cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.154898.v1/t2
title: "Results P1" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_1$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t3
title: "Results P2" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_2$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t4
title: "Results P3" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_3$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t10
title: "Correlation matrix q2 bin 0" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 1.1 &lt; $q^2$ &lt; 2 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t11
title: "Correlation matrix q2 bin 1" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 2 &lt; $q^2$ &lt; 4.3 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t12
title: "Correlation matrix q2 bin 2" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 4.3 &lt; $q^2$ &lt; 6 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t5
title: "Results P4p" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_4^\prime$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t6
title: "Results P5p" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_5^\prime$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t7
title: "Results P6p" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_6^\prime$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t8
title: "Results P8p" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the $P_8^\prime$ angular observable. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t9
title: "Table 2" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Results for the CP averaged observables $F_L$ and $P_1$–$P_8^\prime$. The first uncertainties are statistical and the second systematic.
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t13
title: "Correlation matrix q2 bin 3" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 6 &lt; $q^2$ &lt; 8.68 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t14
title: "Correlation matrix q2 bin 5" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 10.09 &lt; $q^2$ &lt; 12.86 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.154898.v1/t15
title: "Correlation matrix q2 bin 7" of "Angular analysis of the $B^0\to K^*(892)^0\mu^+\mu^-$ decay in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Correlation matrix of angular observables Fl and P1–P8', considering only the statistical uncertainties from the maximum-likelihood fit in the interval 14.18 &lt; $q^2$ &lt; 16 GeV$^2$
description: CMS at CERN LHC: Angular analysis of the B0 --&gt; K*(892)0 mu+ mu- decay in proton-proton collisions at a centre-of-mass energy of 13 TeV.
DOI: 10.17182/hepdata.155182.v2/t1
title: "SI cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SI cross sections, including sensitivities
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v2/t2
title: "SDn cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SDn cross sections, including sensitivities and nuclear structure uncertainties
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v2/t3
title: "SDp cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SDp cross sections, including sensitivities and nuclear structure uncertainties
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v2/t4
title: "Efficiency" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: Data selection efficiency as a function of nuclear recoil energy
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v2/t5
title: "Data" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: Data points used in analysis in log_10(S2)-S1 space
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v1/t1
title: "SI cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SI cross sections, including sensitivities
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v1/t2
title: "SDn cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SDn cross sections, including sensitivities and nuclear structure uncertainties
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v1/t3
title: "SDp cross section" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: 90% CL WIMP SDp cross sections, including sensitivities and nuclear structure uncertainties
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v1/t4
title: "Efficiency" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: Data selection efficiency as a function of nuclear recoil energy
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155182.v1/t5
title: "Data" of "Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment"

description: Data points used in analysis in log_10(S2)-S1 space
description: Results from a WIMP search with 4.2 tonne-year exposure, using the LUX-ZEPLIN experiment.
DOI: 10.17182/hepdata.155340.v1/t1
title: "Table III: Cross section in energy range 0.62-1.05 GeV" of "Measurement of the $e^+e^- \to \pi^+\pi^-\pi^0$ cross section in the energy range 0.62-3.50 GeV at Belle II"

description: Energy bin range ($\sqrt{s'}$), number of events after unfolding ($N_{\mathrm{unf}}$), corrected efficiency ($\varepsilon$), and cross section ($\sigma_{3\pi}$) for $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ in energy range 0.62--1.05~GeV. The two uncertainties in the cross section are the statistical and systematic contributions. The statistical uncertainties for the unfolding and cross section are square roots of the diagonal components of the unfolding covariance matrix. The image shows Figure 23 in the PRD paper, and the points with error bars indicate the cross section in the table.
description: We report a measurement of the $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ cross section in the energy range from 0.62 to 3.50~GeV using an initial-state radiation technique. We use an $e^{+}e^{-}$ data sample corresponding to 191~fb$^{^-1}$ of integrated luminosity, collected at a center-of-mass energy at or near the $\Upsilon (4S)$ resonance with the \belletwo detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0} \gamma$ events, which involve a $\pi^{0} \to \gamma \gamma$ decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6\% are obtained from several control data samples.The uncertainty on the cross section at the $\omega$ and $\phi$ resonances is dominated by the systematic uncertainty of 2.2\%. The resulting cross sections in the 0.62--1.80~GeV energy range yield $a^{3\pi}_{\mu} = [48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst})] \times 10^{-10}$ for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by $2.5$ standard deviations from the most precise current determination.
DOI: 10.17182/hepdata.155340.v1/t2
title: "Table IV: Cross section in energy range 1.05-3.5 GeV" of "Measurement of the $e^+e^- \to \pi^+\pi^-\pi^0$ cross section in the energy range 0.62-3.50 GeV at Belle II"

description: Energy bin range ($\sqrt{s'}$), number of events after unfolding ($N_{\mathrm{unf}}$), corrected efficiency ($\varepsilon$), and cross section ($\sigma_{3\pi}$) for $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ in energy range 1.05--3.50~GeV. The two uncertainties in the cross section are the statistical and systematic contributions. The statistical uncertainties for the unfolding and cross section are square roots of the diagonal components of the unfolding covariance matrix. The image shows Figure 23 in the PRD paper, and the points with error bars indicate the cross section in the table.
description: We report a measurement of the $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ cross section in the energy range from 0.62 to 3.50~GeV using an initial-state radiation technique. We use an $e^{+}e^{-}$ data sample corresponding to 191~fb$^{^-1}$ of integrated luminosity, collected at a center-of-mass energy at or near the $\Upsilon (4S)$ resonance with the \belletwo detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0} \gamma$ events, which involve a $\pi^{0} \to \gamma \gamma$ decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6\% are obtained from several control data samples.The uncertainty on the cross section at the $\omega$ and $\phi$ resonances is dominated by the systematic uncertainty of 2.2\%. The resulting cross sections in the 0.62--1.80~GeV energy range yield $a^{3\pi}_{\mu} = [48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst})] \times 10^{-10}$ for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by $2.5$ standard deviations from the most precise current determination.
DOI: 10.17182/hepdata.155340.v1/t3
title: "Cross section, statistical covariance" of "Measurement of the $e^+e^- \to \pi^+\pi^-\pi^0$ cross section in the energy range 0.62-3.50 GeV at Belle II"

description: The statistic covariance matrix for the $e^+e^- \to \pi^+ \pi^- \pi^0$ cross section measurement at the Belle II. The 212 x 212 matrix of the energy ranges from 0.62 to 3.50 GeV. This covariance matrix, obtained by propagating the covariance matrix in the unfolding procedure, shows the total statistical uncertainties for the cross section results.
description: We report a measurement of the $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ cross section in the energy range from 0.62 to 3.50~GeV using an initial-state radiation technique. We use an $e^{+}e^{-}$ data sample corresponding to 191~fb$^{^-1}$ of integrated luminosity, collected at a center-of-mass energy at or near the $\Upsilon (4S)$ resonance with the \belletwo detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0} \gamma$ events, which involve a $\pi^{0} \to \gamma \gamma$ decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6\% are obtained from several control data samples.The uncertainty on the cross section at the $\omega$ and $\phi$ resonances is dominated by the systematic uncertainty of 2.2\%. The resulting cross sections in the 0.62--1.80~GeV energy range yield $a^{3\pi}_{\mu} = [48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst})] \times 10^{-10}$ for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by $2.5$ standard deviations from the most precise current determination.
DOI: 10.17182/hepdata.155340.v1/t4
title: "Cross section, systematic covariance" of "Measurement of the $e^+e^- \to \pi^+\pi^-\pi^0$ cross section in the energy range 0.62-3.50 GeV at Belle II"

description: The systematic covariance matrix for the $e^+e^- \to \pi^+ \pi^- \pi^0$ cross section measurement at the Belle II. The 212 x 212 matrix of the energy ranges from 0.62 to 3.50 GeV. This covariance matrix includes all systematic uncertainty given in Table I. The total covariance matrix for the measured cross section can be obtained by adding statistical and systematic covariance matrices.
description: We report a measurement of the $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ cross section in the energy range from 0.62 to 3.50~GeV using an initial-state radiation technique. We use an $e^{+}e^{-}$ data sample corresponding to 191~fb$^{^-1}$ of integrated luminosity, collected at a center-of-mass energy at or near the $\Upsilon (4S)$ resonance with the \belletwo detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0} \gamma$ events, which involve a $\pi^{0} \to \gamma \gamma$ decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6\% are obtained from several control data samples.The uncertainty on the cross section at the $\omega$ and $\phi$ resonances is dominated by the systematic uncertainty of 2.2\%. The resulting cross sections in the 0.62--1.80~GeV energy range yield $a^{3\pi}_{\mu} = [48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst})] \times 10^{-10}$ for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by $2.5$ standard deviations from the most precise current determination.
DOI: 10.17182/hepdata.155340.v1/t5
title: "Cross section, inverse covariance covariance" of "Measurement of the $e^+e^- \to \pi^+\pi^-\pi^0$ cross section in the energy range 0.62-3.50 GeV at Belle II"

description: This table provides the ``inverse'' of the total (stat.+ sys.) covariance matrix. This matrix can be used for a chi-square fit of the mass spectrum. We provide this inverse matrix since special care is needed to take the inverse of the given covariance matrix.
description: We report a measurement of the $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0}$ cross section in the energy range from 0.62 to 3.50~GeV using an initial-state radiation technique. We use an $e^{+}e^{-}$ data sample corresponding to 191~fb$^{^-1}$ of integrated luminosity, collected at a center-of-mass energy at or near the $\Upsilon (4S)$ resonance with the \belletwo detector at the SuperKEKB collider. Signal yields are extracted by fitting the two-photon mass distribution in $e^{+}e^{-} \to \pi^{+} \pi^{-} \pi^{0} \gamma$ events, which involve a $\pi^{0} \to \gamma \gamma$ decay and an energetic photon radiated from the initial state. Signal efficiency corrections with an accuracy of 1.6\% are obtained from several control data samples.The uncertainty on the cross section at the $\omega$ and $\phi$ resonances is dominated by the systematic uncertainty of 2.2\%. The resulting cross sections in the 0.62--1.80~GeV energy range yield $a^{3\pi}_{\mu} = [48.91 \pm 0.23~(\mathrm{stat}) \pm 1.07~(\mathrm{syst})] \times 10^{-10}$ for the leading-order hadronic vacuum polarization contribution to the muon anomalous magnetic moment. This result differs by $2.5$ standard deviations from the most precise current determination.
DOI: 10.17182/hepdata.155341.v1/t1
title: "Figure 6 top left" of "Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Distributions of the $\mathrm{NN^{SvsB}}$ output for data and the expected background after the likelihood fit in the $SR_{ctu ++}$ signal region. The post-fit background expectations are shown as filled histograms, the combined pre-fit background expectations are shown as dashed lines. The signal distribution using the Wilson coefficient values $c_{tu}^{(1)}=0.04$, $c_{Qu}^{(1)}=0.1$, $c_{Qu}^{(8)}=0.1$ is shown with a dotted line, normalized to the same number of events as the background.
description: No data abstract available.
DOI: 10.17182/hepdata.155341.v1/t2
title: "Figure 6 top right" of "Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Distributions of the $\mathrm{NN^{SvsB}}$ output for data and the expected background after the likelihood fit in the $SR_{ctu --}$ signal region. The post-fit background expectations are shown as filled histograms, the combined pre-fit background expectations are shown as dashed lines. The signal distribution using the Wilson coefficient values $c_{tu}^{(1)}=0.04$, $c_{Qu}^{(1)}=0.1$, $c_{Qu}^{(8)}=0.1$ is shown with a dotted line, normalized to the same number of events as the background.
description: No data abstract available.
DOI: 10.17182/hepdata.155341.v1/t3
title: "Figure 6 bottom left" of "Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Distributions of the $\mathrm{NN^{SvsB}}$ output for data and the expected background after the likelihood fit in the $SR_{cQu ++}$ signal region. The post-fit background expectations are shown as filled histograms, the combined pre-fit background expectations are shown as dashed lines. The signal distribution using the Wilson coefficient values $c_{tu}^{(1)}=0.04$, $c_{Qu}^{(1)}=0.1$, $c_{Qu}^{(8)}=0.1$ is shown with a dotted line, normalized to the same number of events as the background.
description: No data abstract available.
DOI: 10.17182/hepdata.155341.v1/t4
title: "Figure 6 bottom right" of "Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Distributions of the $\mathrm{NN^{SvsB}}$ output for data and the expected background after the likelihood fit in the $SR_{cQu --}$ signal region. The post-fit background expectations are shown as filled histograms, the combined pre-fit background expectations are shown as dashed lines. The signal distribution using the Wilson coefficient values $c_{tu}^{(1)}=0.04$, $c_{Qu}^{(1)}=0.1$, $c_{Qu}^{(8)}=0.1$ is shown with a dotted line, normalized to the same number of events as the background.
description: No data abstract available.
DOI: 10.17182/hepdata.155341.v1/t5
title: "Table 3" of "Search for same-charge top-quark pair production in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector"

description: Summary of the observed and predicted number of events in the five 2$\ell$ control regions. The background prediction is shown after the combined likelihood fit to data under the signal-plus-background hypothesis across all control regions and signal regions. The uncertainties in the total yields are smaller than the sum in quadrature of the uncertainties in the individual contributions due to anti-correlations resulting from the likelihood fit. Int Conv refers to events with photon conversions in the inner detector, while Mat Conv refers to events with photon conversions in the detector material. QMisID refers to events with charge-misidentified lepton.
description: No data abstract available.