cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.165445.v1/t89
title: "61.d. DT MDS acceptance vs R (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 radial position, 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/t90
title: "61.d. CSC MDS acceptance vs R (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 radial position, 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/t91
title: "62.a. Tracker displaced-jet acceptance vs Z (mH=1000, mX=200)" 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 $m_H=1000\,\mathrm{GeV}$ and $m_X=200\,\mathrm{GeV}$. 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/t92
title: "62.a. ECAL delayed-jet acceptance vs Z (mH=1000, mX=200)" 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 $m_H=1000\,\mathrm{GeV}$ and $m_X=200\,\mathrm{GeV}$. 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/t93
title: "62.a. HCAL displaced-jet acceptance vs Z (mH=1000, mX=200)" 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 $m_H=1000\,\mathrm{GeV}$ and $m_X=200\,\mathrm{GeV}$. 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/t94
title: "62.a. DT MDS acceptance vs Z (mH=1000, mX=200)" 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 $m_H=1000\,\mathrm{GeV}$ and $m_X=200\,\mathrm{GeV}$. 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/t95
title: "62.a. CSC MDS acceptance vs Z (mH=1000, mX=200)" 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 $m_H=1000\,\mathrm{GeV}$ and $m_X=200\,\mathrm{GeV}$. 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/t96
title: "62.b. Tracker displaced-jet acceptance vs Z (mH=350, mX=80)" 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 $m_X=80\,\mathrm{GeV}$. 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/t100
title: "62.b. CSC MDS acceptance vs Z (mH=350, mX=80)" 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 $m_X=80\,\mathrm{GeV}$. 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/t101
title: "62.c. Tracker displaced-jet 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/t102
title: "62.c. ECAL delayed-jet 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/t103
title: "62.c. HCAL displaced-jet 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/t97
title: "62.b. ECAL delayed-jet acceptance vs Z (mH=350, mX=80)" 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 $m_X=80\,\mathrm{GeV}$. 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/t98
title: "62.b. HCAL displaced-jet acceptance vs Z (mH=350, mX=80)" 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 $m_X=80\,\mathrm{GeV}$. 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/t99
title: "62.b. DT MDS acceptance vs Z (mH=350, mX=80)" 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 $m_X=80\,\mathrm{GeV}$. 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 ${\mathrm{fb}}^{-1}$.