cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.141938.v1/t2
title: "Figure 2b" of "Nuclear dependence of the transverse single-spin asymmetry in the production of charged hadrons at forward rapidity in polarized $p+p$, $p+$Al, and $p+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $A_N$ as a function of $N^{Avg.}_{coll}$ for positively-charged hadrons at 1.4 &lt; $\eta$ &lt; 2.4, 0.1 &lt; $x_F$ &lt; 0.2, and 1.8 &lt; $p_T$ &lt; 7.0 GeV/$c$ in $p^{\uparrow}$+$p$, $p^{\uparrow}$+Al, and $p^{\uparrow}$+Au collisions.
description: We report on the nuclear dependence of transverse single-spin asymmetries (TSSAs) in the production of positively-charged hadrons in polarized $p^{\uparrow}$+$p$, $p^{\uparrow}$+Al and $p^{\uparrow}$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The measurements have been performed at forward rapidity (1.4 &lt; $\eta$ &lt; 2.4) over the range of transverse momentum (1.8 &lt; $p_T$ &lt; 7.0 GeV/$c$) and Feynman-$x$ (0.1 &lt; $x_F$&lt; 0.2). We observed a positive asymmetry $A_N$ for positively-charged hadrons in $p^{\uparrow}$+$p$ collisions, and a significantly reduced asymmetry in $p^{\uparrow}$+$A$ collisions. These results reveal a nuclear dependence of charged hadron $A_N$ in a regime where perturbative techniques are relevant. These results provide new opportunities to use $p^{\uparrow}$+$A$ collisions as a tool to investigate the rich phenomena behind TSSAs in hadronic collisions and to use TSSA as a new handle in studying small-system collisions.
DOI: 10.5281/zenodo.17527251
title: L'entrepreneuriat institutionnel comme levier de transformation organisationnelle dans les hôpitaux publics : étude de cas du CHU de Fès.

description: Cet article examine le rôle de l’entrepreneuriat institutionnel dans la transformation organisationnelle des hôpitaux publics, à travers une étude de cas du Centre Hospitalier Universitaire (CHU) Hassan II de Fès. En mobilisant la théorie institutionnelle et le concept d’Institutional Entrepreneurship, la recherche analyse comment certains acteurs organisationnels parviennent à initier et à institutionnaliser des changements significatifs malgré les contraintes bureaucratiques et réglementaires propres au secteur hospitalier public marocain. La méthodologie qualitative adoptée repose sur des entretiens semi-directifs, l’analyse documentaire et l’observation, permettant de dégager les mécanismes, leviers et obstacles rencontrés. Les résultats mettent en évidence que l’entrepreneuriat institutionnel constitue un moteur essentiel pour introduire des pratiques innovantes, renforcer la gouvernance et améliorer la qualité des services de santé. L’étude propose un schéma conceptuel intégrant les acteurs, les ressources, les mécanismes institutionnels et les effets organisationnels. Enfin, elle discute des implications pour le management hospitalier et les politiques publiques de santé au Maroc.
DOI: 10.17182/hepdata.141939.v1/t1
title: "Figure 6" of "Angular decay coefficients of $J/\psi$ mesons at forward rapidity from $p+p$ collisions at $\sqrt{s}=510$ GeV"

description: Polar angular decay coefficient $\lambda_{\theta}$ as a function of transverse momentum for four reference frames and three $p_T$ bins. The numbers in the CS frame for the $p_T$ = 2-3 GeV/$c$ bin are 90% confidence level upper limits.
description: We report the first measurement of the full angular distribution for inclusive $J/\psi$ $\rightarrow$ $\mu^+\mu^-$ decays in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV. The measurements are made for $J/\psi$ transverse momentum 2 &lt; $p_T$ &lt; 10 GeV/$c$ and rapidity 1.2 &lt; $y$ &lt; 2.2 in the Helicity, Collins-Soper, and Gottfried-Jackson reference frames. In all frames the polar coefficient $\lambda_{\theta}$ is strongly negative at low $p_T$ and becomes close to zero at high $p_T$, while the azimuthal coefficient $\lambda_{\phi}$ is close to zero at low $p_T$, and becomes slightly negative at higher $p_T$. The frame-independent coefficient $\bar{\lambda}$ is strongly negative at all $p_T$ in all frames. The data are compared to the theoretical predictions provided by nonrelativistic quantum chromodynamics models.
DOI: 10.17182/hepdata.141939.v1/t2
title: "Figure 7" of "Angular decay coefficients of $J/\psi$ mesons at forward rapidity from $p+p$ collisions at $\sqrt{s}=510$ GeV"

description: "Mixed" angular decay coefficient $\lambda_{\theta \phi}$ as a function of transverse momentum for four reference frames and three $p_T$ bins.
description: We report the first measurement of the full angular distribution for inclusive $J/\psi$ $\rightarrow$ $\mu^+\mu^-$ decays in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV. The measurements are made for $J/\psi$ transverse momentum 2 &lt; $p_T$ &lt; 10 GeV/$c$ and rapidity 1.2 &lt; $y$ &lt; 2.2 in the Helicity, Collins-Soper, and Gottfried-Jackson reference frames. In all frames the polar coefficient $\lambda_{\theta}$ is strongly negative at low $p_T$ and becomes close to zero at high $p_T$, while the azimuthal coefficient $\lambda_{\phi}$ is close to zero at low $p_T$, and becomes slightly negative at higher $p_T$. The frame-independent coefficient $\bar{\lambda}$ is strongly negative at all $p_T$ in all frames. The data are compared to the theoretical predictions provided by nonrelativistic quantum chromodynamics models.
DOI: 10.17182/hepdata.141939.v1/t3
title: "Figure 8" of "Angular decay coefficients of $J/\psi$ mesons at forward rapidity from $p+p$ collisions at $\sqrt{s}=510$ GeV"

description: Azimuthal angular decay coefficient $\lambda_{\phi}$ as a function of transverse momentum for four reference frames and three $p_T$ bins.
description: We report the first measurement of the full angular distribution for inclusive $J/\psi$ $\rightarrow$ $\mu^+\mu^-$ decays in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV. The measurements are made for $J/\psi$ transverse momentum 2 &lt; $p_T$ &lt; 10 GeV/$c$ and rapidity 1.2 &lt; $y$ &lt; 2.2 in the Helicity, Collins-Soper, and Gottfried-Jackson reference frames. In all frames the polar coefficient $\lambda_{\theta}$ is strongly negative at low $p_T$ and becomes close to zero at high $p_T$, while the azimuthal coefficient $\lambda_{\phi}$ is close to zero at low $p_T$, and becomes slightly negative at higher $p_T$. The frame-independent coefficient $\bar{\lambda}$ is strongly negative at all $p_T$ in all frames. The data are compared to the theoretical predictions provided by nonrelativistic quantum chromodynamics models.
DOI: 10.17182/hepdata.141939.v1/t4
title: "Figure 9" of "Angular decay coefficients of $J/\psi$ mesons at forward rapidity from $p+p$ collisions at $\sqrt{s}=510$ GeV"

description: Frame-independent angular decay coefficient $\tilde{\lambda}$ as a function of transverse momentum for the four reference frames and three $p_T$ bins. The numbers in the CS frame for the $p_T$ = 2-3 GeV/$c$ bin are 90% confidence level upper limits.
description: We report the first measurement of the full angular distribution for inclusive $J/\psi$ $\rightarrow$ $\mu^+\mu^-$ decays in $p$+$p$ collisions at $\sqrt{s}$ = 510 GeV. The measurements are made for $J/\psi$ transverse momentum 2 &lt; $p_T$ &lt; 10 GeV/$c$ and rapidity 1.2 &lt; $y$ &lt; 2.2 in the Helicity, Collins-Soper, and Gottfried-Jackson reference frames. In all frames the polar coefficient $\lambda_{\theta}$ is strongly negative at low $p_T$ and becomes close to zero at high $p_T$, while the azimuthal coefficient $\lambda_{\phi}$ is close to zero at low $p_T$, and becomes slightly negative at higher $p_T$. The frame-independent coefficient $\bar{\lambda}$ is strongly negative at all $p_T$ in all frames. The data are compared to the theoretical predictions provided by nonrelativistic quantum chromodynamics models.
DOI: 10.5281/zenodo.17527250
title: L'entrepreneuriat institutionnel comme levier de transformation organisationnelle dans les hôpitaux publics : étude de cas du CHU de Fès.

description: Cet article examine le rôle de l’entrepreneuriat institutionnel dans la transformation organisationnelle des hôpitaux publics, à travers une étude de cas du Centre Hospitalier Universitaire (CHU) Hassan II de Fès. En mobilisant la théorie institutionnelle et le concept d’Institutional Entrepreneurship, la recherche analyse comment certains acteurs organisationnels parviennent à initier et à institutionnaliser des changements significatifs malgré les contraintes bureaucratiques et réglementaires propres au secteur hospitalier public marocain. La méthodologie qualitative adoptée repose sur des entretiens semi-directifs, l’analyse documentaire et l’observation, permettant de dégager les mécanismes, leviers et obstacles rencontrés. Les résultats mettent en évidence que l’entrepreneuriat institutionnel constitue un moteur essentiel pour introduire des pratiques innovantes, renforcer la gouvernance et améliorer la qualité des services de santé. L’étude propose un schéma conceptuel intégrant les acteurs, les ressources, les mécanismes institutionnels et les effets organisationnels. Enfin, elle discute des implications pour le management hospitalier et les politiques publiques de santé au Maroc.
DOI: 10.17182/hepdata.141940.v1/t1
title: "Table 5" of "Measurement of $\Upsilon$(1S+2S+3S) production in $p$$+$$p$ and Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Summary of the measured $\Upsilon$ invariant multiplicities, $BdN/dy$, for one $p + p$ three Au + Au data sets.
description: Measurements of bottomonium production in heavy ion and $p+p$ collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three $\Upsilon$ states, $\Upsilon$(1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au+Au and $p+p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $\Upsilon$(1S + 2S + 3S) → $e^{+}e^{-}$ differential cross section at midrapidity was found to be $B_{ee}d\sigma$/dy = 108 ± 38 (stat) ± 15 (syst) ± 11 (luminosity) pb in $p+p$ collisions. The nuclear modification factor in the 30% most central Au+Au collisions indicates a suppression of the total $\Upsilon$ state yield relative to the extrapolation from $p+p$ collision data. The suppression is consistent with measurements made by STAR at RHIC and at higher energies by the CMS experiment at the Large Hadron Collider.
DOI: 10.17182/hepdata.141940.v1/t2
title: "Table 6a" of "Measurement of $\Upsilon$(1S+2S+3S) production in $p$$+$$p$ and Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Summary of the measured $\Upsilon$ nuclear modification factors, $R_{AA}$, for Au + Au data sets.
description: Measurements of bottomonium production in heavy ion and $p+p$ collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three $\Upsilon$ states, $\Upsilon$(1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au+Au and $p+p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $\Upsilon$(1S + 2S + 3S) → $e^{+}e^{-}$ differential cross section at midrapidity was found to be $B_{ee}d\sigma$/dy = 108 ± 38 (stat) ± 15 (syst) ± 11 (luminosity) pb in $p+p$ collisions. The nuclear modification factor in the 30% most central Au+Au collisions indicates a suppression of the total $\Upsilon$ state yield relative to the extrapolation from $p+p$ collision data. The suppression is consistent with measurements made by STAR at RHIC and at higher energies by the CMS experiment at the Large Hadron Collider.
DOI: 10.17182/hepdata.141940.v1/t3
title: "Table 6b" of "Measurement of $\Upsilon$(1S+2S+3S) production in $p$$+$$p$ and Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: Summary of the measured $\Upsilon$ nuclear modification factors, $R_{AA}$, for Au + Au data sets.
description: Measurements of bottomonium production in heavy ion and $p+p$ collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three $\Upsilon$ states, $\Upsilon$(1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au+Au and $p+p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $\Upsilon$(1S + 2S + 3S) → $e^{+}e^{-}$ differential cross section at midrapidity was found to be $B_{ee}d\sigma$/dy = 108 ± 38 (stat) ± 15 (syst) ± 11 (luminosity) pb in $p+p$ collisions. The nuclear modification factor in the 30% most central Au+Au collisions indicates a suppression of the total $\Upsilon$ state yield relative to the extrapolation from $p+p$ collision data. The suppression is consistent with measurements made by STAR at RHIC and at higher energies by the CMS experiment at the Large Hadron Collider.
DOI: 10.17182/hepdata.141940.v1/t4
title: "Table 7" of "Measurement of $\Upsilon$(1S+2S+3S) production in $p$$+$$p$ and Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

description: $\Upsilon$(1S + 2S + 3S) $R_{AA}$ expected when the excited states are completed suppressed in Au + Au collisions along with the measured result in the 30% most central collision regime. Estimations based on Tables I and II.
description: Measurements of bottomonium production in heavy ion and $p+p$ collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three $\Upsilon$ states, $\Upsilon$(1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au+Au and $p+p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV. The $\Upsilon$(1S + 2S + 3S) → $e^{+}e^{-}$ differential cross section at midrapidity was found to be $B_{ee}d\sigma$/dy = 108 ± 38 (stat) ± 15 (syst) ± 11 (luminosity) pb in $p+p$ collisions. The nuclear modification factor in the 30% most central Au+Au collisions indicates a suppression of the total $\Upsilon$ state yield relative to the extrapolation from $p+p$ collision data. The suppression is consistent with measurements made by STAR at RHIC and at higher energies by the CMS experiment at the Large Hadron Collider.
DOI: 10.17182/hepdata.142036.v1/t1
title: "S/(S+B) weighted mbb distribution" of "Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The mbb distribution after weighted combination of all categories in the analysis weighted with S/(S + B). where S is the total Hbb signal yield (both VBF and ggH) and B is the total background yield including QCD multijet and Z+jets
description: No data abstract available.
DOI: 10.17182/hepdata.142036.v1/t2
title: "Best fit values of the signal strenght modifiers" of "Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The best fit values of the signal strength modifier for the different processes. The uncertainties, corresponding to one standard deviation confidence intervals, include both statistical and systematic sources. The additional breakdown of the uncertainties into their separate statistical and systematic contributions is also shown.
description: No data abstract available.
DOI: 10.17182/hepdata.142036.v1/t3
title: "Signal strenght modifiers by floating both VBF and ggH processes" of "Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: The best fit values of the signal strength modifier for the different processes by floating the VBF and ggH production rates independently. The uncertainties, corresponding to one standard deviation confidence intervals, include both statistical and systematic sources. The additional breakdown of the uncertainties into their separate statistical and systematic contributions is also shown.
description: No data abstract available.
DOI: 10.17182/hepdata.142036.v1/t4
title: "Observed 2D likelihood scan for the signal strenght modifiers" of "Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Two dimensional observed likelihood profile scan as a function of mu_ggH and mu_qqH
description: No data abstract available.
DOI: 10.17182/hepdata.142074.v1/t1
title: "Table 5" of "Upsilon (1S+2S+3S) production in d+Au and p+p collisions at sqrt(s_NN)=200 GeV and cold-nuclear matter effects"

description: $\Upsilon$ invariant yields and cross sections of $p$+$p$ and $d$+Au collisions.
description: The three $\Upsilon$ states, $\Upsilon$(1$S$+2$S$+3$S$), are measured in $d$+Au and $p$+$p$ collisions at $\sqrt{s_{NN}}$ = 200 GeV and rapidities 1.2 &lt; $|y|$ &lt; 2.2 by the PHENIX experiment at the Relativistic Heavy-Ion Collider. Cross sections for the inclusive $\Upsilon$(1$S$+2$S$+3$S$) production are obtained. The inclusive yields per binary collision for $d$+Au collisions relative to those in $p$+$p$ collisions ($R_{dAu}$) are found to be 0.62 $\pm$ 0.26 (stat) $\pm$ 0.13 (syst) in the gold-going direction and 0.91 $\pm$ 0.33 (stat) $\pm$ 0.16 (syst) in the deuteron-going direction. The measured results are compared to a nuclear-shadowing model, EPS09 [JHEP 04, 065 (2009)], combined with a final-state breakup cross section, $\sigma_{br}$, and compared to lower energy $p$+$A$ results. We also compare the results to the PHENIX $J/\psi$ results [Phys. Rev. Lett. 107, 142301 (2011)]. The rapidity dependence of the observed $\Upsilon$ suppression is consistent with lower energy $p$+$A$ measurements.
DOI: 10.17182/hepdata.142075.v1/t1
title: "Figure 5" of "$\phi$ meson production in the forward/backward rapidity region in Cu$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Invariant yield as a function of the number of participating nucleons for 1.2 &lt; $|y|$ &lt; 2.2 and 1 &lt; $p_T$ &lt; 5 GeV/$c$. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured $\phi$ meson production and its nuclear modification in asymmetric Cu+Au heavy-ion collisions at $\sqrt{s_{NN}}$ = 200 GeV at both forward Cu-going direction (1.2 &lt; $y$ &lt; 2.2) and backward Au-going direction (−2.2 &lt; $y$ &lt; −1.2), rapidities. The measurements are performed via the dimuon decay channel and reported as a function of the number of participating nucleons, rapidity, and transverse momentum. In the most central events, 0%–20% centrality, the $\phi$ meson yield integrated over 1 &lt; $p_T$ &lt; 5 GeV/$c$ prefers a smaller value, which means a larger nuclear modification, in the Cu-going direction compared to the Au-going direction. Additionally, the nuclear-modification factor in Cu+Au collisions averaged over all centrality is measured to be similar to the previous PHENIX result in $d$+Au collisions for these rapidities.
DOI: 10.17182/hepdata.142075.v1/t2
title: "Figure 6" of "$\phi$ meson production in the forward/backward rapidity region in Cu$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Invariant yield as a function of transverse momentum for 1.2 &lt; $|y|$ &lt; 2.2 and 0%–93% centrality. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured $\phi$ meson production and its nuclear modification in asymmetric Cu+Au heavy-ion collisions at $\sqrt{s_{NN}}$ = 200 GeV at both forward Cu-going direction (1.2 &lt; $y$ &lt; 2.2) and backward Au-going direction (−2.2 &lt; $y$ &lt; −1.2), rapidities. The measurements are performed via the dimuon decay channel and reported as a function of the number of participating nucleons, rapidity, and transverse momentum. In the most central events, 0%–20% centrality, the $\phi$ meson yield integrated over 1 &lt; $p_T$ &lt; 5 GeV/$c$ prefers a smaller value, which means a larger nuclear modification, in the Cu-going direction compared to the Au-going direction. Additionally, the nuclear-modification factor in Cu+Au collisions averaged over all centrality is measured to be similar to the previous PHENIX result in $d$+Au collisions for these rapidities.
DOI: 10.17182/hepdata.142075.v1/t3
title: "Figure 7" of "$\phi$ meson production in the forward/backward rapidity region in Cu$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: Invariant yield as a function of rapidity for 1 &lt; $p_T$ &lt; 5 GeV/$c$ and 0%–93% centrality. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured $\phi$ meson production and its nuclear modification in asymmetric Cu+Au heavy-ion collisions at $\sqrt{s_{NN}}$ = 200 GeV at both forward Cu-going direction (1.2 &lt; $y$ &lt; 2.2) and backward Au-going direction (−2.2 &lt; $y$ &lt; −1.2), rapidities. The measurements are performed via the dimuon decay channel and reported as a function of the number of participating nucleons, rapidity, and transverse momentum. In the most central events, 0%–20% centrality, the $\phi$ meson yield integrated over 1 &lt; $p_T$ &lt; 5 GeV/$c$ prefers a smaller value, which means a larger nuclear modification, in the Cu-going direction compared to the Au-going direction. Additionally, the nuclear-modification factor in Cu+Au collisions averaged over all centrality is measured to be similar to the previous PHENIX result in $d$+Au collisions for these rapidities.
DOI: 10.17182/hepdata.142075.v1/t4
title: "Figure 8" of "$\phi$ meson production in the forward/backward rapidity region in Cu$+$Au collisions at $\sqrt{s_{NN}}=200$ GeV"

description: The nuclear modification factor $R_{CuAu}$ as a function of the number of participating nucleons for 1.2 &lt; $|y|$ &lt; 2.2 and 1 &lt; $p_T$ &lt; 5 GeV/$c$. Type A represents uncertainties that are uncorrelated from point to point, Type B represents uncertainties that are correlated from point to point, and Type C represents uncertainties in the overall normalization.
description: The PHENIX experiment at the Relativistic Heavy Ion Collider has measured $\phi$ meson production and its nuclear modification in asymmetric Cu+Au heavy-ion collisions at $\sqrt{s_{NN}}$ = 200 GeV at both forward Cu-going direction (1.2 &lt; $y$ &lt; 2.2) and backward Au-going direction (−2.2 &lt; $y$ &lt; −1.2), rapidities. The measurements are performed via the dimuon decay channel and reported as a function of the number of participating nucleons, rapidity, and transverse momentum. In the most central events, 0%–20% centrality, the $\phi$ meson yield integrated over 1 &lt; $p_T$ &lt; 5 GeV/$c$ prefers a smaller value, which means a larger nuclear modification, in the Cu-going direction compared to the Au-going direction. Additionally, the nuclear-modification factor in Cu+Au collisions averaged over all centrality is measured to be similar to the previous PHENIX result in $d$+Au collisions for these rapidities.