cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.69212.v1/t2
title: "Table 2" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Differential cross sections d^2sigma^cent_JPsi/dydpt as function of pt for six centrality classes at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t3
title: "Table 3" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Differential cross sections dsigma^cent_JPsi/dy for four centrality classes at mid-rapidity (-1.37
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t4
title: "Table 4" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Differential cross sections dsigma^cent_JPsi/dy for six centrality classes at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t5
title: "Table 5" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor Q_pA as function of centrality at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t10
title: "Table 10" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor Q_pA as function of pT for six centrality classes at backward (-4.46
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t11
title: "Table 11" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor Q_pA as a function of pT for six centrality classes at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t6
title: "Table 6" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Nuclear modification factor Q_pA as function of centrality in the mid-rapidity range (-1.37
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t7
title: "Table 7" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Values of and for six centrality classes at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t8
title: "Table 8" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Values of and at forward (2.03
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69212.v1/t9
title: "Table 9" of "Centrality dependence of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Values of Delta as a function of centrality at forward (2.03 in pp collisions and is correlated over centrality.
description: CERN-LHC. We present a measurement of inclusive J/$\psi$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV as a function of the centrality of the collision, as estimated from the energy deposited in the Zero Degree Calorimeters. The measurement is performed with the ALICE detector down to zero transverse momentum, $p_{\rm T}$, in the backward ($-4.46 &lt; y_{\rm cms} &lt; -2.96$) and forward ($2.03 &lt; y_{\rm cms} &lt; 3.53$) rapidity intervals in the dimuon decay channel and in the mid-rapidity region ($-1.37 &lt; y_{\rm cms} &lt; 0.43$) in the dielectron decay channel. The backward and forward rapidity intervals correspond to the Pb-going and p-going direction, respectively. The $p_{\rm T}$-differential J/$\psi$ production cross section at backward and forward rapidity is measured for several centrality classes, together with the corresponding average $p_{\rm T}$ and $p^2_{\rm T}$ values. The nuclear modification factor, $Q_{\rm pPb}$, is presented as a function of centrality for the three rapidity intervals, and, additionally, at backward and forward rapidity, as a function of $p_{\rm T}$ for several centrality classes.
DOI: 10.17182/hepdata.69224.v1/t1
title: "Table 1" of "Recoil-proton polarization in π$^−$ -p elastic scattering at 365 MeV"

description: No description provided.
description: THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION'S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED DICKINS64) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// DICKINS64 [D. F. DICKINSON,UCRL-11690(THESIS),1964.] -- PI- P POL AT 485 MEV/C. DOUBLE ARM COUNTER EXPERIMENT DONE AT THE BEVATRON WITH HYDROGEN TARGET AND RESCATTERING OF RECOIL PROTONS IN CARBON ANALYZERS. /// DICKINS65 [D. F. DICKINSON,UCRL-11690-REV.,1965.] -- PREPRINT OF DICKINS66. /// DICKINS66 [D. F. DICKINSON,PL 20,549(1966)] -- /// COMMENTS FROM LOVELACE71 COMPILATION OF THESE DATA -- LOVELACE71 PUTS THIS DATA IN A SPECIAL SECTION RESERVED FOR EXPERIMENTS IN SEVERE DISAGREEMENT WITH OTHERS.
DOI: 10.17182/hepdata.69225.v1/t1
title: "Table 1" of "Proton-proton Elastic Scattering at 8.35 BeV"

description: No description provided.
description: TECHNIQUE USED...BUBBLE/EMULSION.
DOI: 10.17182/hepdata.69225.v1/t2
title: "Table 2" of "Proton-proton Elastic Scattering at 8.35 BeV"

description: No description provided.
description: TECHNIQUE USED...BUBBLE/EMULSION.
DOI: 10.17182/hepdata.69229.v1/t1
title: "Table 1" of "PROTON COMPTON EFFECT"

description: No description provided.
description: THE SCATTERED PHOTON AND RECOIL PROTON WERE DETECTED IN COINCIDENCE IN COUNTER TELESCOPES. PI0 PRODUCTION WAS ELIMINATED BY USING THE COPLANARITY CONDITION. THE DATA ARE TAKEN FROM THE BONN COMPILATION BY GENZEL AND PFEIL.
THE RECOIL PROTON WAS DETECTED IN A COUNTER TELMSCOPE AND SPARK CHAMBERS IN COINCIDENCE WITH ONE DECAY GAMMA.
DOI: 10.17182/hepdata.69229.v1/t2
title: "Table 2" of "PROTON COMPTON EFFECT"

description: No description provided.
description: THE SCATTERED PHOTON AND RECOIL PROTON WERE DETECTED IN COINCIDENCE IN COUNTER TELESCOPES. PI0 PRODUCTION WAS ELIMINATED BY USING THE COPLANARITY CONDITION. THE DATA ARE TAKEN FROM THE BONN COMPILATION BY GENZEL AND PFEIL.
THE RECOIL PROTON WAS DETECTED IN A COUNTER TELMSCOPE AND SPARK CHAMBERS IN COINCIDENCE WITH ONE DECAY GAMMA.
DOI: 10.17182/hepdata.69241.v1/t2
title: "Table 2" of "Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC"

description: Acceptance times efficiency for the loose channel of the Razor analysis for the direct squark-squark model.
description: CERN-LHC. A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.
DOI: 10.17182/hepdata.69241.v1/t1
title: "Table 1" of "Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC"

description: Acceptance for the loose channel of the Razor analysis for the direct squark-squark model.
description: CERN-LHC. A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.
DOI: 10.17182/hepdata.69241.v1/t3
title: "Table 3" of "Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC"

description: Acceptance for the tight channel of the Razor analysis for the direct squark-squark model.
description: CERN-LHC. A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.
DOI: 10.17182/hepdata.69241.v1/t4
title: "Table 4" of "Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC"

description: Acceptance times efficiency for the tight channel of the Razor analysis for the direct squark-squark model.
description: CERN-LHC. A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.
DOI: 10.17182/hepdata.69241.v1/t5
title: "Table 5" of "Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS experiment at the LHC"

description: Acceptance for the 1tau channel of the Taus+jets+MET analysis for the gluino simplified model.
description: CERN-LHC. A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or b-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis. Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models. In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions.