cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.77022.v1/t4
title: "Table 4" of "Search for anomalous Wtb couplings and flavour-changing neutral currents in t-channel single top quark production in pp collisions at sqrt(s) = 7 and 8 TeV"

description: Observed and expected limits for the FCNC couplings at $\sqrt{s}=7$, $8$ TeV, and for combined $7+8$ TeV data.
description: CERN-LHC. 
Limits on anomalous Wtb couplings and search for top quark flavour-changing neural currents using t-channel single top events from proton-proton collision data recorded in 2011 and 2012 with the CMS detector at the LHC at a centre-of-mass energy of 7 and 8 TeV with integrated luminocities of 5.0 and 19.7 /fb respectively and their combination. The final state is one muon and two or three jets. A Bayesian neural network technique, used to discriminate between the signal and backgrounds. The 95% confidence level (CL) exclusion limits on anomalous right-handed vector, and left- and right-handed tensor Wtb couplings are measured to be $|f_{RV}| &lt; 0.16$, $|f_{LT}| &lt; 0.057$, and $-0.049 &lt; f_{RT} &lt; 0.048$, respectively. For the FCNC couplings $\kappa_{tug}$ and $\kappa_{tcg}$, the 95% CL upper limits on coupling strengths are $|\kappa_{tug}|/\Lambda &lt; 4.1 \times 10^{-3} TeV^{-1}$ and $|\kappa_{tcg}|/\Lambda &lt; 1.8 \times 10^{-2} TeV^{-1}$, where $\Lambda$ is the scale for new physics, and correspond to upper limits on the branching fractions of $2.0 \times 10^{-5}$ and $4.1 \times 10^{-4}$ for the decays $t \rightarrow ug$ and $t \rightarrow cg$, respectively.
DOI: 10.17182/hepdata.77022.v1/t5
title: "Table 5" of "Search for anomalous Wtb couplings and flavour-changing neutral currents in t-channel single top quark production in pp collisions at sqrt(s) = 7 and 8 TeV"

description: Observed and expected limits for the FCNC branching ratios at $\sqrt{s}=7$, $8$ TeV, and for combined $7+8$ TeV data.
description: CERN-LHC. 
Limits on anomalous Wtb couplings and search for top quark flavour-changing neural currents using t-channel single top events from proton-proton collision data recorded in 2011 and 2012 with the CMS detector at the LHC at a centre-of-mass energy of 7 and 8 TeV with integrated luminocities of 5.0 and 19.7 /fb respectively and their combination. The final state is one muon and two or three jets. A Bayesian neural network technique, used to discriminate between the signal and backgrounds. The 95% confidence level (CL) exclusion limits on anomalous right-handed vector, and left- and right-handed tensor Wtb couplings are measured to be $|f_{RV}| &lt; 0.16$, $|f_{LT}| &lt; 0.057$, and $-0.049 &lt; f_{RT} &lt; 0.048$, respectively. For the FCNC couplings $\kappa_{tug}$ and $\kappa_{tcg}$, the 95% CL upper limits on coupling strengths are $|\kappa_{tug}|/\Lambda &lt; 4.1 \times 10^{-3} TeV^{-1}$ and $|\kappa_{tcg}|/\Lambda &lt; 1.8 \times 10^{-2} TeV^{-1}$, where $\Lambda$ is the scale for new physics, and correspond to upper limits on the branching fractions of $2.0 \times 10^{-5}$ and $4.1 \times 10^{-4}$ for the decays $t \rightarrow ug$ and $t \rightarrow cg$, respectively.
DOI: 10.17182/hepdata.77033.v1/t1
title: "Table 1" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Unfolded distribution for the inclusive $\Delta|\eta|$ observable in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t2
title: "Table 2" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: Unfolded distribution for the inclusive $\Delta|y|$ observable in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t3
title: "Table 3" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The leptonic inclusive asymmetry in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t4
title: "Table 4" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The leptonic asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t6
title: "Table 6" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The leptonic asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t10
title: "Table 10" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The top-antitop asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t5
title: "Table 5" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The leptonic asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t7
title: "Table 7" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The top-antitop inclusive asymmetry in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t8
title: "Table 8" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The top-antitop asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77033.v1/t9
title: "Table 9" of "Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$ TeV with the ATLAS detector"

description: The top-antitop asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.
description: Measurements of the top--antitop quark pair production charge asymmetry in the dilepton channel are presented using data corresponding to an integrated luminosity of 20.3 $fb^{-1}$ from pp collisions at a center-of-mass energy of $\sqrt{s}=8\,$ TeV collected with the ATLAS detector at the Large Hadron Collider at CERN. Inclusive and differential measurements as a function of the invariant mass, transverse momentum, and longitudinal boost of the $t\bar{t}$ system are performed both in the full phase space and in a fiducial phase space closely matching the detector acceptance. Two observables are studied: $A_{ll}^{C}$ based on the selected leptons and $A_{t\bar{t}}^C$ based on the reconstructed $t\bar{t}$ final state. The inclusive asymmetries are measured in the full phase space to be $A_{ll}^{C} =0.008 \pm 0.006$ and $A_{t\bar{t}}^C = 0.021 \pm 0.016$, which are in agreement with the Standard Model predictions of $A_{ll}^{C} = 0.0064 \pm 0.0003$ and $A_{t\bar{t}}^C = 0.0111 \pm 0.0004$.
DOI: 10.17182/hepdata.77044.v1/t1
title: "Table 1" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the total DIS cross section on C to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t2
title: "Table 2" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the total DIS cross section on C to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t3
title: "Table 3" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the total DIS cross section on C to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t4
title: "Table 4" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the $x$-differential DIS cross section on C to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t5
title: "Table 5" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the $x$-differential DIS cross section on C to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t10
title: "Table 10" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the $x$-differential DIS cross section on Fe to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t6
title: "Table 6" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the $x$-differential DIS cross section on C to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t7
title: "Table 7" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the total DIS cross section on Fe to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t8
title: "Table 8" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the total DIS cross section on Fe to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t9
title: "Table 9" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the total DIS cross section on Fe to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t11
title: "Table 11" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the $x$-differential DIS cross section on Fe to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t12
title: "Table 12" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the $x$-differential DIS cross section on Fe to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t13
title: "Table 13" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the total DIS cross section on Pb to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t14
title: "Table 14" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the total DIS cross section on Pb to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t15
title: "Table 15" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the total DIS cross section on Pb to CH as a function of $E_\nu$.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t17
title: "Table 17" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Statistical error matrix of the ratio of the $x$-differential DIS cross section on Pb to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t16
title: "Table 16" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Ratio of the $x$-differential DIS cross section on Pb to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77044.v1/t18
title: "Table 18" of "Measurement of Partonic Nuclear Effects in Deep-Inelastic Neutrino Scattering using MINERvA"

description: Systematic error matrix of the ratio of the $x$-differential DIS cross section on Pb to CH.
description: Numbers taken from .cc ancillary files provided with arXiv:1601.06313v3.
DOI: 10.17182/hepdata.77045.v1/t1
title: "Table 1" of "Measurement of the forward-backward asymmetry in low-mass bottom-quark pairs produced in proton-antiproton collisions"

description: Results of the $A_{\rm{FB}}$ measurements as functions of $b\bar{b}$ invariant mass. The integral values for each bin are shown.
description: Numbers taken from table 4 of arXiv:1601.06526v1.
DOI: 10.17182/hepdata.77046.v1/t1
title: "Table 1" of "Measurement of the $\phi \to \pi^0 e^+e^-$ transition form factor with the KLOE detector"

description: KLOE measurement of the transition form factor $| F_{\phi \, \pi^0}(q^2) |$ of the $\phi \to \pi^0 e^+e^-$ decay.
description: Numbers taken from table 1 of arXiv:1601.06565v2.
DOI: 10.17182/hepdata.77047.v1/t1
title: "Table 1" of "Study of the reaction $e^+e^- \to \pi^0\gamma$ with the SND detector at the VEPP-2M collider"

description: The c.m.energy ($E$), integrated luminosity ($L$), detection efficiency ($\varepsilon$), number of selected signal events ($N_{\rm sig}$), radiative-correction factor ($1+\delta$), measured Born cross section ($\sigma$). For the cross section the first error is statistical, the second is systematic.
description: Numbers taken from table 2 of arXiv:1601.08061v2.