup> <mover accent="true"> <mi>χ</mi> <mo stretchy="true">~</mo> </mover> <mn>1</mn> <mn>0</mn> </msubsup> <msup> <mi>e</mi> <mo>−</mo> </msup> <msubsup> <mover accent="true"> <mi>χ</mi> <mo stretchy="true">~</mo> </mover> <mn>1</mn> <mn>0</mn> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {e}^{+}{\overset{\sim }{\chi}}_1^0{e}^{-}{\overset{\sim }{\chi}}_1^0 \)</EquationSource> </InlineEquation>. In contrast to the previous study with a singly produced slepton, where the RPV coupling <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>λ</mi> <mn>111</mn> <mo>′</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\lambda}_{111}^{\prime } \)</EquationSource> </InlineEquation> induces <i>both</i> the production and decay of the light neutralino, in our scenario the production proceeds through Drell-Yan-like processes that are essentially independent of RPV couplings. Correspondingly, we implement a displaced-vertex search strategy for which our numerical analysis shows that the high-luminosity LHC can probe <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_27182_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="29" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>λ</mi> <mn>111</mn> <mo>′</mo> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\lambda}_{111}^{\prime } \)</EquationSource> </InlineEquation> values up to three orders of magnitude smaller, and neutralino masses up to about four times larger than those accessible in the previously studied single-slepton production scenario.</p>

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Probing light neutralinos from pair-produced sleptons with displaced vertices at the high-luminosity LHC

  • Giovanna Cottin,
  • Juan Carlos Helo,
  • Fabián Hernández-Pinto,
  • Nicolás A. Neill,
  • Zeren Simon Wang

摘要

We study light neutralinos χ ~ 1 0 \( \left({\overset{\sim }{\chi}}_1^0\right) \) with masses ranging from 10 GeV to several hundred GeV within the framework of R-parity-violating (RPV) supersymmetry. These light neutralinos can be long-lived, decaying with a macroscopic displacement (order cm) inside the LHC main detectors. Complementing previous works on the subject, here we focus on their production through the electroweak pair production of left-chiral sleptons e ~ L \( \left({\tilde{e}}_L\right) \) , with the signal process pp e ~ L + e ~ L \( {\tilde{e}}_L^{+}{\tilde{e}}_L^{-} \) e + χ ~ 1 0 e χ ~ 1 0 \( {e}^{+}{\overset{\sim }{\chi}}_1^0{e}^{-}{\overset{\sim }{\chi}}_1^0 \) . In contrast to the previous study with a singly produced slepton, where the RPV coupling λ 111 \( {\lambda}_{111}^{\prime } \) induces both the production and decay of the light neutralino, in our scenario the production proceeds through Drell-Yan-like processes that are essentially independent of RPV couplings. Correspondingly, we implement a displaced-vertex search strategy for which our numerical analysis shows that the high-luminosity LHC can probe λ 111 \( {\lambda}_{111}^{\prime } \) values up to three orders of magnitude smaller, and neutralino masses up to about four times larger than those accessible in the previously studied single-slepton production scenario.