cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141173.v1/t3
title: "Table 3 - Away" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the away azimuthal regions. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (left panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v1/t4
title: "Table 4 - Jet" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the jet region, obtained as toward-transverse. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (right panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v1/t5
title: "Table 5 - B2 in UE" of "Enhanced deuteron coalescence probability in jets"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the underlying event (transverse region). Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v1/t6
title: "Table 6 - B2 in Jet" of "Enhanced deuteron coalescence probability in jets"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the jet (transverse-toward region). Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t1
title: "Table 1 - Transverse" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the transverse azimuthal regions. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (left panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t2
title: "Table 2 - Toward" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the toward azimuthal regions. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (left panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t3
title: "Table 3 - Away" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the away azimuthal regions. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (left panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t4
title: "Table 4 - Jet" of "Enhanced deuteron coalescence probability in jets"

description: Transverse momentum spectra for the jet region, obtained as toward-transverse. Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The spectrum is shown in Figure 1 (right panel).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t5
title: "Table 5 - B2 in UE" of "Enhanced deuteron coalescence probability in jets"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the underlying event (transverse region). Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141173.v2/t6
title: "Table 6 - B2 in Jet" of "Enhanced deuteron coalescence probability in jets"

description: Coalescence parameter B2 as a function of the transverse momentum per nucleon pT/A, in the jet (transverse-toward region). Events with a leading track with PT&gt;5 GEV at midrapidity are selected. The B2 is shown in Figure 2 (both panels).
description: Transverse spectra of three azimuthal regions for events with pT leading larger than 5 GEV, measured in pp collisions at centre-of-mass per nucleon-nucleon energy of 13 TeV. Moreover, the coalescence parameters B2 in jets and in the underlying event are reported.
DOI: 10.17182/hepdata.141275.v1/t1
title: "Figure 2a" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Electron pair mass distribution for Au+Au events for 1.0 &lt; $p_T$ &lt; 1.5 GeV/$c$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t2
title: "Figure 2b" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Electron pair mass distribution for Au+Au events for 1.0 &lt; $p_T$ &lt; 1.5 GeV/$c$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t3
title: "Figure 2c" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Electron pair mass distribution for Au+Au events for 1.0 &lt; $p_T$ &lt; 1.5 GeV/$c$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t4
title: "Figure 3a" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: The fraction of the direct photon component as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t5
title: "Figure 3b" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: The fraction of the direct photon component as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t6
title: "Figure 4a" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Invariant yield (Au+Au) of direct photons as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t7
title: "Figure 4b" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Invariant yield (Au+Au) of direct photons as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t8
title: "Figure 4c" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Invariant yield (Au+Au) of direct photons as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141275.v1/t9
title: "Figure 4d" of "Enhanced production of direct photons in Au+Au collisions at sqrt(s_NN)=200 GeV and implications for the initial temperature"

description: Invariant cross section ($p$+$p$) of direct photons as a function of $p_T$.
description: The production of low mass $e^+e^-$ pairs for $m_{e^+e^-}$ &lt; 300 MeV/$c^2$ and 1 &lt; $p_T$ &lt;5 GeV/$c$ is measured in $p$+$p$ and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Enhanced yield above hadronic sources is observed. Treating the excess as internal conversions, the invariant yield of direct photons is deduced. In central Au+Au collisions, the excess of direct photon yield over $p$+$p$ is exponential in transverse momentum, with inverse slope $T$ = 221 $\pm$ 19 (stat) $\pm$ 19 (syst) MeV. Hydrodynamical models with initial temperatures ranging from $T_{int}$ ~300-600 MeV at times of ~ 0.6 - 0.15 fm/$c$ after the collision are in qualitative agreement with the data. Lattice QCD predicts a phase transition to quark gluon plasma at ~ 170 MeV.
DOI: 10.17182/hepdata.141276.v1/t1
title: "Table 7" of "Cross section for $b\bar{b}$ production via dielectrons in d$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $b\bar{b}$ cross section
description: We report a measurement of $e^{+}e^{-}$ pairs from semileptonic heavy-flavor decays in $d$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Exploring the mass and transverse-momentum dependence of the yield, the bottom decay contribution can be isolated from charm, and quantified by comparison to PYTHIA and MC@NLO simulations. The resulting $b\bar{b}$-production cross section is $\sigma^{dAu}_{b\bar{b}}$ = 1.37$\pm$0.28(stat)$\pm$0.46(syst) mb, which is equivalent to a nucleon-nucleon cross section of $\sigma^{NN}_{b\bar{b}}$ = 3.4 $\pm$ 0.8(stat)$\pm$1.1(syst) $\mu$b
DOI: 10.17182/hepdata.141277.v1/t1
title: "Table 1" of "Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with charged leptons and jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel for boosted.
description: A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved channel) and topologies with boosted final states with hadronic products partially overlapping and reconstructed as a large-radius jet, caused by a large mass difference between $W_{\mathrm{R}}$ and $N_{\mathrm{R}}$ (``boosted channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits at 95% confidence level are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})&lt;1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos.
DOI: 10.17182/hepdata.141277.v1/t2
title: "Table 2" of "Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with charged leptons and jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Expected 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel for boosted.
description: A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved channel) and topologies with boosted final states with hadronic products partially overlapping and reconstructed as a large-radius jet, caused by a large mass difference between $W_{\mathrm{R}}$ and $N_{\mathrm{R}}$ (``boosted channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits at 95% confidence level are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})&lt;1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos.
DOI: 10.17182/hepdata.141277.v1/t3
title: "Table 3" of "Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with charged leptons and jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Observed 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel for boosted.
description: A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved channel) and topologies with boosted final states with hadronic products partially overlapping and reconstructed as a large-radius jet, caused by a large mass difference between $W_{\mathrm{R}}$ and $N_{\mathrm{R}}$ (``boosted channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits at 95% confidence level are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})&lt;1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos.
DOI: 10.17182/hepdata.141277.v1/t10
title: "Table 10" of "Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with charged leptons and jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector"

description: Expected 95% CL exclusion contours for the assumption of Majorana type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel for resolved.
description: A search for heavy right-handed Majorana or Dirac neutrinos $N_{\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved channel) and topologies with boosted final states with hadronic products partially overlapping and reconstructed as a large-radius jet, caused by a large mass difference between $W_{\mathrm{R}}$ and $N_{\mathrm{R}}$ (``boosted channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits at 95% confidence level are set on masses in the heavy right-handed $W_{\mathrm{R}}$ boson and $N_{\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\mathrm{R}}$ neutrinos at $m(N_{\mathrm{R}})&lt;1$ TeV. $N_{\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\mathrm{R}})$ up to 3.6 TeV for $m(W_{\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos.