cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.116236.v1/t4
title: "Table 4" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=49 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/t5
title: "Table 5" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=57 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/t6
title: "Table 6" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=63 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/t7
title: "Table 7" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=69 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/t8
title: "Table 8" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=75 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/t9
title: "Table 9" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at THETA=81 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: 10.5064/f6g2petf/3cw0jh
title: Moore-et-al_MD_0121_Vaccine-Administration.pdf
DOI: 10.17182/hepdata.116236.v1/t11
title: "Table 11" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=93 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/t12
title: "Table 12" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=99 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/t13
title: "Table 13" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=104 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/t14
title: "Table 14" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=110 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/t15
title: "Table 15" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=117 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/t16
title: "Table 16" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=123 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/t17
title: "Table 17" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=130 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/t18
title: "Table 18" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=138 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/t19
title: "Table 19" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=148 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/t20
title: "Table 20" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Excitation function at pion c.m. angle THETA=162 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/t21
title: "Table 21" of "Cross Section for $\gamma n \to \pi^0 n$ measured at Mainz/A2"

description: Total cross section as a function of incident photon energy E.
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.78549.v1/t3
title: "Table 3" of "Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC"

description: v2 of anti-deuterons and deuterons vs $p_{\mathrm T}$ for different centrality intervals
description: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|&lt;0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $&lt;$ $p_{\mathrm{T}}$ $&lt; $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $&gt;$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.
DOI: 10.17182/hepdata.78255.v1/t1
title: "Table 1" of "D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV"

description: $v_2$ vs. $p_{\rm T}$ of $D^0$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|&lt;0.8.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|&lt;0.8, in the transverse momentum interval 1&lt;$p_{\rm T}$&lt;24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.
DOI: 10.17182/hepdata.78255.v1/t2
title: "Table 2" of "D-meson azimuthal anisotropy in mid-central Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV"

description: $v_2$ vs. $p_{\rm T}$ of $D^+$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|&lt;0.8.
The second (sys) error is the systematic uncertainty from the B feed-down contribution.
The first (sys) error is the systematic uncertainty from the other sources.
description: CERN-LHC. The azimuthal anisotropy coefficient $v_2$ of prompt $D^0$, $D^+$, $D^{*+}$ and $D_s^+$ mesons was measured in mid-central (30-50% centrality class) Pb-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}$ = 5.02 TeV, with the ALICE detector at the LHC. The D mesons were reconstructed via their hadronic decays at mid-rapidity, |$y$|&lt;0.8, in the transverse momentum interval 1&lt;$p_{\rm T}$&lt;24 GeV/$c$. The measured D-meson $v_2$ has similar values as that of charged pions. The $D_s^+$ $v_2$, measured for the first time, is found to be compatible with that of non-strange D mesons. The measurements are compared with theoretical calculations of charm-quark transport in a hydrodynamically expanding medium and have the potential to constrain medium parameters.
DOI: 10.17182/hepdata.78549.v1/t1
title: "Table 1" of "Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC"

description: Deuteron $p_{\mathrm T}$ spectra for $p_{\mathrm T} &gt; $ 4.4 GeV/$c$. Low $p_{\mathrm T}$ points can be found here 'http://hepdata.cedar.ac.uk/view/ins1380491'
description: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|&lt;0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $&lt;$ $p_{\mathrm{T}}$ $&lt; $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $&gt;$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.
DOI: 10.17182/hepdata.78549.v1/t2
title: "Table 2" of "Measurement of deuteron spectra and elliptic flow in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}$ = 2.76 TeV at the LHC"

description: $\overline{\mathrm d}/ d $ vs $p_{\mathrm T}$ for $p_{\mathrm T} &gt; $ 4.4 GeV/$c$. Low $p_{\mathrm T}$ points can be found here 'http://hepdata.cedar.ac.uk/view/ins1380491'
description: The transverse momentum ($p_{\mathrm{T}}$) spectra and elliptic flow coefficient ($v_{2}$) of deuterons and anti-deuterons at mid-rapidity ($|y|&lt;0.5$) are measured with the ALICE detector at the LHC in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV. The measurement of the $p_{\mathrm{T}}$ spectra of (anti-)deuterons is done up to 8 GeV/$c$ in 0-10\% centrality class and up to 6 GeV/$c$ in 10-20\% and 20-40\% centrality classes. The $v_{2}$ is measured in the 0.8 $&lt;$ $p_{\mathrm{T}}$ $&lt; $5 GeV/$c$ interval and in six different centrality intervals (0-5\%, 5-10\%, 10-20\%, 20-30\%, 30-40\% and 40-50\%) using the scalar product technique. Measured \pio$^{\pm}$, K$^{\pm}$ and p+$\overline{\mathrm{p}}$ transverse-momentum spectra and $v_{2}$ are used to predict the deuteron $p_{\mathrm{T}}$ spectra and $v_{2}$ within the Blast-Wave model. The predictions are able to reproduce the $v_{2}$ coefficient in the measured $p_{\mathrm{T}}$ range and the transverse-momentum spectra for $p_{\mathrm{T}}$ $&gt;$ 1.8 GeV/$c$ within the experimental uncertainties. The measurement of the coalescence parameter $B_2$ is performed, showing a $p_{\mathrm{T}}$ dependence in contrast with the simplest coalescence model, which fails to reproduce also the measured $v_{2}$ coefficient. In addition, the coalescence parameter $B_2$ and the elliptic flow coefficient in the 20-40\% centrality interval are compared with the AMPT model which is able, in its version without string melting, to reproduce the measured $v_{2}$($p_{\mathrm{T}}$) and the $B_2$($p_{\mathrm{T}}$) trend.