cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.149851.v2/t1
title: "Figure 2" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The number of observed events as a function of the number of tracks in the SUEP candidate, for all CRs (A–H) and the SR, as well as two signal samples. The three figures correspond to contiguous $S_{boosted}^{SUEP}$ ranges. The VR is not used in the fit so the estimation comes from the observed values in the control regions. For all other regions and bins, the post-fit values for a background-only fit are shown.
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t2
title: "Figure 4 (observed)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The observed exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t3
title: "Figure 4 (expected)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t4
title: "Figure 4 (Upper 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected upper $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t5
title: "Figure 4 (Lower 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected lower $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t6
title: "Supplementary Figure 2 (top)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The $95\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass $m_{\phi}$ for $m_S = 300$ GeV, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t7
title: "Supplementary Figure 2 (middle)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The $95\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass $m_{\phi}$ for $m_S = 600$ GeV, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t10
title: "Supplementary Figure 3 (expected)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.5$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 40, 40, 20\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t11
title: "Supplementary Figure 3 (Upper 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected upper $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.5$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 40, 40, 20\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t12
title: "Supplementary Figure 3 (Lower 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected lower $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.5$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 40, 40, 20\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t13
title: "Supplementary Figure 4 (observed)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The observed exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.7$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 15, 15, 70\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t8
title: "Supplementary Figure 2 (bottom)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The $95\%$ CL observed upper limits on the cross section shown as a functions of $T_D$ and the pseudoscalar mass $m_{\phi}$ for $m_S = 1000$ GeV, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t9
title: "Supplementary Figure 3 (observed)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The observed exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.5$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 40, 40, 20\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t14
title: "Supplementary Figure 4 (expected)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.7$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 15, 15, 70\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t15
title: "Supplementary Figure 4 (Upper 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected upper $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.7$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 15, 15, 70\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t16
title: "Supplementary Figure 4 (Lower 68)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected lower $68\%$ exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'} = 0.7$ GeV ($A' \rightarrow e^+e^-, \mu^+\mu^-, \pi^+\pi^-$ with $\mathcal{BR} = 15, 15, 70\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v2/t17
title: "Supplementary Table 4" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: For a selection of signal samples in era 2018 with $m_{\phi} = T_D = 3$ GeV, the relative efficiencies and the total efficiency with respect to the selection on the generator-level $H_T$,$H^{gen}_T &gt; 1000$ GeV.
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v1/t1
title: "Figure 2" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The number of observed events as a function of the number of tracks in the SUEP candidate, for all CRs (A–H) and the SR, as well as two signal samples. The three figures correspond to contiguous $S_{boosted}^{SUEP}$ ranges. The VR is not used in the fit so the estimation comes from the observed values in the control regions. For all other regions and bins, the post-fit values for a background-only fit are shown.
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v1/t2
title: "Figure 4 (observed)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The observed exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.
DOI: 10.17182/hepdata.149851.v1/t3
title: "Figure 4 (expected)" of "Search for soft unclustered energy patterns in proton-proton collisions at 13 TeV"

description: The expected exclusions for the nominal $\sigma$ cross section in the plane of $m_{\phi}$ and $T_D$, for various $m_S$ values, for the case $m_{A'}=1.0$ GeV ($A' \rightarrow \pi^+\pi^-$ with $\mathcal{BR}=100\%$).
description: The first search for soft unclustered energy patterns (SUEPs) is performed using an integrated luminosity of 138 $fb^-1$ of proton-proton collision data at $\sqrt{s}=13$ TeV, collected in 2016--2018 by the CMS detector at the LHC. Such SUEPs are predicted by Hidden Valley models with a new, confining force with a large 't Hooft coupling. In events with boosted topologies, selected by high-threshold hadronic triggers, the multiplicity and sphericity of clustered tracks are used to reject the background from standard model quantum chromodynamics. With no observed excess of events over the standard model expectation, limits are set on the cross section for production via gluon fusion of a scalar mediator with SUEP-like decays.