cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.150033.v1/t8
title: "Panel 8" of "Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95\% \CL observed upper limits for $\sigma(\PP\to\PhOneTwo\to 2\PaOne) \mathcal{B}^2(\PaOne\to 2\PGm)$ for the NMSSM as a function of $\MPaOne$ for $\MPhOneTwo$ = 90~GEV. The data presented here reflect the results of the 2017 and 2018 datasets combined with the previously published results of the 2016 dataset in \cite{CMS:2018jid}
description: This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{−1}.
This analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 &lt; cτ &lt; 100 mm. - increases luminosity to 60–137 fb^{−1} (was 36 fb^{−1} for HIG-18-003 [2016 data]). - covers a range of 10E−2 &gt; ε &gt; 10E−8 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E−5 &gt; ε &gt; 10E−9). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY
Analysis strategy of this analysis - Data-driven background (BKG) estimation method - Below Υ; Template method [1] - 1DBKGtemplate; TI(µµ1) and TII(µµ2) - 2DBKGtemplate; TI(µµ1)⊗TII(µµ2) - Above Υ; Gaussian kernel-density estimate (KDE) method
DOI: 10.17182/hepdata.150033.v1/t10
title: "Panel 10" of "Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95\% \CL observed upper limits for $\sigma(\PP\to\PhOneTwo\to 2\PaOne) \mathcal{B}^2(\PaOne\to 2\PGm)$ for the NMSSM as a function of $\MPaOne$ for $\MPhOneTwo$ = 150~GEV. The data presented here reflect the results of the 2017 and 2018 datasets combined with the previously published results of the 2016 dataset in \cite{CMS:2018jid}
description: This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{−1}.
This analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 &lt; cτ &lt; 100 mm. - increases luminosity to 60–137 fb^{−1} (was 36 fb^{−1} for HIG-18-003 [2016 data]). - covers a range of 10E−2 &gt; ε &gt; 10E−8 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E−5 &gt; ε &gt; 10E−9). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY
Analysis strategy of this analysis - Data-driven background (BKG) estimation method - Below Υ; Template method [1] - 1DBKGtemplate; TI(µµ1) and TII(µµ2) - 2DBKGtemplate; TI(µµ1)⊗TII(µµ2) - Above Υ; Gaussian kernel-density estimate (KDE) method
DOI: 10.17182/hepdata.150033.v1/t11
title: "Panel 11" of "Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95\% \CL observed upper limits (black solid curves) from this search as interpreted in the dark SUSY scenario for the process $\PP \to \Ph \to 2\nOne \to 2\gammaDark + 2\nDark \to 4\PGm + \PX$, with \mbox{$\MnOne = 60\GeV$} and $\MnDark = 1\GeV$. The limits are presented in the plane of $\varepsilon$ and $\MgammaDark$. The color gradient represents different branching fraction assumptions for \mbox{$\mathcal{B}(\Ph \to 2\nOne \to 2\gammaDark + 2\nDark)$}, ranging from dark orange (0.05\%) to light orange (10\%). The degradation of the limit around 1\GeV is attributed to the drop in the dimuon branching fraction $\mathcal{B}(\gammaDark \to 2\mu)$ due to the dimuon resonance of the $\phi$ meson~\cite{Batell:2009yf}
description: This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{−1}.
This analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 &lt; cτ &lt; 100 mm. - increases luminosity to 60–137 fb^{−1} (was 36 fb^{−1} for HIG-18-003 [2016 data]). - covers a range of 10E−2 &gt; ε &gt; 10E−8 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E−5 &gt; ε &gt; 10E−9). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY
Analysis strategy of this analysis - Data-driven background (BKG) estimation method - Below Υ; Template method [1] - 1DBKGtemplate; TI(µµ1) and TII(µµ2) - 2DBKGtemplate; TI(µµ1)⊗TII(µµ2) - Above Υ; Gaussian kernel-density estimate (KDE) method
DOI: 10.17182/hepdata.150033.v1/t7
title: "Panel 7" of "Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95\% \CL observed upper limits on $\varepsilon^{2} \mathcal{B}(\ZDark \to \sDark \overline{\sDark}) \mathcal{B}^{2}(\sDark \rightarrow 2\PGm)$ for the vector portal model as a function of the dark scalar mass $\MsDark$ and dark vector boson mass $\MZDark$. The yellow and green bands indicate one and two standard deviation values of the limit, respectively. Because the model-independent limits are calculated only up to a dimuon mass of 60\GeV, the \sDark mass considered for these limits is below 60\GeV
description: This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{−1}.
This analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 &lt; cτ &lt; 100 mm. - increases luminosity to 60–137 fb^{−1} (was 36 fb^{−1} for HIG-18-003 [2016 data]). - covers a range of 10E−2 &gt; ε &gt; 10E−8 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E−5 &gt; ε &gt; 10E−9). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY
Analysis strategy of this analysis - Data-driven background (BKG) estimation method - Below Υ; Template method [1] - 1DBKGtemplate; TI(µµ1) and TII(µµ2) - 2DBKGtemplate; TI(µµ1)⊗TII(µµ2) - Above Υ; Gaussian kernel-density estimate (KDE) method
DOI: 10.17182/hepdata.150033.v1/t9
title: "Panel 9" of "Model-independent search for pair production of new bosons decaying into muons in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95\% \CL observed upper limits for $\sigma(\PP\to\PhOneTwo\to 2\PaOne) \mathcal{B}^2(\PaOne\to 2\PGm)$ for the NMSSM as a function of $\MPaOne$ for $\MPhOneTwo$ = 125~GEV. The data presented here reflect the results of the 2017 and 2018 datasets combined with the previously published results of the 2016 dataset in \cite{CMS:2018jid}
description: This analysis (HIG-21-004 [2017+2018 CMS data]) is an extenstion to the search (HIG-18-003 [2016 data]) for new light bosons decaying into muon pairs using data sample corresponding to an integrated luminosity of 35.9 fb^{−1}.
This analysis HIG-21-004 [2017+2018 CMS data] - explores a larger parameter space, dimuon mass from 0.21-60 GeV (was from 0.25-8.5 GeV for HIG-18-003 [2016 data]), with 0 &lt; cτ &lt; 100 mm. - increases luminosity to 60–137 fb^{−1} (was 36 fb^{−1} for HIG-18-003 [2016 data]). - covers a range of 10E−2 &gt; ε &gt; 10E−8 for kinetic mixing in the dark sector, which is complementary to others (EXO-20-014 and EXO-21-006, 10E−5 &gt; ε &gt; 10E−9). - expanded fiducial volume benefit from phase-1 pixel upgrade. - interprets four bench mark models using model-independent limits - Axion-like particle (ALP) - Vector portal - NMSSM - Dark SUSY
Analysis strategy of this analysis - Data-driven background (BKG) estimation method - Below Υ; Template method [1] - 1DBKGtemplate; TI(µµ1) and TII(µµ2) - 2DBKGtemplate; TI(µµ1)⊗TII(µµ2) - Above Υ; Gaussian kernel-density estimate (KDE) method
DOI: 10.17182/hepdata.150034.v1/t1
title: "Prompt Jpsi lambda theta measured in the HX frame" of "Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s}$ = 13 TeV"

description: prompt $\mathrm{J}\mspace{-2mu}/\mspace{-2mu}\psi$ $\lambda_\theta$
description: CERN-LHC-CMS. Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$.
DOI: 10.17182/hepdata.150034.v1/t2
title: "Non prompt Jpsi lambda theta measured in the HX frame" of "Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s}$ = 13 TeV"

description: non prompt $\mathrm{J}\mspace{-2mu}/\mspace{-2mu}\psi$ $\lambda_\theta$
description: CERN-LHC-CMS. Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$.
DOI: 10.17182/hepdata.150034.v1/t3
title: "Prompt psi(2S) lambda theta measured in the HX frame" of "Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s}$ = 13 TeV"

description: prompt $\psi(2S)$ $\lambda_\theta$
description: CERN-LHC-CMS. Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$.
DOI: 10.17182/hepdata.150034.v1/t4
title: "Non prompt psi(2S) lambda theta measured in the HX frame" of "Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s}$ = 13 TeV"

description: non prompt $\psi(2S)$ $\lambda_\theta$
description: CERN-LHC-CMS. Measurement of the polarizations of prompt and non-prompt J/$\psi$ and $\psi$(2S) mesons produced in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$.
DOI: 10.17182/hepdata.150407.v1/t1
title: "Figure 2a" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Fit results for the pair produced merged three-quark average jet mass ($\bar{m}$) distribution, after the selection of $p_{\rm T}&gt;300$ GeV, $|\eta|&lt;2.4$, and $\tau_{32,\mathrm{DDT}}&lt;0$ on both leading and subleading jet and $A_m&lt;0.15$
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t2
title: "Figure 2b" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Fit results for the pair produced merged three-quark average jet mass ($\bar{m}$) distribution, after the selection of $p_{\rm T}&gt;300$ GeV, $|\eta|&lt;2.4$, and $N^1_{2,\mathrm{DDT}}&lt;0$ on both leading and subleading jet
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t3
title: "Figure 3a" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Fit results for the region 1 of pair produced resolved three jet mass ($m_{jjj}$) distribution, after $H_{\rm T}&gt;600$ GeV, $|\eta|&lt;2.4$, sixth jet $p_{\rm T}&gt;40$ GeV, $D^2_{[(6,3)+(3,2)]}&lt;1.25$, $A_m &lt;0.25$, $\Delta&gt;250$ GeV, $D^2_{[3,2]}&lt;0.05$
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t4
title: "Figure 3b" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Fit results for the region 2 of pair produced resolved three jet mass ($m_{jjj}$) distribution, after $H_{\rm T}&gt;600$ GeV, $|\eta|&lt;2.4$, sixth jet $p_{\rm T}&gt;50$ GeV, $D^2_{[(6,3)+(3,2)]}&lt;1.0$, $A_m &lt;0.175$, $\Delta&gt;180$ GeV, $D^2_{[3,2]}&lt;0.175$
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t5
title: "Figure 3c" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Fit results for the region 3 of pair produced resolved three jet mass ($m_{jjj}$) distribution, after $H_{\rm T}&gt;600$ GeV, $|\eta|&lt;2.4$, sixth jet $p_{\rm T}&gt;100$ GeV, $D^2_{[(6,3)+(3,2)]}&lt;0.9$, $A_m &lt;0.15$, $\Delta&gt;150$ GeV, $D^2_{[3,2]}&lt;0.2$
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t6
title: "Figure 4a" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the signal strength for the pair produced merged trijets. Acceptance after the selection $p_{\rm T}&gt;300$ GeV, $|\eta|&lt;2.4$, and $\tau_{32,\mathrm{DDT}}&lt;0$ on both leading and subleading jet and $A_m&lt;0.15$ between the two leading jets.
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t7
title: "Figure 4b" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the signal strength for the pair produced merged dijets. Acceptance after the selection $p_{\rm T}&gt;300$ GeV, $|\eta|&lt;2.4$, and $N^1_{2,\mathrm{DDT}}&lt;0$ on both leading and subleading jet and $A_m&lt;0.15$ between the two leading jets.
description: No data abstract available.
DOI: 10.17182/hepdata.150407.v1/t8
title: "Figure 4c" of "Searches for Pair-Produced Multijet Resonances using Data Scouting in Proton-Proton Collisions at $\sqrt{s}$ = 13 TeV"

description: Expected and observed upper limits on the signal strength for the pair produced resolved trijets (including overlaps). Acceptance for three regions search requions described in table 1 of the paper.
description: No data abstract available.
DOI: 10.17182/hepdata.150507.v1/t1
title: "Scalar LQ signal acceptance times efficiency" of "Search for leptoquark pair production decaying into $te^- \bar{t}e^+$ or $t\mu^- \bar{t}\mu^+$ in multi-lepton final states in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Selection efficiency times acceptance summed over two signal regions for the scalar leptoquark signals as a function of $m_{\mathrm{LQ}_{mix}^{\mathrm{d}}}$, assuming B = 1.
description: A search for leptoquark pair production decaying into $te^-\bar{t}e^+$ or $t\mu^-\bar{t}\mu^+$ in final states with multiple leptons is presented. The search is based on a dataset of $pp$ collisions at $\sqrt{s}$=13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. Events are selected with two or more light leptons (electron or muon) and at least two jets out of which at least one jet is identified as coming from a $b$-hadron. Four signal regions, with the requirement of at least three light leptons, are considered based on the number of leptons of a given flavour. The main background processes are estimated using dedicated control regions in a simultaneous fit with the signal regions to data. No excess above the Standard Model background prediction is observed and 95% confidence level limits on the production cross section times branching ratio are derived as a function of the leptoquark mass. Under the assumption of exclusive decays into $te^-$($t\mu^-$), the corresponding lower limit on the scalar mixed-generation leptoquark mass $m_{LQ_{\mathrm{mix}}^{\mathrm{d}}}$ is at 1.58 (1.59) TeV and on the vector leptoquark mass $m_{\tilde{U}_1}$ at 1.67 (1.67) TeV in the minimal coupling scenario and at 1.95 (1.95) TeV in the Yang-Mills scenario.
DOI: 10.17182/hepdata.150507.v1/t2
title: "Vector LQ signal acceptance times efficiency" of "Search for leptoquark pair production decaying into $te^- \bar{t}e^+$ or $t\mu^- \bar{t}\mu^+$ in multi-lepton final states in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Selection efficiency times acceptance summed over two signal regions for the vector leptoquark signals as a function of $m_{\tilde{U}_{1}}$, assuming B = 1 and Yang-Mills coupling scenario.
description: A search for leptoquark pair production decaying into $te^-\bar{t}e^+$ or $t\mu^-\bar{t}\mu^+$ in final states with multiple leptons is presented. The search is based on a dataset of $pp$ collisions at $\sqrt{s}$=13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. Events are selected with two or more light leptons (electron or muon) and at least two jets out of which at least one jet is identified as coming from a $b$-hadron. Four signal regions, with the requirement of at least three light leptons, are considered based on the number of leptons of a given flavour. The main background processes are estimated using dedicated control regions in a simultaneous fit with the signal regions to data. No excess above the Standard Model background prediction is observed and 95% confidence level limits on the production cross section times branching ratio are derived as a function of the leptoquark mass. Under the assumption of exclusive decays into $te^-$($t\mu^-$), the corresponding lower limit on the scalar mixed-generation leptoquark mass $m_{LQ_{\mathrm{mix}}^{\mathrm{d}}}$ is at 1.58 (1.59) TeV and on the vector leptoquark mass $m_{\tilde{U}_1}$ at 1.67 (1.67) TeV in the minimal coupling scenario and at 1.95 (1.95) TeV in the Yang-Mills scenario.
DOI: 10.17182/hepdata.150507.v1/t4
title: "Cross section upper limit at 95% CL for $t\mu t\mu$" of "Search for leptoquark pair production decaying into $te^- \bar{t}e^+$ or $t\mu^- \bar{t}\mu^+$ in multi-lepton final states in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Summary of the observed and expected 95% CL upper limits on the cross section for $\mathrm{LQ}_{\mathrm{mix}}^{\mathrm{d}}$ pair production as a function of $m_{\mathrm{LQ}_{\mathrm{mix}}^{\mathrm{d}}}$ under the assumptions of B(LQ$\rightarrow t\mu$)=1.
description: A search for leptoquark pair production decaying into $te^-\bar{t}e^+$ or $t\mu^-\bar{t}\mu^+$ in final states with multiple leptons is presented. The search is based on a dataset of $pp$ collisions at $\sqrt{s}$=13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. Events are selected with two or more light leptons (electron or muon) and at least two jets out of which at least one jet is identified as coming from a $b$-hadron. Four signal regions, with the requirement of at least three light leptons, are considered based on the number of leptons of a given flavour. The main background processes are estimated using dedicated control regions in a simultaneous fit with the signal regions to data. No excess above the Standard Model background prediction is observed and 95% confidence level limits on the production cross section times branching ratio are derived as a function of the leptoquark mass. Under the assumption of exclusive decays into $te^-$($t\mu^-$), the corresponding lower limit on the scalar mixed-generation leptoquark mass $m_{LQ_{\mathrm{mix}}^{\mathrm{d}}}$ is at 1.58 (1.59) TeV and on the vector leptoquark mass $m_{\tilde{U}_1}$ at 1.67 (1.67) TeV in the minimal coupling scenario and at 1.95 (1.95) TeV in the Yang-Mills scenario.
DOI: 10.17182/hepdata.150507.v1/t3
title: "Cross section upper limit at 95% CL for $tete$" of "Search for leptoquark pair production decaying into $te^- \bar{t}e^+$ or $t\mu^- \bar{t}\mu^+$ in multi-lepton final states in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Summary of the observed and expected 95% CL upper limits on the cross section for $\mathrm{LQ}_{\mathrm{mix}}^{\mathrm{d}}$ pair production as a function of $m_{\mathrm{LQ}_{\mathrm{mix}}^{\mathrm{d}}}$ under the assumptions of B(LQ$\rightarrow te$)=1.
description: A search for leptoquark pair production decaying into $te^-\bar{t}e^+$ or $t\mu^-\bar{t}\mu^+$ in final states with multiple leptons is presented. The search is based on a dataset of $pp$ collisions at $\sqrt{s}$=13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb$^{-1}$. Events are selected with two or more light leptons (electron or muon) and at least two jets out of which at least one jet is identified as coming from a $b$-hadron. Four signal regions, with the requirement of at least three light leptons, are considered based on the number of leptons of a given flavour. The main background processes are estimated using dedicated control regions in a simultaneous fit with the signal regions to data. No excess above the Standard Model background prediction is observed and 95% confidence level limits on the production cross section times branching ratio are derived as a function of the leptoquark mass. Under the assumption of exclusive decays into $te^-$($t\mu^-$), the corresponding lower limit on the scalar mixed-generation leptoquark mass $m_{LQ_{\mathrm{mix}}^{\mathrm{d}}}$ is at 1.58 (1.59) TeV and on the vector leptoquark mass $m_{\tilde{U}_1}$ at 1.67 (1.67) TeV in the minimal coupling scenario and at 1.95 (1.95) TeV in the Yang-Mills scenario.