cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.106472.v1/t10
title: "Figure 2-10" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, $p+p$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t11
title: "Figure 3-1" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 0% to 5% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t12
title: "Figure 3-2" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 0% to 10% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t13
title: "Figure 3-3" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 10% to 20% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t14
title: "Figure 3-4" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 0% to 20% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t15
title: "Figure 3-5" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 20% to 40% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t16
title: "Figure 3-6" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 40% to 60% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t17
title: "Figure 3-7" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 20% to 60% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t9
title: "Figure 2-9" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $E\frac{dN^3}{dp^3}$ vs. $p_T$, 0% to 92% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.21227/e1ph-yf38
title: "Tor Measurement Analysis"

description: "The security and anonymity guarantees of the Tornetwork are fundamentally linked to its network-layer topology,yet few studies have been grounded in large-scale, empiricalmeasurements of its live operation. This paper presents a datasetand a structural analysis of the live Tor network. We introducea dataset of 88,121 circuits, ethically collected over a four-week period from non-exit relays to capture real-world relayselection patterns. Our analysis provides two key insights intoTor\u2019s structure at the network layer. First, we find a high degreeof role specialization, with very few relays serving in multipleroles (e.g., as both a Middle and Exit node). Second, we providea quantitative measurement of structural centralization, findingthat traffic is moderately concentrated on high-bandwidth relays.By publishing this dataset and its initial findings, we provide acritical resource for the research community and establish anempirical baseline for developing more accurate, data drivenunderstanding of Tor\u2019s security and performance."
DOI: 10.17182/hepdata.106472.v1/t18
title: "Figure 3-8" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 60% to 92% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t19
title: "Figure 3-9" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$, 0% to 92% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t20
title: "Figure 4-1" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\pi^{0}}$ $R_{AA}$, 0% to 92% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t21
title: "Figure 4-2" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ ${R_{AA}}$, 0% to 92% centrality $Au+Au$.
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t22
title: "Figure 5-1" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$ vs centrality ($p_T&gt;$20 GeV/c).
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t23
title: "Figure 5-2" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: ${\eta}$ $R_{AA}$ vs centrality ($p_T&gt;$5 GeV/c).
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t24
title: "Figure 5-3" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: Slope ${\eta}$ $R_{AA}$ ($5
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106472.v1/t25
title: "Figure 5-4" of "Transverse momentum dependence of meson suppression in Au+Au collisions at sqrt(s_NN) = 200 GeV"

description: $\chi^{2}/{NDF}$, Prob%, ${\eta}$ $R_{AA}$ ($5$ 5 GeV/c) Prob vs centrality
description: BNL-RHIC. New measurements by the PHENIX experiment at RHIC for $\eta$ production at midrapidity as a function of transverse momentum ($p_T$) and collision centrality in $\sqrt{s_{NN}}=200$ GeV Au+Au and $p+p$ collisions are presented. They indicate nuclear modification factors ($R_{\rm AA}$) which are similar both in magnitude and trend to those found in earlier $\pi^{0}$ measurements. Linear fits to $R_{\rm AA}$ as a function of $p_T$ in 5--20 GeV/$c$ show that the slope is consistent with zero within two standard deviations at all centralities although a slow rise cannot be excluded. Having different statistical and systematic uncertainties, the $\pi^{0}$ and $\eta$ measurements are complementary at high $p_T$; thus, along with the extended $p_T$ range of these data they can provide additional constraints for theoretical modeling and the extraction of transport properties.
DOI: 10.17182/hepdata.106641.v1/t1
title: "Table 1" of "Measurement of the very rare $K^+\rightarrow\pi^+\nu\bar{\nu}$ decay"

description: Observed and expected upper limits on branching ratio \(K^{+}\rightarrow\pi^{+}X\) at 90% CL.
description: Upper limits at 90% CL on Branching Ratio of \(K^{+}\rightarrow\pi^{+}X\), and on couplings \(sin^2(\theta)\), vs mass from a search at the NA62 experiment at the CERN SPS.
DOI: 10.17182/hepdata.106641.v1/t2
title: "Table 2" of "Measurement of the very rare $K^+\rightarrow\pi^+\nu\bar{\nu}$ decay"

description: Observed upper limits on branching ratio \(K^{+}\rightarrow\pi^{+}X\) at 90% CL as functions of X mass and lifetime.
description: Upper limits at 90% CL on Branching Ratio of \(K^{+}\rightarrow\pi^{+}X\), and on couplings \(sin^2(\theta)\), vs mass from a search at the NA62 experiment at the CERN SPS.
DOI: 10.17182/hepdata.106641.v1/t3
title: "Table 3" of "Measurement of the very rare $K^+\rightarrow\pi^+\nu\bar{\nu}$ decay"

description: Exclusion region limits on coupling strength \(sin^{2}\theta\) at 90% CL as a function of X mass, for visible X decays.
description: Upper limits at 90% CL on Branching Ratio of \(K^{+}\rightarrow\pi^{+}X\), and on couplings \(sin^2(\theta)\), vs mass from a search at the NA62 experiment at the CERN SPS.
DOI: 10.17182/hepdata.106642.v1/t1
title: "Table 1" of "Measurements of angular distance and momentum ratio distributions in three-jet and Z + two-jet final states in pp collisions"

description: Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ &lt; 1.0)
description: Collinear (small-angle) and large-angle, as well as soft and hard radiations are investigated in three-jet and Z + two-jet events collected in proton-proton collisions at the LHC. The normalized production cross sections are measured as a function of the ratio of transverse momenta of two jets and their angular separation. The measurements in the three-jet and Z + two-jet events are based on data collected at a center-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.8 $\mathrm{fb}^{-1}$. The Z + two-jet events are reconstructed in the dimuon decay channel of the Z boson. The three-jet measurement is extended to include $\sqrt(s) = 13$ TeV data corresponding to an integrated luminosity of 2.3 $\mathrm{fb}^{-1}$. The results are compared to predictions from event generators that include parton showers, multiple parton interactions, and hadronization. The collinear and soft regions are in general well described by parton showers, whereas the regions of large angular separation are often best described by calculations using higher-order matrix elements.
DOI: 10.17182/hepdata.106642.v1/t2
title: "Table 2" of "Measurements of angular distance and momentum ratio distributions in three-jet and Z + two-jet final states in pp collisions"

description: Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ &gt; 1.0)
description: Collinear (small-angle) and large-angle, as well as soft and hard radiations are investigated in three-jet and Z + two-jet events collected in proton-proton collisions at the LHC. The normalized production cross sections are measured as a function of the ratio of transverse momenta of two jets and their angular separation. The measurements in the three-jet and Z + two-jet events are based on data collected at a center-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.8 $\mathrm{fb}^{-1}$. The Z + two-jet events are reconstructed in the dimuon decay channel of the Z boson. The three-jet measurement is extended to include $\sqrt(s) = 13$ TeV data corresponding to an integrated luminosity of 2.3 $\mathrm{fb}^{-1}$. The results are compared to predictions from event generators that include parton showers, multiple parton interactions, and hadronization. The collinear and soft regions are in general well described by parton showers, whereas the regions of large angular separation are often best described by calculations using higher-order matrix elements.