cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.82813.v1/t3
title: "Table 3" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Invariant yield of Z$^{0}$ production in 2.5 &lt; y &lt; 4.0 divided by the average nuclear overlap function as a function of rapidity in the 0-90% centrality class. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.
description: The production of Z-bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported.

Z-boson candidates are reconstructed in the dimuon decay channel (${\rm Z}^{0} \rightarrow \mu^{+}\mu^{-}$), based on muons selected with pseudo-rapidity $-4.0&lt;\eta_{\mu}&lt;-2.5$ and $p_{\rm T}^\mu&gt;20$ GeV/$c$.

The invariant yield and the nuclear modification factor, $R_{AA}$, are presented as a function of rapidity and collision centrality.

The value of $R_{\rm AA}$ for the 0-20% central Pb-Pb collisions is $0.67 \pm 0.11 \, \mbox{(stat.)} \, \pm 0.03 \, \mbox{(syst.)} \, \pm 0.06 \, \mbox{(corr. syst.)}$, exhibiting a deviation of $2.6 \sigma$ from unity.

The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by $2.3\sigma$ in the 0-90% centrality class and by $3\sigma$ in the 0-20% central collisions.
DOI: 10.17182/hepdata.82813.v1/t4
title: "Table 4" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Nuclear modification factor of Z$^{0}$ production as a function of rapidity in the 0-90% centrality class. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.
description: The production of Z-bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported.

Z-boson candidates are reconstructed in the dimuon decay channel (${\rm Z}^{0} \rightarrow \mu^{+}\mu^{-}$), based on muons selected with pseudo-rapidity $-4.0&lt;\eta_{\mu}&lt;-2.5$ and $p_{\rm T}^\mu&gt;20$ GeV/$c$.

The invariant yield and the nuclear modification factor, $R_{AA}$, are presented as a function of rapidity and collision centrality.

The value of $R_{\rm AA}$ for the 0-20% central Pb-Pb collisions is $0.67 \pm 0.11 \, \mbox{(stat.)} \, \pm 0.03 \, \mbox{(syst.)} \, \pm 0.06 \, \mbox{(corr. syst.)}$, exhibiting a deviation of $2.6 \sigma$ from unity.

The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by $2.3\sigma$ in the 0-90% centrality class and by $3\sigma$ in the 0-20% central collisions.
DOI: 10.17182/hepdata.82813.v1/t5
title: "Table 5" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Invariant yield of Z$^{0}$ production in 2.5 &lt; y &lt; 4.0 divided by the average nuclear overlap function as a function of the average number of participants scaled by the average number of binary nucleon-nucleon collisions. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.
description: The production of Z-bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported.

Z-boson candidates are reconstructed in the dimuon decay channel (${\rm Z}^{0} \rightarrow \mu^{+}\mu^{-}$), based on muons selected with pseudo-rapidity $-4.0&lt;\eta_{\mu}&lt;-2.5$ and $p_{\rm T}^\mu&gt;20$ GeV/$c$.

The invariant yield and the nuclear modification factor, $R_{AA}$, are presented as a function of rapidity and collision centrality.

The value of $R_{\rm AA}$ for the 0-20% central Pb-Pb collisions is $0.67 \pm 0.11 \, \mbox{(stat.)} \, \pm 0.03 \, \mbox{(syst.)} \, \pm 0.06 \, \mbox{(corr. syst.)}$, exhibiting a deviation of $2.6 \sigma$ from unity.

The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by $2.3\sigma$ in the 0-90% centrality class and by $3\sigma$ in the 0-20% central collisions.
DOI: 10.17182/hepdata.82813.v1/t6
title: "Table 6" of "Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV"

description: Nuclear modification factor of Z$^{0}$ production in 2.5 &lt; y &lt; 4.0 as a function of the average number of participants scaled by the average number of binary nucleon-nucleon collisions. The first uncertainty is statistical, the second is the uncorrelated systematic and the third is the correlated systematic.
description: The production of Z-bosons at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV is reported.

Z-boson candidates are reconstructed in the dimuon decay channel (${\rm Z}^{0} \rightarrow \mu^{+}\mu^{-}$), based on muons selected with pseudo-rapidity $-4.0&lt;\eta_{\mu}&lt;-2.5$ and $p_{\rm T}^\mu&gt;20$ GeV/$c$.

The invariant yield and the nuclear modification factor, $R_{AA}$, are presented as a function of rapidity and collision centrality.

The value of $R_{\rm AA}$ for the 0-20% central Pb-Pb collisions is $0.67 \pm 0.11 \, \mbox{(stat.)} \, \pm 0.03 \, \mbox{(syst.)} \, \pm 0.06 \, \mbox{(corr. syst.)}$, exhibiting a deviation of $2.6 \sigma$ from unity.

The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by $2.3\sigma$ in the 0-90% centrality class and by $3\sigma$ in the 0-20% central collisions.
DOI: 10.17182/hepdata.80235.v1/t2
title: "Table 2" of "J/$\psi$ elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 5.02 TeV"

description: Transverse momentum dependence of inclusive J/$\psi$ $v_2$ at $\sqrt{s_{\rm NN}}=5.02$ TeV for the 20-40% centrality class (mid-rapidity). The first uncertainty (stat) is statistical, the second (sys,uncorrel) is the uncorrelated systematic, while the third one (sys,correl) is a $p_{\rm T}$-correlated systematic uncertainty.
description: CERN-LHC. We report a precise measurement of the J/$\psi$ elliptic flow in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV with the ALICE detector at the LHC. The J/$\psi$ mesons are reconstructed at mid-rapidity ($|y| &lt; 0.9$) in the dielectron decay channel and at forward rapidity ($2.5
DOI: 10.17182/hepdata.80235.v1/t4
title: "Table 4" of "J/$\psi$ elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 5.02 TeV"

description: Transverse momentum dependence of inclusive J/$\psi$ $v_2$ at $\sqrt{s_{\rm NN}}=5.02$ TeV for the 40-60% centrality class (forward rapidity). The first uncertainty (stat) is statistical, the second (sys,uncorrel) is the uncorrelated systematic, while the third one (sys,correl) is a $p_{\rm T}$-correlated systematic uncertainty.
description: CERN-LHC. We report a precise measurement of the J/$\psi$ elliptic flow in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV with the ALICE detector at the LHC. The J/$\psi$ mesons are reconstructed at mid-rapidity ($|y| &lt; 0.9$) in the dielectron decay channel and at forward rapidity ($2.5
DOI: 10.17182/hepdata.84281.v1/t1
title: "Table 1" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Beam-energy dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.17182/hepdata.84281.v1/t3
title: "Table 3" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Beam-energy dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.17182/hepdata.84281.v1/t5
title: "Table 5" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Centrality dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.17182/hepdata.79498.v1/t1
title: "Table 1" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

description: Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for $\pi$, $\it{e}$ test beam (dE/dx). Statistical uncertainties as vertical error bars.
description: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.
DOI: 10.17182/hepdata.84281.v1/t2
title: "Table 2" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Beam-energy dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.17182/hepdata.84281.v1/t4
title: "Table 4" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Centrality dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.17182/hepdata.84281.v1/t6
title: "Table 6" of "Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV"

description: Centrality dependence of nu_dyn.
description: CERN-LHC. First results on K/pi, p/pi and K/p fluctuations are obtained with the ALICE detector at the CERN LHC as a function of centrality in Pb--Pb collisions at sqrt(s) = 2.76. The observable nu_dyn, which is defined in terms of the moments of particle multiplicity distributions, is used to quantify the magnitude of dynamical fluctuations of relative particle yields and also provides insight into the correlation between particle pairs. This study is based on a novel experimental technique, called the Identity Method, which allows one to measure the moments of multiplicity distributions in case of incomplete particle identification. The results for p/pi show a change of sign in nu_dyn from positive to negative towards more peripheral collisions. For central collisions, the results follow the smooth trend of the data at lower energies and nu_dyn exhibits a change in sign for p/pi and K/p.
DOI: 10.5064/f6g2petf/62qlqs
title: Moore-et-al_MD_0521_Governor Larry Hogan - Official Website for the Governor of Maryland_11.pdf
DOI: 10.17182/hepdata.116236.v1/t1
title: "Table 1" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=18 deg as function of incident photon energy E. The uncertainties are statistical and systematic, combined in quadrature.
description: A2 at MAMI. The differential cross section evaluated for 27 energy bins span the photon-energy range 290–813 MeV (W=1.195–1.553 GeV)
and the pion c.m. polar production angles, ranging from $18^o$ to $162^o$, making use of model-dependent nuclear corrections to
extract data on the neutron from measurements on the deuteron target. Additionally, the total cross section was measured.
The tagged photon beam produced by the 883 MeV electron beam of the Mainz Microtron MAMI was used. The data was obtained
with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.116236.v1/t2
title: "Table 2" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=32 deg as function of incident photon energy E. The uncertainties are statistical and systematic, combined in quadrature.
description: A2 at MAMI. The differential cross section evaluated for 27 energy bins span the photon-energy range 290–813 MeV (W=1.195–1.553 GeV)
and the pion c.m. polar production angles, ranging from $18^o$ to $162^o$, making use of model-dependent nuclear corrections to
extract data on the neutron from measurements on the deuteron target. Additionally, the total cross section was measured.
The tagged photon beam produced by the 883 MeV electron beam of the Mainz Microtron MAMI was used. The data was obtained
with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.116236.v1/t3
title: "Table 3" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=41 deg as function of incident photon energy E. The uncertainties are statistical and systematic, combined in quadrature.
description: A2 at MAMI. The differential cross section evaluated for 27 energy bins span the photon-energy range 290–813 MeV (W=1.195–1.553 GeV)
and the pion c.m. polar production angles, ranging from $18^o$ to $162^o$, making use of model-dependent nuclear corrections to
extract data on the neutron from measurements on the deuteron target. Additionally, the total cross section was measured.
The tagged photon beam produced by the 883 MeV electron beam of the Mainz Microtron MAMI was used. The data was obtained
with Crystal Ball/TAPS experimental setup.
DOI: 10.17182/hepdata.79498.v1/t2
title: "Table 2" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

description: Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for $\pi$, $\it{e}$ test beam (dE/dx + TR). Statistical uncertainties as vertical error bars.
description: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.
DOI: 10.17182/hepdata.79498.v1/t3
title: "Table 3" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

description: Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for $\pi$, $\it{e}$ and proton in pp collisions ($\sqrt{s} = 7$ TeV). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.
description: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.
DOI: 10.17182/hepdata.79498.v1/t4
title: "Table 4" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

description: Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for cosmic-ray muons (dE/dx). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.
description: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.
DOI: 10.17182/hepdata.79498.v1/t5
title: "Table 5" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

description: Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for cosmic-ray muons (dE/dx + TR). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.
description: CERN-LHC. The Transition Radiation Detector (TRD) was designed and built to enhance the capabilities of the ALICE detector at the Large Hadron Collider (LHC). While aimed at providing electron identification and triggering, the TRD also contributes significantly to the track reconstruction and calibration in the central barrel of ALICE. In this paper the design, construction, operation, and performance of this detector are discussed. A pion rejection factor of up to 410 is achieved at a momentum of 1 GeV/$c$ in p-Pb collisions and the resolution at high transverse momentum improves by about 40% when including the TRD information in track reconstruction. The triggering capability is demonstrated both for jet, light nuclei, and electron selection.
DOI: 10.17182/hepdata.116236.v1/t10
title: "Table 10" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=87 deg as function of incident photon energy E. The uncertainties are statistical and systematic, combined in quadrature.
description: A2 at MAMI. The differential cross section evaluated for 27 energy bins span the photon-energy range 290–813 MeV (W=1.195–1.553 GeV)
and the pion c.m. polar production angles, ranging from $18^o$ to $162^o$, making use of model-dependent nuclear corrections to
extract data on the neutron from measurements on the deuteron target. Additionally, the total cross section was measured.
The tagged photon beam produced by the 883 MeV electron beam of the Mainz Microtron MAMI was used. The data was obtained
with Crystal Ball/TAPS experimental setup.