cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.132793.v1/t52
title: "Figure17_leadj_mzx_width3_highlimit" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative width values of 3% at the high boundary of the limit-sensitive mass range for the ZX spectrum of the leading small-R jet category. The vertical line corresponds to the expected nominal exclusion limit at 95% CL.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t53
title: "Figure17_leadj_mzx_width5_lowlimit" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative width values of 5% at the low boundary of the limit-sensitive mass range for the ZX spectrum of the leading small-R jet category. The vertical line corresponds to the expected nominal exclusion limit at 95% CL.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t54
title: "Figure17_leadj_mzx_width5_highlimit" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative width values of 5% at the high boundary of the limit-sensitive mass range for the ZX spectrum of the leading small-R jet category. The vertical line corresponds to the expected nominal exclusion limit at 95% CL.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t55
title: "Figure17_leadj_mzx_width10_lowlimit" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative width values of 10% at the low boundary of the limit-sensitive mass range for the ZX spectrum of the leading small-R jet category. The vertical line corresponds to the expected nominal exclusion limit at 95% CL.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t56
title: "Figure17_leadj_mzx_width10_highlimit" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Distribution of exclusion upper limits on signal event yields at 95% CL from 1000 pseudo-experiments for Gaussian-shaped signals with relative width values of 10% at the high boundary of the limit-sensitive mass range for the ZX spectrum of the leading small-R jet category. The vertical line corresponds to the expected nominal exclusion limit at 95% CL.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t57
title: "Table 1: data yields" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Data yields of the six event categories in the $Z\to e^+e^-$ and $\mu^+\mu^-$ decay channels. The merged-$e^+e^-$ events are included in the $e^+e^-$ channel, increasing the event yield, mainly in the leading large-$R$-jet category, by 0.6 %.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t58
title: "Table 2: fit ranges and functions" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: A list of mass spectra, event categories and their corresponding fit ranges, functional forms, numbers of free parameters and global $\chi^2$ $p$-values from background-only fits. The fit range values are rounded to the nearest 5 GeV. Here $f_1(x)=p_0\left(\mathrm{e}^{-p_1x}+p_2\mathrm{e}^{-(p_1+p_3)x}+p_4\mathrm{e}^{-(p_1+p_3+p_5)x}+\cdots\right)$ and $f_2(x)=p_0(1-x)^{p_1}x^{p_2+p_3\ln\!x+p_4\ln^2\!x+\cdots}$
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t59
title: "Table 3: sensitive mass ranges and p-values" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: A list of mass spectra, event categories and their corresponding signal-sensitive mass ranges. The initial BH $p$-value is obtained by using the background derived from the background-only fit in the full fit range, whereas the new BH $p$-value uses the background derived from the background-only fit in the range excluding the initial BH interval.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t60
title: "Table 4: Pseudo experiment table" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: A list of mass spectra, event categories, relative width values of Gaussian-shaped signals and limit-sensitive mass ranges and fractions, corresponding to the mass values in the previous column, of pseudo-experiments having exclusion upper limits higher than the nominal exclusion limit at 95% CL
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t61
title: "Table 5: cutflow of HVT model A signals" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Cutflow of HVT model $A$ signals ($W^\prime \to ZW \to \ell\ell qq$) with $m_{W^\prime} = 1$ TeV and $m_{W^\prime} = 4$ TeV based on MC simulations.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132793.v1/t62
title: "Table 6: acceptance times efficiency" of "A search for new resonances in multiple final states with a high transverse momentum $Z$ boson in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance times efficiency ($\mathcal{A} \times \epsilon$) values in % in the dominant event category for $p^Z_{\mathrm{T}} &gt; 100$ GeV in the $Z \to \ell^{+}\ell^{-}$ decay channel.
description: A search for new resonances in multiple final states with a high transverse momentum Z boson in $\sqrt{s}=$13 TeV pp collisions with the ATLAS detector 

A generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100GeV, decaying to $e^{+}e^{-}$ or $\mu^{+}\mu^{-}$. The analysed data collected with the
ATLAS detector in proton–proton collisions at a center-of-mass energy of 13 TeV at the Large Hadron Collider corresponds to an integrated luminosity of 139 $fb^{-1}$. Two invariant mass distributions are
examined for a localised excess with respect to the Standard Model background in six independent event categories and their combination to increase the sensitivity. No significant excess is observed.
Exclusion limits at 95% confidence level are derived for two cases: a model independent interpretation of Gaussian-shaped resonances with the mass width between 3% and 10% of the resonance mass,
and a specific model of the heavy vector triplet with the decay mode $𝑊^{\prime} \to ZW \to \ell\ell qq$.
DOI: 10.17182/hepdata.132824.v1/t1
title: "Table 1: figure 2a" of "Production of $\pi^0$, $\eta$, and $K_S$ mesons in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV"

description: $\pi^0$ spectra from figure 2a from minimum bias U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.
description: BNL-RHIC. The PHENIX experiment at the Relativistic Heavy Ion Collider measured $\pi^0$ and $\eta$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $\pi^0$($\eta$)$\rightarrow\gamma\gamma$ decay modes. A strong suppression of $\pi^0$ and $\eta$ meson production at high transverse momentum was observed in central U$+$U collisions relative to binary scaled $p$$+$$p$ results. Yields of $\pi^0$ and $\eta$ mesons measured in U$+$U collisions show similar suppression pattern to the ones measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV for similar numbers of participant nucleons. The $\eta$/$\pi^0$ ratios do not show dependence on centrality or transverse momentum, and are consistent with previously measured values in hadron-hadron, hadron-nucleus, nucleus-nucleus, and $e^+e^-$ collisions.
DOI: 10.17182/hepdata.132824.v1/t3
title: "Table 3: figure 2a" of "Production of $\pi^0$, $\eta$, and $K_S$ mesons in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV"

description: $\pi^0$ spectra from figure 2a from 20-40% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.
description: BNL-RHIC. The PHENIX experiment at the Relativistic Heavy Ion Collider measured $\pi^0$ and $\eta$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $\pi^0$($\eta$)$\rightarrow\gamma\gamma$ decay modes. A strong suppression of $\pi^0$ and $\eta$ meson production at high transverse momentum was observed in central U$+$U collisions relative to binary scaled $p$$+$$p$ results. Yields of $\pi^0$ and $\eta$ mesons measured in U$+$U collisions show similar suppression pattern to the ones measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV for similar numbers of participant nucleons. The $\eta$/$\pi^0$ ratios do not show dependence on centrality or transverse momentum, and are consistent with previously measured values in hadron-hadron, hadron-nucleus, nucleus-nucleus, and $e^+e^-$ collisions.
DOI: 10.17182/hepdata.132824.v1/t2
title: "Table 2: figure 2a" of "Production of $\pi^0$, $\eta$, and $K_S$ mesons in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV"

description: $\pi^0$ spectra from figure 2a from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.
description: BNL-RHIC. The PHENIX experiment at the Relativistic Heavy Ion Collider measured $\pi^0$ and $\eta$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $\pi^0$($\eta$)$\rightarrow\gamma\gamma$ decay modes. A strong suppression of $\pi^0$ and $\eta$ meson production at high transverse momentum was observed in central U$+$U collisions relative to binary scaled $p$$+$$p$ results. Yields of $\pi^0$ and $\eta$ mesons measured in U$+$U collisions show similar suppression pattern to the ones measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV for similar numbers of participant nucleons. The $\eta$/$\pi^0$ ratios do not show dependence on centrality or transverse momentum, and are consistent with previously measured values in hadron-hadron, hadron-nucleus, nucleus-nucleus, and $e^+e^-$ collisions.
DOI: 10.17182/hepdata.132824.v1/t4
title: "Table 4: figure 2a" of "Production of $\pi^0$, $\eta$, and $K_S$ mesons in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV"

description: $\pi^0$ spectra from figure 2a from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.
description: BNL-RHIC. The PHENIX experiment at the Relativistic Heavy Ion Collider measured $\pi^0$ and $\eta$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $\pi^0$($\eta$)$\rightarrow\gamma\gamma$ decay modes. A strong suppression of $\pi^0$ and $\eta$ meson production at high transverse momentum was observed in central U$+$U collisions relative to binary scaled $p$$+$$p$ results. Yields of $\pi^0$ and $\eta$ mesons measured in U$+$U collisions show similar suppression pattern to the ones measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV for similar numbers of participant nucleons. The $\eta$/$\pi^0$ ratios do not show dependence on centrality or transverse momentum, and are consistent with previously measured values in hadron-hadron, hadron-nucleus, nucleus-nucleus, and $e^+e^-$ collisions.