cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.130236.v1/t20
title: "K0L0-dcs10" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.855 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t21
title: "K0S0-dcs01" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.690 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t22
title: "K0S0-dcs02" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.720 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t23
title: "K0S0-dcs03" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.750 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t24
title: "K0S0-dcs04" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.775 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t25
title: "K0S0-dcs05" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.795 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.25549/vercoutere-ouc110611388
title: Beach house

description: Gray and brown house with black roof next to an orange and brown cobblestone road; a gray post with white highlights stands beside the road with a gray rail extending in both directions from the post. Blue waves roll onto a white beach beside the road. The background has a black grid (fence?) colored orange and yellow green and a dark blue and black sky. See description of 001 for OT notes.
DOI: 10.17182/hepdata.130236.v1/t26
title: "K0S0-dcs06" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.815 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t27
title: "K0S0-dcs07" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.835 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130236.v1/t28
title: "K0S0-dcs08" of "Experimental study of the $\gamma p\rightarrow K^0\Sigma^+$, $\gamma n\rightarrow K^0\Lambda$, and $\gamma n\rightarrow K^0 \Sigma^0$ reactions at the Mainz Microtron"

description: Differential cross section at W= 1.855 GeV
description: A2 Collaboration at MAMI.
Differential and total cross sections for the quasifree reactions
$\gamma p \to K^0\Sigma^+$, $\gamma n \to K^0\Lambda$ and $\gamma n \to K^0\Sigma^0$
have been measured from threshold up to a c.m. energy W = 1855 MeV
at the MAMI-C electron accelerator by using a liquid deuterium
target. W was calculated from the incident beam energy assuming
quasifree kinematics. Fermi-motion corrections were not possible
in the present analysis due to the large combinatoric background.
The systematic uncertainty is the combination of uncertainties from
the photon flux (from 1.1% to 2.4%), acceptance (from 2% to 4%), and
branching ratios (1.4% for $\gamma n \to K^0\Lamda$ and $\gamma n \to K^0\Sigma^0$,
and 0.6% for $\gamma p \to K^0\Sigma^+$). The statistical
uncertainties are dominate and varied from a maximum of 34% at
$cos\Theta_{cm}=0.625$ to a minimum of 14% at $cos\Theta_{cm}=-0.625$.
Total cross sections were extracted by fitting the differential
cross sections with Legendre polynomials.
DOI: 10.17182/hepdata.130237.v1/t1
title: "Table 3 p-p" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fraction of non-prompt $\rm{J}/\psi$ in pp collisions at $\sqrt{s}$ = 5.02 TeV for different $p_\mathrm{T}$ ranges, as determined with a procedure of interpolation from measurments at other energies. It is not a direct measurment.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t2
title: "Figure 3" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Inclusive d$^2\sigma$/d$y$d$p_{\rm T}$ in bins of $p_{\mathrm{T}}^{J/\psi}$ for prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t10
title: "Figure 8a" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Nuclear modification factor ($R_{pPb}$) in bins of $p_{\mathrm{T}}^{J/\psi}$ for non-prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity. The extrapolation uncertainty related to the procedure to go from the visible region ($p_{\mathrm{T}}$ &gt; 1 GeV/c) to $p_{\mathrm{T}}$ &gt; 0 is considered separately.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t3
title: "Figure 4" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Fraction of non-prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV for different $p_\mathrm{T}$ ranges.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t4
title: "Figure 5a" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: d$\sigma$/dy for prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_NN}$=5.02 TeV. The systematic uncertainty includes also the contribution from the extrapolation procedure to go from the visible region ($p_{\mathrm{T}}$ &gt; 1 GeV/c) to $p_{\mathrm{T}}$ &gt; 0.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t5
title: "Figure 5b" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: d$^2\sigma$/d$y$d$p_{\rm T}$ in bins of $p_{\mathrm{T}}^{J/\psi}$ for prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t6
title: "Figure 6a" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: d$\sigma$/dy for non-prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_NN}$=5.02 TeV. The extrapolation uncertainty related to the procedure to go from the visible region ($p_{\mathrm{T}}$ &gt; 1 GeV/c) to $p_{\mathrm{T}}$ &gt; 0 is considered separately.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t7
title: "Figure 6b" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: d$^2\sigma$/d$y$d$p_{\rm T}$ in bins of $p_{\mathrm{T}}^{J/\psi}$ for non-prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity..
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t8
title: "Figure 7a" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Nuclear modification factor ($R_{pPb}$) in bins of $p_{\mathrm{T}}^{J/\psi}$ for prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.17182/hepdata.130237.v1/t9
title: "Figure 7b" of "Inclusive, prompt and non-prompt ${\rm J}/\psi$ production at midrapidity in p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV"

description: Nuclear modification factor ($R_{pPb}$) for inclusive and prompt J/$\psi$ in p--Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity.
description: The measurement of inclusive, prompt, and non-prompt J/$\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\rm{J}/\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\mathrm{T}$ = 0. Non-prompt J/$\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\psi$ on a statistical basis for $p_\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p−Pb run, corresponding to an integrated luminosity of $\it{L}_{int}$=292$\pm$11$\mathrm{\mu b}^{-1}$.
DOI: 10.25549/vercoutere-ouc110611461
title: Nude woman in a green room with blue windows

description: One nude white female depicted from head to knees is outlined in black. She has black hair; a red face, shoulders, waist and parts of breasts; a partially green leg; a partially blue leg; and black pubic area. She is standing in a room with green walls and two small blackwindows on both sides of her head. See description of 001 for OT notes.