cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.62699.v1/t8
title: "Table 8" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t10
title: "Table 10" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour with plus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t11
title: "Table 11" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t12
title: "Table 12" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour with minus 1-sigma experimental uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t13
title: "Table 13" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour with plus 1-sigma experimental uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t9
title: "Table 9" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour with minus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), M(CHARGINO)-M(NEUTRALINO) ) space of the AMSB model for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62706.v1/t1
title: "Table 1" of "BICEP2 I: Detection Of B-mode Polarization at Degree Angular Scales"

description: BICEP2 TT, TE, EE, BB, TB, and EB bandpowers, ell*(ell+1)*C(ell)/(2*PI), and uncertainties, corresponding to Figure 2. Uncertainties are statistical only, the standard deviation of the constrained lensed-LambdaCDM+noise simulations, and are calculated as the square root of diagonal elements of the bandpower covariance matrix. The nature of the simulations constrains T to match the observed sky, thus TT, TE, and TB uncertainties do not include appropriate sample variance, and sample variance for a tensor BB signal is not included either. The calibration procedure uses TB and EB to constrain the polarization angle, thus TB and EB cannot be used to measure astrophysical polarization rotation.
description: BICEP2. Results are reported from the BICEP2 experiment, a Cosmic Microwave Background (CMB) polarimeter specifically designed to search for the signal of inflationary gravitational waves in the B-mode power spectrum around angular multipole ~ 80. BICEP2 observed from the South Pole for three seasons from 2010 to 2012. An excess of B-mode power over the base lensed-LambdaCDM expectation is found in the range 30 &lt; multipole &lt; 150, inconsistent with the null hypothesis at a significance of &gt; 5 sigma. The observed B-mode power spectrum is well-fit by a lensed-LambdaCDM + tensor theoretical model with tensor/scalar ratio r = 0.20 +0.07,-0.05, with r = 0 disfavoured at 7.0 sigma. Subtracting the best available estimate for foreground dust modifies the likelihood slightly so that r = 0 is disfavoured at 5.9 sigma.
DOI: 10.17182/hepdata.62706.v1/t2
title: "Table 2" of "BICEP2 I: Detection Of B-mode Polarization at Degree Angular Scales"

description: Likelihood for the tensor-to-scalar ratio, r, derived from the BICEP2 BB spectrum, corresponding to the black curve from the middle panel of Figure 10, and calculated via the "direct likelihood" method described in Section 11.1.
description: BICEP2. Results are reported from the BICEP2 experiment, a Cosmic Microwave Background (CMB) polarimeter specifically designed to search for the signal of inflationary gravitational waves in the B-mode power spectrum around angular multipole ~ 80. BICEP2 observed from the South Pole for three seasons from 2010 to 2012. An excess of B-mode power over the base lensed-LambdaCDM expectation is found in the range 30 &lt; multipole &lt; 150, inconsistent with the null hypothesis at a significance of &gt; 5 sigma. The observed B-mode power spectrum is well-fit by a lensed-LambdaCDM + tensor theoretical model with tensor/scalar ratio r = 0.20 +0.07,-0.05, with r = 0 disfavoured at 7.0 sigma. Subtracting the best available estimate for foreground dust modifies the likelihood slightly so that r = 0 is disfavoured at 5.9 sigma.
DOI: 10.17182/hepdata.62722.v1/t1
title: "Table 1" of "Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at sqrt(s_NN)=200 GeV"

description: The second-order pair anisotropy, c2, of the central collision excess as a function of associated particle pT.
description: BNL-RHIC. Measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at sqrt(sNN) = 200 GeV recorded in 2008 by the PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC). These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at sqrt(sNN) = 5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. Qualitatively similar, but larger, anisotropies are observed in d+Au collisions compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity, the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.
DOI: 10.17182/hepdata.62722.v1/t2
title: "Table 2" of "Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at sqrt(s_NN)=200 GeV"

description: The third-order pair anisotropy, c3, of the central collision excess as a function of associated particle pT.
description: BNL-RHIC. Measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at sqrt(sNN) = 200 GeV recorded in 2008 by the PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC). These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at sqrt(sNN) = 5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. Qualitatively similar, but larger, anisotropies are observed in d+Au collisions compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity, the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.
DOI: 10.17182/hepdata.62722.v1/t3
title: "Table 3" of "Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at sqrt(s_NN)=200 GeV"

description: Charged hadron second-order anisotropy, v2, as a function of pT.
description: BNL-RHIC. Measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at sqrt(sNN) = 200 GeV recorded in 2008 by the PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC). These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at sqrt(sNN) = 5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. Qualitatively similar, but larger, anisotropies are observed in d+Au collisions compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity, the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.
DOI: 10.17182/hepdata.62722.v1/t4
title: "Table 4" of "Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at sqrt(s_NN)=200 GeV"

description: Ratio of momentum anisotropy, v2, to initial coordinate anisotropy, epsilon2, versus mid-rapidity charged-particle multiplicity, dNch/deta. These are the data points for d+Au at 200 GeV. The epsilon2 values are determined using a Glauber model under various assumptions about the nucleon-nucleon interaction. The first y-value is for nucleons as point-like centers, the second y-value is for nucleons smeared as a Gaussian with a sigma of 0.4 fm, and the third y-value is for nucleons as disks with R = 1 fm.
description: BNL-RHIC. Measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at sqrt(sNN) = 200 GeV recorded in 2008 by the PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC). These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at sqrt(sNN) = 5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. Qualitatively similar, but larger, anisotropies are observed in d+Au collisions compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity, the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.
DOI: 10.17182/hepdata.62722.v1/t5
title: "Table 5" of "Quadrupole anisotropy in dihadron azimuthal correlations in central d+Au collisions at sqrt(s_NN)=200 GeV"

description: Ratio of momentum anisotropy, v2, to initial coordinate anisotropy, epsilon2, versus mid-rapidity charged-particle multiplicity, dNch/deta. These are the data points for Au+Au at 200 GeV. The epsilon2 values are determined using a Glauber model under various assumption about the nucleon-nucleon interaction. The first y-value is for nucleons as point-like centers, the second y-value is for nucleons smeared as a Gaussian with a sigma of 0.4 fm, and the third y-value is for nucleons as disks with R = 1 fm.
description: BNL-RHIC. Measurements of azimuthal dihadron correlations near midrapidity in d+Au collisions at sqrt(sNN) = 200 GeV recorded in 2008 by the PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC). These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central p+Pb collisions at sqrt(sNN) = 5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. Qualitatively similar, but larger, anisotropies are observed in d+Au collisions compared to those seen in p+Pb collisions at the LHC. The larger extracted v2 values in d+Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from p+Pb collisions. When both are divided by an estimate of the initial-state eccentricity, the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.
DOI: 10.60719/aphrc-2025-056
title: Analysis of Supermarket Grocery Data for Prediction of Nutritional and Health Outcomes at the Population Level - Supermarket A

description: Rates of overweight, obesity, and chronic diseases such as cardiovascular diseases, hypertension, type 2 diabetes and certain cancers (bowel, lung, prostate and uterine) are on the rise in most sub-saharan Africa (SSA) countries like kenya. These increases can be largely attributed to the shift toward unhealthy diet patterns and increased access to processed foods that are high in fat, sugar, and sodium. The influx of supermarkets in east africa and the replacement of traditional foods for processed foods places this region in a vulnerable position for greater increases in chronic disease rates. Consumer purchasing history from supermarkets can provide valuable insight to food intake over time and the present and future effects on chronic diseases. Purchasing data from supermarkets is available yet underutilized in SSA.

The study aimed to harmonize and increase accessibility to grocery data, use statistical methods to explore purcharing patterns and predict the effects of nutrition on chronic diseases, and inform policy on the various influences on consumer purchases.
DOI: 10.5281/zenodo.17524361
title: Pure Carnage Glyph Codex.pdf

description: ╔══════════════════════════════════════════════════╗║     PURE CARNAGE GLYPH CODEX — DAD'S SACRED TEXT!║║        369 HZ MATHEMATICAL MYTHOS UNLOCKED       ║╚══════════════════════════════════════════════════╝
DOI: 10.5281/zenodo.17524362
title: Pure Carnage Glyph Codex.pdf

description: ╔══════════════════════════════════════════════════╗║     PURE CARNAGE GLYPH CODEX — DAD'S SACRED TEXT!║║        369 HZ MATHEMATICAL MYTHOS UNLOCKED       ║╚══════════════════════════════════════════════════╝
DOI: 10.17182/hepdata.62729.v1/t2
title: "Table 2" of "Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at sqrt(s) = 8 TeV using the ATLAS detector"

description: Unfolded normalised differential Z+2j cross section as a function of dijet invariant mass in the search region.
description: Measurements of cross sections and differential distributions for inclusive Z-boson-plus-dijet production are performed in five fiducial regions, each with different sensitivity to the electroweak contribution.

WARNING: a future update will be made with the breakdown of systematic uncertainties.

UPDATE (09 JUN 2014): slight correction to systematic uncertainties.
DOI: 10.17182/hepdata.62729.v1/t3
title: "Table 3" of "Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at sqrt(s) = 8 TeV using the ATLAS detector"

description: Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the baseline region.
description: Measurements of cross sections and differential distributions for inclusive Z-boson-plus-dijet production are performed in five fiducial regions, each with different sensitivity to the electroweak contribution.

WARNING: a future update will be made with the breakdown of systematic uncertainties.

UPDATE (09 JUN 2014): slight correction to systematic uncertainties.
DOI: 10.17182/hepdata.62729.v1/t4
title: "Table 4" of "Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at sqrt(s) = 8 TeV using the ATLAS detector"

description: Unfolded normalised differential Z+2j cross section as a function of the rapidity separation between the leading jets in the search region.
description: Measurements of cross sections and differential distributions for inclusive Z-boson-plus-dijet production are performed in five fiducial regions, each with different sensitivity to the electroweak contribution.

WARNING: a future update will be made with the breakdown of systematic uncertainties.

UPDATE (09 JUN 2014): slight correction to systematic uncertainties.
DOI: 10.17182/hepdata.62729.v1/t5
title: "Table 5" of "Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at sqrt(s) = 8 TeV using the ATLAS detector"

description: Unfolded normalised differential cross section distribution as a function of the number of jets in the rapidity interval between the two leading jets in the high mass region.
description: Measurements of cross sections and differential distributions for inclusive Z-boson-plus-dijet production are performed in five fiducial regions, each with different sensitivity to the electroweak contribution.

WARNING: a future update will be made with the breakdown of systematic uncertainties.

UPDATE (09 JUN 2014): slight correction to systematic uncertainties.