cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.95354.v1/t33
title: "chargino+chargino acceptances (wino LSP, 2018B)" of "Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Signal acceptance times efficiency ($A\times\epsilon$) for each of the generated chargino masses and lifetimes for $\mathrm{p}\mathrm{p} \rightarrow \widetilde{\chi}^\pm_{1} \widetilde{\chi}^\mp_{1}$ events, in the case of a purely wino neutralino LSP. The denominator for the acceptance is the total number of $\widetilde{\chi}^\pm_{1} \widetilde{\chi}^\mp_{1}$ events generated, while the numerator is the number of those events that are selected by the signal selection after being processed with the same reconstruction software used on the data. These $A\times\epsilon$ values correspond to the conditions simulated for the 2018B data-taking period. The uncertainties are only the statistical uncertainties resulting from the sizes of the generated samples.
description: A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this "disappearing track" signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $101\text{fb}^{-1}$ recorded in 2017 and 2018. The observation of $48$ events is consistent with the estimated background of $47.8 \, _{-2.3}^{+2.7} \, (\text{stat}) \pm 8.1 \, (\text{syst})$ events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At $95\%$ confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below $750$ ($175$) GeV for a lifetime of $3$ ($0.05$) ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015-2018, the most stringent constraints to date. At $95\%$ confidence level, chargino masses in the wino case are excluded below $884$ ($474$) GeV for a lifetime of $3$ ($0.2$) ns.
DOI: 10.17182/hepdata.95354.v1/t34
title: "chargino+neutralino acceptances (wino LSP, 2018B)" of "Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Signal acceptance times efficiency ($A\times\epsilon$) for each of the generated chargino masses and lifetimes for $\mathrm{p}\mathrm{p} \rightarrow \widetilde{\chi}^\pm_{1} \widetilde{\chi}^0_{1}$ events, in the case of a purely wino neutralino LSP. The denominator for the acceptance is the total number of $\widetilde{\chi}^\pm_{1} \widetilde{\chi}^0_{1}$ events generated, while the numerator is the number of those events that are selected by the signal selection after being processed with the same reconstruction software used on the data. These $A\times\epsilon$ values correspond to the conditions simulated for the 2018B data-taking period. The uncertainties are only the statistical uncertainties resulting from the sizes of the generated samples.
description: A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this "disappearing track" signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $101\text{fb}^{-1}$ recorded in 2017 and 2018. The observation of $48$ events is consistent with the estimated background of $47.8 \, _{-2.3}^{+2.7} \, (\text{stat}) \pm 8.1 \, (\text{syst})$ events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At $95\%$ confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below $750$ ($175$) GeV for a lifetime of $3$ ($0.05$) ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015-2018, the most stringent constraints to date. At $95\%$ confidence level, chargino masses in the wino case are excluded below $884$ ($474$) GeV for a lifetime of $3$ ($0.2$) ns.
DOI: 10.17182/hepdata.95354.v1/t35
title: "chargino+chargino acceptances (higgsino LSP, 2018B)" of "Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Signal acceptance times efficiency ($A\times\epsilon$) for each of the generated chargino masses and lifetimes for $\mathrm{p}\mathrm{p} \rightarrow \widetilde{\chi}^\pm_{1} \widetilde{\chi}^\mp_{1}$ events, in the case of a purely higgsino neutralino LSP. The denominator for the acceptance is the total number of $\widetilde{\chi}^\pm_{1} \widetilde{\chi}^\mp_{1}$ events generated, while the numerator is the number of those events that are selected by the signal selection after being processed with the same reconstruction software used on the data. These $A\times\epsilon$ values correspond to the conditions simulated for the 2018B data-taking period. The uncertainties are only the statistical uncertainties resulting from the sizes of the generated samples.
description: A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this "disappearing track" signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $101\text{fb}^{-1}$ recorded in 2017 and 2018. The observation of $48$ events is consistent with the estimated background of $47.8 \, _{-2.3}^{+2.7} \, (\text{stat}) \pm 8.1 \, (\text{syst})$ events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At $95\%$ confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below $750$ ($175$) GeV for a lifetime of $3$ ($0.05$) ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015-2018, the most stringent constraints to date. At $95\%$ confidence level, chargino masses in the wino case are excluded below $884$ ($474$) GeV for a lifetime of $3$ ($0.2$) ns.
DOI: 10.17182/hepdata.95354.v1/t36
title: "chargino+neutralino acceptances (higgsino LSP, 2018B)" of "Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Signal acceptance times efficiency ($A\times\epsilon$) for each of the generated chargino masses and lifetimes for $\mathrm{p}\mathrm{p} \rightarrow \widetilde{\chi}^\pm_{1} \widetilde{\chi}^0_{1,2}$ events, in the case of a purely higgsino neutralino LSP. The denominator for the acceptance is the total number of $\widetilde{\chi}^\pm_{1} \widetilde{\chi}^0_{1,2}$ events generated, while the numerator is the number of those events that are selected by the signal selection after being processed with the same reconstruction software used on the data. These $A\times\epsilon$ values correspond to the conditions simulated for the 2018B data-taking period. The uncertainties are only the statistical uncertainties resulting from the sizes of the generated samples.
description: A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this "disappearing track" signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $101\text{fb}^{-1}$ recorded in 2017 and 2018. The observation of $48$ events is consistent with the estimated background of $47.8 \, _{-2.3}^{+2.7} \, (\text{stat}) \pm 8.1 \, (\text{syst})$ events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At $95\%$ confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below $750$ ($175$) GeV for a lifetime of $3$ ($0.05$) ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015-2018, the most stringent constraints to date. At $95\%$ confidence level, chargino masses in the wino case are excluded below $884$ ($474$) GeV for a lifetime of $3$ ($0.2$) ns.
DOI: 10.17182/hepdata.95354.v1/t37
title: "Estimated backgrounds and observation" of "Search for disappearing tracks in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Summary of the estimated backgrounds and the observation. The first and second uncertainties shown are the statistical and systematic contributions, respectively.
description: A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this "disappearing track" signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of $101\text{fb}^{-1}$ recorded in 2017 and 2018. The observation of $48$ events is consistent with the estimated background of $47.8 \, _{-2.3}^{+2.7} \, (\text{stat}) \pm 8.1 \, (\text{syst})$ events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At $95\%$ confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below $750$ ($175$) GeV for a lifetime of $3$ ($0.05$) ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015-2018, the most stringent constraints to date. At $95\%$ confidence level, chargino masses in the wino case are excluded below $884$ ($474$) GeV for a lifetime of $3$ ($0.2$) ns.
DOI: 10.17182/hepdata.95432.v2/t1
title: "Table 1" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Signal acceptance times selection efficiency as a function of the resonance mass, at various stages of the event selection. From top to bottom: an event pre-selection (trigger, object definitions and $E_{T}^{miss}&gt;10$ GeV) is performed first; the requirements on the di-$\tau$ object and large-$R$ jet detailed in the text are then applied; finally, the $HH$ SR definition must be satisfied.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v1/t1
title: "Table 1" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Signal acceptance times selection efficiency as a function of the resonance mass, at various stages of the event selection. From top to bottom: an event pre-selection (trigger, object definitions and $E_{T}^{miss}&gt;10$ GeV) is performed first; the requirements on the di-$\tau$ object and large-$R$ jet detailed in the text are then applied; finally, the $HH$ SR definition must be satisfied.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v1/t2
title: "Table 2" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Distribution of $m^{vis}_{HH}$ after applying all the event selection that define the $HH$ SR, except the requirement on $m^{vis}_{HH}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. The $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ signal is overlaid for two resonance mass hypotheses with a cross-section set to the expected limit, while all backgrounds are pre-fit. The first and the last bins contains the under-flow and over-flow bin entries, respectively. The hatched bands represent combined statistical and systematic uncertainties.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v1/t3
title: "Table 3" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Event yields of the various estimated backgrounds and data, computed in the signal region of the search for $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. Statistical and systematic uncertainties are quoted. The background yields and uncertainties are pre-fit and are found to be similar to those post-fit.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v2/t2
title: "Table 2" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Distribution of $m^{vis}_{HH}$ after applying all the event selection that define the $HH$ SR, except the requirement on $m^{vis}_{HH}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. The $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$ signal is overlaid for two resonance mass hypotheses with a cross-section set to the expected limit, while all backgrounds are pre-fit. The first and the last bins contains the under-flow and over-flow bin entries, respectively. The hatched bands represent combined statistical and systematic uncertainties.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v2/t3
title: "Table 3" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Event yields of the various estimated backgrounds and data, computed in the signal region of the search for $X\rightarrow HH \rightarrow b\bar{b}\tau^{+}\tau^{-}$. The background labelled as "Others" contains $W$+jets, diboson, $t\bar{t}$ and single-top-quark processes. Statistical and systematic uncertainties are quoted. The background yields and uncertainties are pre-fit and are found to be similar to those post-fit.
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95432.v2/t4
title: "Table 4" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Expected and observed 95% CL upper limits on the production of a heavy, narrow-width, scalar resonance decaying to a pair of Higgs bosons ($X\rightarrow HH$). The final state used in the search consists of a boosted $b\bar{b}$ pair and a boosted hadronically decaying $\tau^{+}\tau^{-}$ pair, and the SM braching ratio of the Higgs boson are assumed. The $\pm 1\sigma$ and $\pm 2\sigma$ variations about the expected limit are indicated by the error bands. Two different requirements are applied on the visible mass of the two boosted Higgs boson candidates for the resonance mass hypotheses of 1.6 TeV and 2.5 TeV, leading to discontinuities in the limits (at 1.6 TeV, the difference between imposing no requirement and $m^{vis}_{HH}&gt;900$ GeV is less than 1% though).
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.15468/dl.4wmgyh
title: Occurrence Download

description: A dataset containing 976 species occurrences available in GBIF matching the query:
{
 "and" : [
 "Geometry POLYGON((-73.20733 42.42832,-73.20733 42.49643,-73.29592 42.49643,-73.29592 42.42832,-73.20733 42.42832))",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "OccurrenceStatus is Present",
 "TaxonKey is Magnoliopsida"
 ]
}

 The dataset includes 976 records from 17 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015795-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.95432.v1/t4
title: "Table 4" of "Reconstruction and identification of boosted di-$\tau$ systems in a search for Higgs boson pairs using 13 TeV proton$-$proton collision data in ATLAS"

description: Expected and observed 95% CL upper limits on the production of a heavy, narrow-width, scalar resonance decaying to a pair of Higgs bosons ($X\rightarrow HH$). The final state used in the search consists of a boosted $b\bar{b}$ pair and a boosted hadronically decaying $\tau^{+}\tau^{-}$ pair, and the SM braching ratio of the Higgs boson are assumed. The $\pm 1\sigma$ and $\pm 2\sigma$ variations about the expected limit are indicated by the error bands. Two different requirements are applied on the visible mass of the two boosted Higgs boson candidates for the resonance mass hypotheses of 1.6 TeV and 2.5 TeV, leading to discontinuities in the limits (at 1.6 TeV, the difference between imposing no requirement and $m^{vis}_{HH}&gt;900$ GeV is less than 1% though).
description: CERN-LHC. A search for resonant Higgs boson pair production is performed in the $b\bar{b}\tau^{+}\tau^{-}$ final state with boosted objects using $L=139$ fb$^{-1}$, $\sqrt{s}=13$ TeV proton-proton collision data with the ATLAS detector. 95% CL upper limits are set on the production cross section of a heavy, narrow, scalar resonance decaying into a pair of Higgs bosons.
DOI: 10.17182/hepdata.95433.v1/t1
title: "Table 1" of "Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Data from paper Table 3. Measured and expected fiducial cross-sections in the ZZjj inclusive fiducial region.
description: CERN LHC. A search for the electroweak (EW) production of two Z bosons in association with 2 jets (j) and constraints on anomalous quartic gauge couplings are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector in 2016-2018 and corresponding to an integrated luminosity of 137.1 fb−1. The search is performed in the fully leptonic final state where the two Z bosons decay to either a pair of electrons or a pair of muons. 
 The inclusive fiducial region is defined as: 
 pt(l) &gt; 20,10,5,5 GeV, |eta(l)|&lt; 2.5 
 60 &lt; m(ll)&lt; 120 GeV, m(4l)&gt;180 GeV 
 pT(j) &gt; 30 GeV, |eta(j)| &lt; 4.7 
 m(jj) &gt; 100 GeV and DeltaR(l,j)&gt;0.4. 
 The VBS-enriched loose selection additionally requires: 
 m(jj) &gt; 400 GeV and DeltaEta(jj)&gt;2.4. 
 The VBS-enriched tight selection additionally requires: 
 m(jj) &gt; 1 TeV and DeltaEta(jj)&gt;2.4.
DOI: 10.17182/hepdata.95433.v1/t2
title: "Table 2" of "Evidence for electroweak production of four charged leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV"

description: Data from paper Table 3. Measured and expected fiducial cross-sections in the VBS-enriched loose fiducial region.
description: CERN LHC. A search for the electroweak (EW) production of two Z bosons in association with 2 jets (j) and constraints on anomalous quartic gauge couplings are presented. The analysis is based on a data sample of proton-proton collisions at √s= 13 TeV collected with the CMS detector in 2016-2018 and corresponding to an integrated luminosity of 137.1 fb−1. The search is performed in the fully leptonic final state where the two Z bosons decay to either a pair of electrons or a pair of muons. 
 The inclusive fiducial region is defined as: 
 pt(l) &gt; 20,10,5,5 GeV, |eta(l)|&lt; 2.5 
 60 &lt; m(ll)&lt; 120 GeV, m(4l)&gt;180 GeV 
 pT(j) &gt; 30 GeV, |eta(j)| &lt; 4.7 
 m(jj) &gt; 100 GeV and DeltaR(l,j)&gt;0.4. 
 The VBS-enriched loose selection additionally requires: 
 m(jj) &gt; 400 GeV and DeltaEta(jj)&gt;2.4. 
 The VBS-enriched tight selection additionally requires: 
 m(jj) &gt; 1 TeV and DeltaEta(jj)&gt;2.4.