cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165445.v1/t104
title: "62.c. DT MDS acceptance vs Z (mH=350, mX=160)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=350\,\mathrm{GeV}$ and $m_X=160\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t105
title: "62.c. CSC MDS acceptance vs Z (mH=350, mX=160)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=350\,\mathrm{GeV}$ and $m_X=160\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t106
title: "62.d. Tracker displaced-jet acceptance vs Z (mH=125, mX=25)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=125\,\mathrm{GeV}$ and $m_X=25\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t107
title: "62.d. ECAL delayed-jet acceptance vs Z (mH=125, mX=25)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=125\,\mathrm{GeV}$ and $m_X=25\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t108
title: "62.d. HCAL displaced-jet acceptance vs Z (mH=125, mX=25)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=125\,\mathrm{GeV}$ and $m_X=25\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t109
title: "62.d. DT MDS acceptance vs Z (mH=125, mX=25)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=125\,\mathrm{GeV}$ and $m_X=25\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t110
title: "62.d. CSC MDS acceptance vs Z (mH=125, mX=25)" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptances for various LLP triggers using different subdetectors, as functions of the LLP decay position along the beam line, for $H \to X X \to b\bar{b}\,b\bar{b}$ events for 2023 conditions with $m_H=125\,\mathrm{GeV}$ and $m_X=25\,\mathrm{GeV}$. The $c\tau$ is 0.1\,m for the displaced-jet triggers using the tracker and 1\,m for the other triggers. The acceptance is shown for the displaced-jet triggers using the tracker (cyan points), for the delayed-jet triggers using ECAL timing (red circles), for the displaced-jet triggers using the HCAL (blue squares), for the MDS triggers with the DTs (green triangles), and for the MDS triggers with the CSCs (pink points). The boundaries of the tracker, ECAL, HCAL, DTs, and CSCs are also shown.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t111
title: "63. MDS Run 2, Run 3 acceptance comparison" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Comparison of the acceptances in Run 2 and Run 3 for the CSC (left) and DT (right) MDS triggers at the L1T and HLT as functions of the LLP lifetime, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=125$ GeV and $m_{S}=40$ GeV, for 2023 conditions. The acceptance is defined as the fraction of events that pass the specified selection, given an LLP decay in the fiducial region of the CSCs (left) or DTs (right). The left plot compares the acceptance of the Run 2 strategy of triggering on $p_T^{miss}$ (blue circles), which corresponds to an offline requirement of $&gt;200$ GeV, with that of the Run 3 strategy of triggering on the MDS signature in the CSCs, for both the L1T (L1T+HLT) acceptance is shown with orange squares (red triangles). The right plot compares the acceptance of the Run 2 strategy of triggering on $p_T^{miss}$ (blue circles) with the Run 3 strategy of triggering on the MDS signature in the DTs (red triangles), for L1T+HLT.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t112
title: "64. L1T and L1T+HLT acceptance for CSC MDS" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T (blue circles) and L1T+HLT (orange squares) acceptances for the CSC MDS trigger as functions of the LLP decay positions in the $z$-direction, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=350$ GeV, $m_{S}=80$ GeV, and $c\tau_{S}=1$ m, for 2023 conditions.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t113
title: "65. HLT and L1T+HLT aceptance for DT MDS" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT (blue circles) and L1T+HLT (orange squares) acceptances for the DT MDS trigger as functions of the LLP decay positions in the radial direction, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=350$ GeV, $m_{S}=80$ GeV, and $c\tau_{S}=1$ m, for 2023 conditions.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t114
title: "66.a. 2D L1T acceptance for CSC MDS" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T acceptance for the CSC MDS trigger as functions of the LLP decay position, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=350$ GeV, $m_{S}=80$ GeV, and $c\tau_{S}=1$ m, for 2023 conditions.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t115
title: "66.b. 2D L1T+HLT acceptance for CSC MDS" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptance for the CSC MDS trigger as functions of the LLP decay position, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=350$ GeV, $m_{S}=80$ GeV, and $c\tau_{S}=1$ m, for 2023 conditions.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t116
title: "67. 2D HLT acceptance for DT MDS" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT acceptance for the DT MDS trigger as a function of the LLP decay position, for $H \to S S \to b\bar{{b}}\,b\bar{{b}}$ events with $m_{H}=350$ GeV, $m_{S}=80$ GeV, and $c\tau_{S}=1$ m, for 2023 conditions. The L1T acceptance that is based on the $p_T^{miss}$ trigger is not included.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t117
title: "68. Disp. tau trigger acceptance vs decay vtx radial pos" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT acceptance of the displaced $\tau_\mathrm{h}$ trigger, for simulated $\mathrm{p}\mathrm{p} \to \tilde{\tau}\tilde{\tau},(\tilde{\tau} \to \tau\tilde{\chi}^{0}_{1})$ events,where each $\tau$ decays hadronically and the $\tilde{\tau}$ has a simulated $c\tau$ of 10 cm. The acceptance is shown for the displaced di-$\tau_\mathrm{h}$ trigger path for 2022 data-taking conditions and is plotted with respect to the generator-level $\tau$ lepton decay vertex radial position. Selections on the visible component of the generator-level $\tau$ lepton $\mathrm{p_{T}}$ ($\mathrm{p_{T}}(\tau) &gt; 30$ GeV), its pseudorapidity ($|\eta(\tau)| &lt;$ 2.1), and its decay vertex radial position ($R &lt; $115 cm) are applied.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t118
title: "70.a. HLT muon pt resolution vs pt" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Inverse HLT muon $p_\text{T}$ resolution ($(1/p_\text{T}^\text{HLT}-1/p_\text{T}^\text{gen})/(1/p_\text{T}^\text{gen})$) as a function of the generator-level muon $p_\text{T}$, for simulated HAHM signal events, where the dark Higgs boson ($\text{H}_\text{D}$) mixes with the SM Higgs boson ($\text{H}$) and decays to a pair of long-lived dark photons ($\text{Z}_\text{D}$), for various values of $m_{\text{Z}_\text{D}}$ and $\epsilon$. Conditions for 2022 data-taking are shown. The muons must have $p_\text{T}&gt;10\text{ GeV}$, and the L2 and L3 muons are geometrically matched to the generator-level muons.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t119
title: "70.b. HLT muon pt resolution vs Lxy" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Inverse HLT muon $p_\text{T}$ resolution ($(1/p_\text{T}^\text{HLT}-1/p_\text{T}^\text{gen})/(1/p_\text{T}^\text{gen})$) as a function of the generator-level $L_{xy}$, for simulated HAHM signal events, where the dark Higgs boson ($\text{H}_\text{D}$) mixes with the SM Higgs boson ($\text{H}$) and decays to a pair of long-lived dark photons ($\text{Z}_\text{D}$), for various values of $m_{\text{Z}_\text{D}}$ and $\epsilon$. Conditions for 2022 data-taking are shown. The muons must have $p_\text{T}&gt;10\text{ GeV}$, and the L2 and L3 muons are geometrically matched to the generator-level muons. The dashed vertical lines indicate the radial positions of the layers of the tracking detectors, with BPX, TIB, and TOB denoting the barrel pixel, tracker inner barrel, and tracker outer barrel, respectively.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.