cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146557.v1/t14
title: "Supplemental a" of "Trends in Yield and Azimuthal Shape Modification in Dihadron Correlations in Relativistic Heavy Ion Collisions"

description: $p+p$ yield vs $p_T^a$ supplemental tables.
description: BNL-RHIC. Hard-scattered parton probes produced in collisions of large nuclei indicate large partonic energy loss, possibly with collective produced-medium response to the lost energy. We present measurements of $\pi^0$ trigger particles at transverse momenta $p^t_T$ = 4–12 GeV/$c$ and associated charged hadrons ($p^a_T$ = 0.5–7 GeV/$c$) vs. relative azimuthal angle $\Delta \phi$ in Au$\mathord{+}$Au and $p\mathord{+}p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Au$\mathord{+}$Au $\Delta\phi$ distribution at low $p^a_T$, whose shape has been interpreted as a medium effect, is modified for $p^t_T$ $&lt;$ 7 GeV/$c$. At higher $p^t_T$, the data are consistent with unmodified or very weakly modified shapes, even for the lowest measured $p^a_T$, which quantitatively challenges some medium response models. The associated yield of hadrons opposing the trigger particle in Au$\mathord{+}$Au relative to $p\mathord{+}p$ ($I_{AA}$) is suppressed at high $p_T$ ($I_{AA}$ $\approx$ 0.35–0.5), but less than for inclusive suppression ($R_{AA}$ $\approx$ 0.2).
DOI: 10.17182/hepdata.146557.v1/t15
title: "Supplemental b" of "Trends in Yield and Azimuthal Shape Modification in Dihadron Correlations in Relativistic Heavy Ion Collisions"

description: Au+Au yield vs $p_T^a$ supplemental tables.
description: BNL-RHIC. Hard-scattered parton probes produced in collisions of large nuclei indicate large partonic energy loss, possibly with collective produced-medium response to the lost energy. We present measurements of $\pi^0$ trigger particles at transverse momenta $p^t_T$ = 4–12 GeV/$c$ and associated charged hadrons ($p^a_T$ = 0.5–7 GeV/$c$) vs. relative azimuthal angle $\Delta \phi$ in Au$\mathord{+}$Au and $p\mathord{+}p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Au$\mathord{+}$Au $\Delta\phi$ distribution at low $p^a_T$, whose shape has been interpreted as a medium effect, is modified for $p^t_T$ $&lt;$ 7 GeV/$c$. At higher $p^t_T$, the data are consistent with unmodified or very weakly modified shapes, even for the lowest measured $p^a_T$, which quantitatively challenges some medium response models. The associated yield of hadrons opposing the trigger particle in Au$\mathord{+}$Au relative to $p\mathord{+}p$ ($I_{AA}$) is suppressed at high $p_T$ ($I_{AA}$ $\approx$ 0.35–0.5), but less than for inclusive suppression ($R_{AA}$ $\approx$ 0.2).
DOI: 10.17182/hepdata.146557.v1/t16
title: "Supplemental c" of "Trends in Yield and Azimuthal Shape Modification in Dihadron Correlations in Relativistic Heavy Ion Collisions"

description: Au+Au yield vs $p_T^a$ supplemental tables.
description: BNL-RHIC. Hard-scattered parton probes produced in collisions of large nuclei indicate large partonic energy loss, possibly with collective produced-medium response to the lost energy. We present measurements of $\pi^0$ trigger particles at transverse momenta $p^t_T$ = 4–12 GeV/$c$ and associated charged hadrons ($p^a_T$ = 0.5–7 GeV/$c$) vs. relative azimuthal angle $\Delta \phi$ in Au$\mathord{+}$Au and $p\mathord{+}p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The Au$\mathord{+}$Au $\Delta\phi$ distribution at low $p^a_T$, whose shape has been interpreted as a medium effect, is modified for $p^t_T$ $&lt;$ 7 GeV/$c$. At higher $p^t_T$, the data are consistent with unmodified or very weakly modified shapes, even for the lowest measured $p^a_T$, which quantitatively challenges some medium response models. The associated yield of hadrons opposing the trigger particle in Au$\mathord{+}$Au relative to $p\mathord{+}p$ ($I_{AA}$) is suppressed at high $p_T$ ($I_{AA}$ $\approx$ 0.35–0.5), but less than for inclusive suppression ($R_{AA}$ $\approx$ 0.2).
DOI: 10.17182/hepdata.146645.v1/t1
title: "Figure 2" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The cluster reconstruction efficiency, including both DT and CSC clusters, as a function of the simulated r and |z| decay positions of the particle S decaying to $d\bar{d}$ in events with $\it{p}_{T}^\text{miss} &gt;$ 200 GeV, for a mass of 40 GeV and a range of c$\tau$ values uniformly distributed between 1 and 10 m.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t2
title: "Figure 3-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The DT cluster reconstruction efficiency as a function of the simulated r decay positions of S decaying to $d\bar{d}$ in events with $\it{p}_{T}^\text{miss} &gt;$ 200 GeV, for a mass of 40 GeV and a range of c$\tau$ values between 1 and 10 m. The clusters are selected from signal events satisfying the $\it{p}_{T}^\text{miss} &gt;$ 200 GeV requirement.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t3
title: "Figure 3-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The CSC cluster reconstruction efficiency as a function of the simulated |z| decay positions of S decaying to $d\bar{d}$ in events with $\it{p}_{T}^\text{miss} &gt;$ 200 GeV, for a mass of 40 GeV and a range of c$\tau$ values between 1 and 10 m. The clusters are selected from signal events satisfying the $\it{p}_{T}^\text{miss} &gt;$ 200 GeV requirement.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t4
title: "Figure 4" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The geometric acceptance multiplied by the efficiency of the $\it{p}_{T}^\text{miss} &gt;$ 200 GeV selection as a function of the proper decay length c$\tau$ for a scalar particle S with a mass of 40 GeV. The acceptance region for DT is defined by requiring the LLP to decay in the region with |z| &lt; 661 cm and 380 cm &lt; r &lt; 736 cm. The acceptance region for CSC is defined by requiring the LLP decay in the region with $|\eta| &lt; 2.4$, r &lt; 695.5 cm, and 661 cm &lt; |z| &lt; 1100 cm or in the region with $|\eta| &lt; 2.4$, r &lt; 270 cm, and 500 cm &lt; |z| &lt; 661 cm. Single CSC cluster requires exactly one LLP to decay in CSC; Single DT cluster requires exactly one LLP to decay in DT; Double cluster requires both LLP to decay in CSC or DT. The denominator in this plot includes all generated events. The nominator includes events that pass the acceptance requirements above and $\it{p}_{T}^\text{miss} &gt;$ 200 GeV.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t5
title: "Figure 5" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Distributions of the cluster time for signal, where S decaying to $d\bar{d}$ for a proper decay length c$\tau$ of 1 m and mass of 40 GeV, and for a background-enriched sample in data selected by inverting the $N_\text{hits}$ requirement.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t10
title: "Figure 7-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ for single CSC clusters are shown for signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), compared to the shape of background in a selection in which the cluster is not matched to any RPC hit and passes all other selections. The background is dominated by clusters from noise and low-pT particles.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t12
title: "Figure 10-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $N_\text{clusters}$ passing the $N_\text{hits}$ selection in the search region for DT-DT category.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t6
title: "Figure 6-a (signal)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of $N_\text{hits}$ for single CSC clusters are shown for signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m).
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t7
title: "Figure 6-a (background)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of $N_\text{hits}$ for single CSC clusters are shown for compared to the OOT background ($t_\text{clusters} &lt; 12.5$ ns). The OOT background is representative of the overall background shape, because the background passing all the selections described above is dominated by pileup and underlying events.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t8
title: "Figure 6-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ for single CSC clusters are shown for signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), compared to the shape of background in a selection in which the cluster is not matched to any RPC hit and passes all other selections. The background is dominated by clusters from noise and low-pT particles.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t9
title: "Figure 7-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The distributions of $N_\text{hits}$ for single CSC clusters are shown for signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), compared to the shape of background in a selection in which the cluster is not matched to any RPC hit and passes all other selections. The background is dominated by clusters from noise and low-pT particles.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t11
title: "Figure 10-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $N_\text{clusters}$ passing the $N_\text{hits}$ selection in the search region for CSC-CSC category.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t13
title: "Figure 10-c" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $N_\text{clusters}$ passing the $N_\text{hits}$ selection in the search region for DT-CSC category.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t14
title: "Figure 11-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $N_\text{hits}$ in the search region of the single-CSC cluster category are shown. The $N_\text{hits}$ distribution includes only events in bins A and D. The right-hand bin in the Nhits distribution includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t15
title: "Figure 11-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ in the search region of the single-CSC cluster category are shown. The $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ distribution includes only events in bins A and B.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t16
title: "Figure 12-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $N_\text{hits}$ in the search region of the single-DT cluster category are shown. The $N_\text{hits}$ distribution includes only events in bins A and D. The right-hand bin in the Nhits distribution includes overflow events.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t17
title: "Figure 12-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The signal (assuming B(H $\rightarrow$ SS) = 1%, S $\rightarrow d\bar{d}$, and c$\tau$ = 1 m), background, and data distributions of $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ in the search region of the single-DT cluster category are shown. The $\Delta\phi(\it{p}_{T}^\text{miss} \text{,cluster)}$ distribution includes only events in bins A and B.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t18
title: "Figure 13-a (3 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 3 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t19
title: "Figure 13-a (7 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t20
title: "Figure 13-a (15 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t21
title: "Figure 13-a (40 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t22
title: "Figure 13-a (55 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow d\bar{d}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t23
title: "Figure 13-b (0.4 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 0.4 GeV mass and $ S \rightarrow \pi^{0} \pi^{0}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t24
title: "Figure 13-b (1 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 1 GeV mass and $ S \rightarrow \pi^{0} \pi^{0}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t25
title: "Figure 13-c (7 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 7 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t26
title: "Figure 13-c (15 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t27
title: "Figure 13-c (40 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t28
title: "Figure 13-c (55 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow \tau^{+} \tau^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t29
title: "Figure 14-a (15 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 15 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t30
title: "Figure 14-a (40 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 40 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t31
title: "Figure 14-a (55 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 55 GeV mass and $ S \rightarrow b\bar{b}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t32
title: "Figure 14-b (0.4 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 0.4 GeV mass and $ S \rightarrow \pi^{+} \pi^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t33
title: "Figure 14-b (1 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 1 GeV mass and $ S \rightarrow \pi^{+} \pi^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t34
title: "Figure 14-c (1.5 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 1.5 GeV mass and $ S \rightarrow K^{+}K^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t35
title: "Figure 14-d (1.5 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 1.5 GeV mass and $ S \rightarrow K^{0}K^{0}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t37
title: "Figure 14-f (0.4 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 0.4 GeV mass and $ S \rightarrow \e^{+} \e^{-}$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t38
title: "Figure 15-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) as functions of mass and c$\tau$ assuming S inherits all couplings from the Higgs boson evaluated at the LLP mass.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t36
title: "Figure 14-e (0.4 GeV)" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) for 0.4 GeV mass and $ S \rightarrow \gamma\gamma$ decay mode.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t39
title: "Figure 15-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) as functions of mass and c$\tau$ assuming S inherits all couplings from the Higgs boson evaluated at the LLP mass.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t40
title: "Figure 15-c" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) as functions of mass and c$\tau$ assuming S inherits all couplings from the Higgs boson evaluated at the LLP mass.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t41
title: "Figure 16-a" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) as functions of mass and c$\tau$ assuming S inherits all couplings from the Higgs boson evaluated at the LLP mass.
description: No data abstract available.
DOI: 10.17182/hepdata.146645.v1/t42
title: "Figure 16-b" of "Search for long-lived particles decaying in the CMS muon detectors in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The 95% CL observed and expected limits on the branching fraction B(H $\rightarrow$ SS) as functions of mass and c$\tau$ assuming S inherits all couplings from the Higgs boson evaluated at the LLP mass.
description: No data abstract available.