cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83964.v1/t5
title: "Table 5" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Nuclear modification factor R_AA of $\pi^{0}$ produced in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.25% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83964.v1/t6
title: "Table 6" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Nuclear modification factor R_AA of $\pi^{0}$ produced in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.3% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83964.v1/t10
title: "Table 10" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Ratio of the $\eta$ to $\pi^{0}$ invariant yields in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83964.v1/t7
title: "Table 7" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Nuclear modification factor R_AA of $\eta$ produced in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.25% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83964.v1/t8
title: "Table 8" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Nuclear modification factor R_AA of $\eta$ produced in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.3% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83964.v1/t9
title: "Table 9" of "Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV"

description: Ratio of the $\eta$ to $\pi^{0}$ invariant yields in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity.
description: CERN-LHC. Neutral pion and $\eta$ meson production in the transverse momentum range 1 $&lt; p_{\rm T} &lt;$ 20 GeV/$c$ have been measured at midrapidity by the ALICE experiment at the Large Hadron Collider (LHC) in central and semi-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV. These results extend the $p_{\rm T}$ reach of the previous ALICE PI0 measurements from 12 GeV/$c$ to 20 GeV/$c$ and present the first measurement of the ETA meson in heavy-ion collisions at the LHC. The $\eta$ to $\pi^{0}$ ratio is similar for the two centralities and reaches a plateau value of 0.457 $\pm$ 0.013$^{stat}$ $\pm$ 0.018$^{syst}$. A suppression of the same magnitude for $\pi^{0}$ and $\eta$ meson production is observed in Pb-Pb collisions with respect to their production in pp collisions scaled by the number of binary nucleon-nucleon collisions. For both mesons, the nuclear modification factor $R_{\rm AA}$ reaches a minimum at $p_{\rm T} \approx $ 7 GeV/$c$ and then increases with transverse momentum. The measurements show a stronger suppression with respect to what was observed at lower center-of-mass energies in the $p_{\rm T}$ range 6 $&lt; p_{\rm T} &lt;$ 10 GeV/$c$. The results are compared with statistical hadronization models at low-$p_{\rm T}$ and with NLO pQCD jet quenching predictions at high-$p_{\rm T}$.
DOI: 10.17182/hepdata.83965.v1/t1
title: "Table 1" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured integrated cross sections for the $Z\gamma$ process for neutrino final states at $\sqrt{s} = 13$ TeV in the extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t2
title: "Table 2" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured differential cross sections for the $pp \rightarrow \nu\bar{\nu}\gamma$ process at $\sqrt{s} = 13$ TeV as a function of photon $E_{T}$ in the inclusive $N_{jets} \geq 0$ extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t3
title: "Table 3" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured differential cross sections for the $pp \rightarrow \nu\bar{\nu}\gamma$ process at $\sqrt{s} = 13$ TeV as a function of photon $E_{T}$ in the exclusive $N_{jets} = 0$ extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t4
title: "Table 4" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured differential cross sections for the $pp \rightarrow \nu\bar{\nu}\gamma$ process as a function of $p_{T}^{\nu\bar{\nu}}$ in the inclusive $N_{jets} \geq 0$ extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t5
title: "Table 5" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured differential cross sections for the $pp \rightarrow \nu\bar{\nu}\gamma$ process as a function of $p_{T}^{\nu\bar{\nu}}$ in the exclusive $N_{jets} = 0$ extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t6
title: "Table 6" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Measured differential cross sections as a function of $N_{jets}$ in the extended fiducial region defined in the paper.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t7
title: "Table 7" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Observed and expected one dimensional 95% C.L. limits on vertex function parameters for the $ZZ\gamma$ and $Z\gamma\gamma$ vertices.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.
DOI: 10.17182/hepdata.83965.v1/t8
title: "Table 8" of "Measurement of the $ Z\gamma \to \nu \overline{\nu}\gamma $ production cross section in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings"

description: Observed and expected one dimensional 95% C.L. limits on EFT parameters for the $ZZ\gamma$ and $Z\gamma\gamma$ vertices.
description: CERN-LHC. The production of $Z$ bosons in association with a high energy photon ($Z\gamma$ production) is studied in the neutrino decay channel of the $Z$ boson using $pp$ collisions at $\sqrt{s}$ = 13 TeV. The analysis uses a data sample with an integrated luminosity of 36.1~fb$^{-1}$ collected by the ATLAS detector in 2015 and 2016. $Z\gamma$ events with invisible decays of the $Z$ boson are selected by requiring significant missing transverse energy ($E_{\mathrm{T}}^{\mathrm{miss}}$) in conjunction with a single isolated photon with large transverse energy ($E_{\mathrm{T}}$). The rate of $Z\gamma$ production is measured as a function of photon $E_{\mathrm{T}}$, $E_{\mathrm{T}}^{\mathrm{miss}}$ and jet multiplicity. Evidence for anomalous triple gauge coupling is sought in $Z\gamma$ production with photon $E_{\mathrm{T}}$ greater than 600 GeV. No excess is observed relative to the Standard Model expectation, and upper limits are set on the strength of $ZZ\gamma$ and $Z\gamma\gamma$ couplings.

The extended fiducial region is defined as:
- ptPhoton &gt; 150 GeV 
- ptNuNubar &gt; 150 GeV
- |etaPhoton| &lt; 2.37
- ptJet &gt; 50 GeV
- |etaJet| &lt; 4.5
- min(DeltaR(jet,photon)) &gt; 0.3;
- Inclusive selection: Njets&gt;=0; Exclusive selection: Njets=0.