cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.229.v1/t8
title: "Table 8" of "Measurements of polarization in pi- p elastic scattering at large angles"

description: No description provided.
description: THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BURLESON71) 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.) /// ASBURY69 [J. G. ASBURY,PRL 23,194(1969)] -- K+ P POL EXPERIMENT USING SIMILAR EQUIPMENT TO PI P EXPERIMENTS. CONTAINS MORE DETAILED DESCRIPTION OF APPARATUS THAN BURLESON71 OR HILL71. /// BURLESON71 [G. BURLESON,PRL 26,338(1971)] -- PI+ P POL AT 1.60,1.80,2.11,AND 2.31 GEV/C. DONE AT ZGS WITH ETHYLENE GLYCOL TARGET AND COUNTER HODOSCOPES IN COINCIDENCE. /// HILL71 [D. HILL,PRL 27,1241(1971)] -- PI- P POL AT 1.60,1.70,1.88,2.07,AND 2.28 GEV/C. SIMILAR SETUP TO BURLESON71. /// YOKOSAWA74 [A. YOKOSAWA,PRIV. COMM.,1974.] -- TABLES OF DATA FROM BURLESON71 AND HILL71. IN THE PI+ P DATA AT 1.60 AND 1.80 GEV/C THE VALUE OF T FOR THE DATA POINT NEAREST 180 DEGREES IS APPARENTLY MISPRINTED. THESE TWO T VALUES HAVE BEEN CHANGED TO AGREE WITH THE PLOTS IN BURLESON71.LOVELACE71 HAS ALL THE PI+ P DATA (LOVELACE71 ID=BURLES71),AND A SPOT CHECK INDICATES AGREEMENT WITH THE YOKOSAWA74 TABLES (WITH THE ABOVE CORRECTIONS AT 1.60 AND 1.80 GEV/C).THE ONLY PI- P DATA ARE SOME APPARENTLY PRELIMINARY RESULTS AT 1.88 GEV/C (LOVELACE71 ID=YOKOSA71) WHICH DO NOT AGREE WITH YOKOSAWA74.
DOI: 10.17182/hepdata.229.v1/t9
title: "Table 9" of "Measurements of polarization in pi- p elastic scattering at large angles"

description: No description provided.
description: THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION& apos;S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BURLESON71) 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.) /// ASBURY69 [J. G. ASBURY,PRL 23,194(1969)] -- K+ P POL EXPERIMENT USING SIMILAR EQUIPMENT TO PI P EXPERIMENTS. CONTAINS MORE DETAILED DESCRIPTION OF APPARATUS THAN BURLESON71 OR HILL71. /// BURLESON71 [G. BURLESON,PRL 26,338(1971)] -- PI+ P POL AT 1.60,1.80,2.11,AND 2.31 GEV/C. DONE AT ZGS WITH ETHYLENE GLYCOL TARGET AND COUNTER HODOSCOPES IN COINCIDENCE. /// HILL71 [D. HILL,PRL 27,1241(1971)] -- PI- P POL AT 1.60,1.70,1.88,2.07,AND 2.28 GEV/C. SIMILAR SETUP TO BURLESON71. /// YOKOSAWA74 [A. YOKOSAWA,PRIV. COMM.,1974.] -- TABLES OF DATA FROM BURLESON71 AND HILL71. IN THE PI+ P DATA AT 1.60 AND 1.80 GEV/C THE VALUE OF T FOR THE DATA POINT NEAREST 180 DEGREES IS APPARENTLY MISPRINTED. THESE TWO T VALUES HAVE BEEN CHANGED TO AGREE WITH THE PLOTS IN BURLESON71.LOVELACE71 HAS ALL THE PI+ P DATA (LOVELACE71 ID=BURLES71),AND A SPOT CHECK INDICATES AGREEMENT WITH THE YOKOSAWA74 TABLES (WITH THE ABOVE CORRECTIONS AT 1.60 AND 1.80 GEV/C).THE ONLY PI- P DATA ARE SOME APPARENTLY PRELIMINARY RESULTS AT 1.88 GEV/C (LOVELACE71 ID=YOKOSA71) WHICH DO NOT AGREE WITH YOKOSAWA74.
DOI: 10.17182/hepdata.238.v1/t1
title: "Table 1" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t2
title: "Table 2" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t3
title: "Table 3" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t4
title: "Table 4" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t5
title: "Table 5" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t7
title: "Table 7" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t8
title: "Table 8" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t10
title: "Table 10" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t11
title: "Table 11" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t12
title: "Table 12" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t13
title: "Table 13" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t14
title: "Table 14" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t6
title: "Table 6" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t9
title: "Table 9" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t15
title: "Table 15" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t16
title: "Table 16" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t17
title: "Table 17" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: No description provided.
description: ARGONNE.
DOI: 10.17182/hepdata.238.v1/t18
title: "Table 18" of "Differential cross sections for elastic pi+ p scattering between 1.2 and 2.3 GeV/c"

description: THE ERRORS INCLUDE THE 2 TO 5 PCT SYSTEMATIC UNCERTAINTY. OBTAINED FROM THE LEGENDRE POLYNOMIAL FITS TO D(SIG)/DOMEGA.
description: ARGONNE.
DOI: 10.17182/hepdata.248.v1/t1
title: "Table 1" of "Nuclear Cross Sections for 1.4-Bev Neutrons"

description: 'ALL'.
description: TECHNIQUE USED...D2O AND H2O TARGETS.
DOI: 10.17182/hepdata.248.v1/t2
title: "Table 2" of "Nuclear Cross Sections for 1.4-Bev Neutrons"

description: No description provided.
description: TECHNIQUE USED...D2O AND H2O TARGETS.
DOI: 10.17182/hepdata.249.v1/t1
title: "Table 1" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)] for $2.0 &lt; y &lt; 2.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t2
title: "Table 2" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)] for $2.0 &lt; y &lt; 2.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t3
title: "Table 3" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t4
title: "Table 4" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $2.0 &lt; y &lt; 4.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t6
title: "Table 6" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t10
title: "Table 10" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y )$ for $p_T &lt; 30$ GeV/$c$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t5
title: "Table 5" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}y$ [pb] for $p_T &lt; 30$ GeV.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t7
title: "Table 7" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t8
title: "Table 8" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t9
title: "Table 9" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T )$ for $2.0 &lt; y &lt; 4.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t11
title: "Table 11" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t12
title: "Table 12" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t13
title: "Table 13" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t14
title: "Table 14" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $2.0 &lt; y &lt; 4.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t15
title: "Table 15" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}y$ [pb] for $p_T &lt; 30$ GeV.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t16
title: "Table 16" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t17
title: "Table 17" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t18
title: "Table 18" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t19
title: "Table 19" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T )$ for $2.0 &lt; y &lt; 4.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t20
title: "Table 20" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y )$ for $p_T &lt; 30$ GeV/$c$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0
DOI: 10.17182/hepdata.249.v1/t21
title: "Table 21" of "Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV"

description: The ratio of differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $\sqrt{s}=8$ and $\sqrt{s}=7$ TeV in $2.0 &lt; y &lt; 4.5$.
description: CERN-LHCb.The production of $\Upsilon$ mesons in $pp$ collisions 
 at $\sqrt{s}=7$ and $8$ TeV is studied with the LHCb detector using data samples corresponding 
 to an integrated luminosity of 1 fb$^{-1}$ and 2 fb$^{-1}$ respectively. The production cross-sections
 and ratios of cross-sections are measured as functions of the meson transverse momentum
 $p_T$ and rapidity $y$, for $p_T &lt; 30$ GeV/$c$ and $2.0