cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.76732.v1/t6
title: "Table 6" of "Measurement of the $ZZ$ production cross section in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector"

description: The measured differential cross-section normalized to the bin width in values of the leading reconstructed dilepton pT for the 2 lepton, 2 neutrino channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
description: CERN-LHC. Measurements of the cross section for ZZ production using the 4l and 2l2nu decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons, 2 electrons and missing transverse momentum, and 2 muons and missing transverse momentum (MET).

The uncertainty on the global normalisation ("Lumi") is 1.9%. See JHEP 01 (2017) 099 for more details.

 The 4l channel fiducial region is defined as:
 - 4e, 4mu or 2e2mu
 - Ambiguities in pairing are resolved by choosing the combination that results in the smaller value of the sum |mll - mZ| for the two pairs, where mll is the mass of the dilepton system.
 - ptLepton &gt; 7 GeV (at least one with ptLepton &gt; 24 GeV)
 - |etaMuon| &lt;2.7, |etaElectron|&lt;2.5 (for all but one electron), |etaElectron|&lt;4.9 (for at most one electron)
 - Both lepton pairs are required to have invariant mass between 66 and 116 GeV.
 - min(DeltaR(l,l)) &gt; 0.2.

 The 2l2nu channel fiducial region is defined as:
 - 2e+MET or 2mu+MET
 - ptLepton &gt; 25 GeV
 - |etaLepton| &lt; 2.5
 - mll must be between 76 and 106 GeV
 - -MET*cos(phi_METZ)&gt;90 GeV, where phi_METZ is the angle between the Z and the MET
 - |MET - pTZ| / pTZ &lt; 0.4, where pTZ is the transverse momentum of the dilepton system
 - No events with a jet for which ptJet &gt; 25 GeV and |etaJet| &lt; 4.5
 - No events with a third electron (muon) for which ptLepton &gt; 7 (6) GeV
 - min(DeltaR(l,l)) &gt; 0.3
DOI: 10.17182/hepdata.76732.v1/t7
title: "Table 7" of "Measurement of the $ZZ$ production cross section in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector"

description: The measured differential cross-section normalized to the bin width in values of the angle between the dilepton pair for the 2 lepton, 2 neutrino channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
description: CERN-LHC. Measurements of the cross section for ZZ production using the 4l and 2l2nu decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons, 2 electrons and missing transverse momentum, and 2 muons and missing transverse momentum (MET).

The uncertainty on the global normalisation ("Lumi") is 1.9%. See JHEP 01 (2017) 099 for more details.

 The 4l channel fiducial region is defined as:
 - 4e, 4mu or 2e2mu
 - Ambiguities in pairing are resolved by choosing the combination that results in the smaller value of the sum |mll - mZ| for the two pairs, where mll is the mass of the dilepton system.
 - ptLepton &gt; 7 GeV (at least one with ptLepton &gt; 24 GeV)
 - |etaMuon| &lt;2.7, |etaElectron|&lt;2.5 (for all but one electron), |etaElectron|&lt;4.9 (for at most one electron)
 - Both lepton pairs are required to have invariant mass between 66 and 116 GeV.
 - min(DeltaR(l,l)) &gt; 0.2.

 The 2l2nu channel fiducial region is defined as:
 - 2e+MET or 2mu+MET
 - ptLepton &gt; 25 GeV
 - |etaLepton| &lt; 2.5
 - mll must be between 76 and 106 GeV
 - -MET*cos(phi_METZ)&gt;90 GeV, where phi_METZ is the angle between the Z and the MET
 - |MET - pTZ| / pTZ &lt; 0.4, where pTZ is the transverse momentum of the dilepton system
 - No events with a jet for which ptJet &gt; 25 GeV and |etaJet| &lt; 4.5
 - No events with a third electron (muon) for which ptLepton &gt; 7 (6) GeV
 - min(DeltaR(l,l)) &gt; 0.3
DOI: 10.17182/hepdata.76735.v1/t1
title: "Table 1" of "Measurement of the ttbbar production cross section using events in the e mu final state in pp collisions at sqrt(s)=13 TeV"

description: Summary of the individual contributions to the uncertainty in the $\sigma_{t\bar{t}}$ measurement.
description: The cross section of top quark-antiquark pair production in proton-proton collisions at $\sqrt{s}$ = 13 TeV is measured by the CMS experiment at the LHC, using data corresponding to an integrated luminosity of 2.2 inverse femtobarns. The measurement is performed by analyzing events in which the final state includes one electron, one muon, and two or more jets, at least one of which is identified as originating from hadronization of a b quark. The measured cross section is 815 +/- 9 (stat) +/- 38 (syst) +/- 19 (lumi) pb, in agreement with the expectation from the standard model.
DOI: 10.17182/hepdata.76735.v1/t3
title: "Table 3" of "Measurement of the ttbbar production cross section using events in the e mu final state in pp collisions at sqrt(s)=13 TeV"

description: Number of dilepton events obtained after applying the full selection. The results are given for the individual sources of background, $t\bar{t}$ signal with a top quark mass of 172.5 GeV and $\sigma_{t\bar{t}}$ = 832 +/- 46 pb, and data. The uncertainties correspond to statistical and systematic components.
description: The cross section of top quark-antiquark pair production in proton-proton collisions at $\sqrt{s}$ = 13 TeV is measured by the CMS experiment at the LHC, using data corresponding to an integrated luminosity of 2.2 inverse femtobarns. The measurement is performed by analyzing events in which the final state includes one electron, one muon, and two or more jets, at least one of which is identified as originating from hadronization of a b quark. The measured cross section is 815 +/- 9 (stat) +/- 38 (syst) +/- 19 (lumi) pb, in agreement with the expectation from the standard model.
DOI: 10.17182/hepdata.76739.v1/t1
title: "Fiducial cross section" of "Measurement of the WZ production cross section in pp collisions at sqrt(s) = 13 TeV"

description: The fiducial pp to WZ to lnul'l' cross section. The first systematic uncertainty is detector systematics and the second is luminosity uncertainty. The theoretical prediction is calculated with MCFM at NLO with NNPDF3.0 PDFs, with dynamic renormalization and factorization scales set to muR = muF = m[WZ]. The uncertainty is obtained by varying the factorization and renormalization scales independently up and down by a factor of two with the condition that 0.5 &lt; muR/muF &lt; 2.
description: CERN-LHC. The WZ production cross section in proton-proton collisions at sqrt(s) = 13 TeV is measured with the CMS experiment at the LHC using a data sample corresponding to an integrated luminosity of 2.3 inverse fb. The measurement is performed in the leptonic decay modes WZ to l nu l' l', where l, l' = e, mu. The measured cross section for the range 60 &lt; m[l'l'] &lt; 120 GeV is 39.9 +/- 3.2 (stat) +2.9/-3.1 (syst) +/- 0.4 (theo) +/- 1.3 (lumi) pb, consistent with the standard model prediction.

Fiducial region definition
- leading Z lepton pt &gt; 20 GeV
- subleading Z lepton pt &gt; 10 GeV
- W lepton pt &gt; 20 GeV
- lepton |eta| &lt; 2.5
- Z invariant mass between 60 and 120 GeV
- any same-flavor opposite-sign lepton pair invariant mass &gt; 4 GeV

Total cross section region definition
- Z invariant mass between 60 and 120 GeV
- any same-flavor opposite-sign lepton pair invariant mass &gt; 4 GeV
DOI: 10.17182/hepdata.76730.v1/t31
title: "Table 31" of "Measurement of charged-particle distributions sensitive to the underlying event in $\sqrt{s} = 13$ TeV proton-proton collisions with the ATLAS detector at the LHC"

description: Mean charged-particle average transverse momentum as a function of charged-particle multiplicity in trans-min region for trans-min azimuthal region.
description: We present charged-particle distributions sensitive to the underlying event, measured by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV, in low-luminosity Large Hadron Collider fills corresponding to an integrated luminosity of 1.6 nb$^{-1}$. The distributions were constructed using charged particles with absolute pseudorapidity less than 2.5 and with transverse momentum greater than 500 MeV, in events with at least one such charged particle with transverse momentum above 1 GeV. These distributions characterise the angular distribution of energy and particle flows with respect to the charged particle with highest transverse momentum, as a function of both that momentum and of charged-particle multiplicity. The results have been corrected for detector effects and are compared to the predictions of various Monte Carlo event generators, experimentally establishing the level of underlying-event activity at LHC Run 2 energies and providing inputs for the development of event generator modelling. The current models in use for UE modelling typically describe this data to 5% accuracy, compared with data uncertainties of less than 1%.
DOI: 10.17182/hepdata.76730.v1/t32
title: "Table 32" of "Measurement of charged-particle distributions sensitive to the underlying event in $\sqrt{s} = 13$ TeV proton-proton collisions with the ATLAS detector at the LHC"

description: Mean charged-particle average transverse momentum as a function of charged-particle multiplicity in trans-max region for trans-max azimuthal region.
description: We present charged-particle distributions sensitive to the underlying event, measured by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV, in low-luminosity Large Hadron Collider fills corresponding to an integrated luminosity of 1.6 nb$^{-1}$. The distributions were constructed using charged particles with absolute pseudorapidity less than 2.5 and with transverse momentum greater than 500 MeV, in events with at least one such charged particle with transverse momentum above 1 GeV. These distributions characterise the angular distribution of energy and particle flows with respect to the charged particle with highest transverse momentum, as a function of both that momentum and of charged-particle multiplicity. The results have been corrected for detector effects and are compared to the predictions of various Monte Carlo event generators, experimentally establishing the level of underlying-event activity at LHC Run 2 energies and providing inputs for the development of event generator modelling. The current models in use for UE modelling typically describe this data to 5% accuracy, compared with data uncertainties of less than 1%.
DOI: 10.17182/hepdata.76732.v1/t8
title: "Table 8" of "Measurement of the $ZZ$ production cross section in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector"

description: The measured differential cross-section normalized to the bin width in values of the transverse mass of the reconstructed diboson pair for the 2 lepton, 2 neutrino channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
description: CERN-LHC. Measurements of the cross section for ZZ production using the 4l and 2l2nu decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons, 2 electrons and missing transverse momentum, and 2 muons and missing transverse momentum (MET).

The uncertainty on the global normalisation ("Lumi") is 1.9%. See JHEP 01 (2017) 099 for more details.

 The 4l channel fiducial region is defined as:
 - 4e, 4mu or 2e2mu
 - Ambiguities in pairing are resolved by choosing the combination that results in the smaller value of the sum |mll - mZ| for the two pairs, where mll is the mass of the dilepton system.
 - ptLepton &gt; 7 GeV (at least one with ptLepton &gt; 24 GeV)
 - |etaMuon| &lt;2.7, |etaElectron|&lt;2.5 (for all but one electron), |etaElectron|&lt;4.9 (for at most one electron)
 - Both lepton pairs are required to have invariant mass between 66 and 116 GeV.
 - min(DeltaR(l,l)) &gt; 0.2.

 The 2l2nu channel fiducial region is defined as:
 - 2e+MET or 2mu+MET
 - ptLepton &gt; 25 GeV
 - |etaLepton| &lt; 2.5
 - mll must be between 76 and 106 GeV
 - -MET*cos(phi_METZ)&gt;90 GeV, where phi_METZ is the angle between the Z and the MET
 - |MET - pTZ| / pTZ &lt; 0.4, where pTZ is the transverse momentum of the dilepton system
 - No events with a jet for which ptJet &gt; 25 GeV and |etaJet| &lt; 4.5
 - No events with a third electron (muon) for which ptLepton &gt; 7 (6) GeV
 - min(DeltaR(l,l)) &gt; 0.3
DOI: 10.17182/hepdata.76735.v1/t2
title: "Table 2" of "Measurement of the ttbbar production cross section using events in the e mu final state in pp collisions at sqrt(s)=13 TeV"

description: Measurement of the $t\bar{t}$ production cross-section in $pp$ collisions at $\sqrt{s} = 13$ TeV.
description: The cross section of top quark-antiquark pair production in proton-proton collisions at $\sqrt{s}$ = 13 TeV is measured by the CMS experiment at the LHC, using data corresponding to an integrated luminosity of 2.2 inverse femtobarns. The measurement is performed by analyzing events in which the final state includes one electron, one muon, and two or more jets, at least one of which is identified as originating from hadronization of a b quark. The measured cross section is 815 +/- 9 (stat) +/- 38 (syst) +/- 19 (lumi) pb, in agreement with the expectation from the standard model.
DOI: 10.17182/hepdata.76740.v1/t1
title: "Table 1" of "Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$"

description: The values of $\Delta\Gamma_i/\Delta w$ with the statistical and systematic uncertainties in the ${B^0 \to D^- e^+ \nu_{e}}$ and ${B^0 \to D^- \mu^+ \nu_{\mu}}$ sub-samples. The recoil variable, $w$, is defined as the product of the 4-velocities of the $B$ and $D$ mesons. The value of $w_\rm{max}$ is 1.58901 for the sub-samples with a neutral $B$ meson. The $\Delta\Gamma_i/\Delta w$ results are statistically uncorrelated amongst bins and samples. The systematic correlations between bins and samples are given in the file SubsampleResults.csv of the arXiv source.
description: KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\to D\ell\nu_\ell$ ($\ell=e,\mu$) based on 711 fb$^{-1}$ of $e^+e^-\to \Upsilon(4S)$ data recorded by the Belle detector and containing $772 \times 10^6$ $B\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\to D\ell\nu_\ell$ is found to be $\mathcal{B}(B^0 \to D^- \ell^+ \nu_{\ell})=(2.31\pm 0.03(\mathrm{stat})\pm 0.11(\mathrm{syst}))\%$.

UPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).
DOI: 10.17182/hepdata.76732.v1/t2
title: "Table 2" of "Measurement of the $ZZ$ production cross section in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector"

description: The measured differential cross-section normalized to the bin width in values of the leading reconstructed dilepton pT for the 4 lepton channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
description: CERN-LHC. Measurements of the cross section for ZZ production using the 4l and 2l2nu decay channels in proton-proton collisions at a centre-of-mass energy of 8 TeV with 20.3 fb^-1 of data collected in 2012. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons, 2 electrons and missing transverse momentum, and 2 muons and missing transverse momentum (MET).

The uncertainty on the global normalisation ("Lumi") is 1.9%. See JHEP 01 (2017) 099 for more details.

 The 4l channel fiducial region is defined as:
 - 4e, 4mu or 2e2mu
 - Ambiguities in pairing are resolved by choosing the combination that results in the smaller value of the sum |mll - mZ| for the two pairs, where mll is the mass of the dilepton system.
 - ptLepton &gt; 7 GeV (at least one with ptLepton &gt; 24 GeV)
 - |etaMuon| &lt;2.7, |etaElectron|&lt;2.5 (for all but one electron), |etaElectron|&lt;4.9 (for at most one electron)
 - Both lepton pairs are required to have invariant mass between 66 and 116 GeV.
 - min(DeltaR(l,l)) &gt; 0.2.

 The 2l2nu channel fiducial region is defined as:
 - 2e+MET or 2mu+MET
 - ptLepton &gt; 25 GeV
 - |etaLepton| &lt; 2.5
 - mll must be between 76 and 106 GeV
 - -MET*cos(phi_METZ)&gt;90 GeV, where phi_METZ is the angle between the Z and the MET
 - |MET - pTZ| / pTZ &lt; 0.4, where pTZ is the transverse momentum of the dilepton system
 - No events with a jet for which ptJet &gt; 25 GeV and |etaJet| &lt; 4.5
 - No events with a third electron (muon) for which ptLepton &gt; 7 (6) GeV
 - min(DeltaR(l,l)) &gt; 0.3
DOI: 10.17182/hepdata.76740.v1/t2
title: "Table 2" of "Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$"

description: The values of $\Delta\Gamma_i/\Delta w$ with the statistical and systematic uncertainties in the ${B^+ \to \bar{D}^0 e^+ \nu_{e}}$ and ${B^+ \to \bar{D}^0 \mu^+ \nu_{\mu}}$ sub-samples. The recoil variable, $w$, is defined as the product of the 4-velocities of the $B$ and $D$ mesons. The value of $w_\rm{max}$ is 1.59209 for the sub-samples with a charged $B$ meson. The $\Delta\Gamma_i/\Delta w$ results are statistically uncorrelated amongst bins and samples. The systematic correlations between bins and samples are given in the file SubsampleResults.csv of the arXiv source.
description: KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\to D\ell\nu_\ell$ ($\ell=e,\mu$) based on 711 fb$^{-1}$ of $e^+e^-\to \Upsilon(4S)$ data recorded by the Belle detector and containing $772 \times 10^6$ $B\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\to D\ell\nu_\ell$ is found to be $\mathcal{B}(B^0 \to D^- \ell^+ \nu_{\ell})=(2.31\pm 0.03(\mathrm{stat})\pm 0.11(\mathrm{syst}))\%$.

UPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).
DOI: 10.17182/hepdata.76730.v1/t29
title: "Table 29" of "Measurement of charged-particle distributions sensitive to the underlying event in $\sqrt{s} = 13$ TeV proton-proton collisions with the ATLAS detector at the LHC"

description: Mean charged-particle average transverse momentum as a function of $p_\mathrm{T}^\mathrm{lead}$ for toward azimuthal region.
description: We present charged-particle distributions sensitive to the underlying event, measured by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV, in low-luminosity Large Hadron Collider fills corresponding to an integrated luminosity of 1.6 nb$^{-1}$. The distributions were constructed using charged particles with absolute pseudorapidity less than 2.5 and with transverse momentum greater than 500 MeV, in events with at least one such charged particle with transverse momentum above 1 GeV. These distributions characterise the angular distribution of energy and particle flows with respect to the charged particle with highest transverse momentum, as a function of both that momentum and of charged-particle multiplicity. The results have been corrected for detector effects and are compared to the predictions of various Monte Carlo event generators, experimentally establishing the level of underlying-event activity at LHC Run 2 energies and providing inputs for the development of event generator modelling. The current models in use for UE modelling typically describe this data to 5% accuracy, compared with data uncertainties of less than 1%.
DOI: 10.17182/hepdata.76740.v1/t3
title: "Table 3" of "Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$"

description: The values of $\Delta\Gamma_i/\Delta w$ obtained in different bins of $w$ after combination of the ${B^+ \to \bar{D}^0 e^+ \nu_{e}}, {B^+ \to \bar{D}^0 \mu^+ \nu_{\mu}}, {B^0 \to D^- e^+ \nu_{e}},$ and ${B^0 \to D^- \mu^+ \nu_{\mu}}$ sub-samples. The value of $w_\rm{max} = 1.59055$ is the average of the values for charged and neutral $B$ mesons.
description: KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\to D\ell\nu_\ell$ ($\ell=e,\mu$) based on 711 fb$^{-1}$ of $e^+e^-\to \Upsilon(4S)$ data recorded by the Belle detector and containing $772 \times 10^6$ $B\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\to D\ell\nu_\ell$ is found to be $\mathcal{B}(B^0 \to D^- \ell^+ \nu_{\ell})=(2.31\pm 0.03(\mathrm{stat})\pm 0.11(\mathrm{syst}))\%$.

UPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).
DOI: 10.17182/hepdata.76740.v1/t4
title: "Table 4" of "Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$"

description: The correlation matrix of the systematic error. The value of $w_\rm{max} = 1.59055$ is the average of the values for charged and neutral $B$ mesons.
description: KEK-BF. We present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$ using the decay $B\to D\ell\nu_\ell$ ($\ell=e,\mu$) based on 711 fb$^{-1}$ of $e^+e^-\to \Upsilon(4S)$ data recorded by the Belle detector and containing $772 \times 10^6$ $B\bar{B}$ pairs. One $B$ meson in the event is fully reconstructed in a hadronic decay mode while the other, on the signal side, is partially reconstructed from a charged lepton and either a $D^+$ or $D^0$ meson in a total of 23 hadronic decay modes. The isospin-averaged branching fraction of the decay $B\to D\ell\nu_\ell$ is found to be $\mathcal{B}(B^0 \to D^- \ell^+ \nu_{\ell})=(2.31\pm 0.03(\mathrm{stat})\pm 0.11(\mathrm{syst}))\%$.

UPDATE (23 FEB 2017): split Table 1 from paper into two data tables so that $w_\rm{max}$ can be replaced by the numerical value (different for charged and neutral $B$ mesons).