cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.42744.v1/t1
title: "Table 1" of "Observation of exclusive electron positron production in hadron hadron collisions."

description: Exclusive cross section.
description: Fermilab-Tevatron. Measurement of the cross section for exclusive E+ E- production in PBAR P collisions at a centre-of-mass energy of 1960 GeV. 16 events are observed from a sample of integrated luminosity of 532 pb-1.
DOI: 10.17182/hepdata.42758.v1/t1
title: "Table 1" of "Measurement of the inclusive jet cross section using the k(T) algorithm in p anti-p collisions at s**(1/2) = 1.96-TeV"

description: Measured jet differential cross section as a function of PT.
description: Fermilab-Tevatron. Measurement of the inclusive jet production cross section in PBAR P collisions at centre of mass energy 1.96 TeV. The jets are reconstructed using the KT algorithm and come from a data sample of integrated luminosity 385 pb-1 covering the jet ABS(YRAP) range 0.1 to 0.7 and jet transverse momentum 54 to 700 GeV.
DOI: 10.17182/hepdata.42759.v1/t1
title: "Table 1" of "Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV in dilepton final states"

description: TTBAR production cross section.
description: Fermilab-Tevatron. Measurement of the TOP TOPBAR production cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV using Dilepton Final State events. The data come from a sample of integrated luminsoity (234-230)pb-1with two charged leptons in the final state. 13 events were observed with and e xpected background of 3.2+-0.7. The analysis assumes a top quark mass of 175 GeV.
DOI: 10.17182/hepdata.42761.v1/t1
title: "Table 1" of "Measurement of the t anti-t production cross-section in p anti-p collisions at s**(1/2) = 1.96-TeV using lepton plus jets events with semileptonic B decays to muons"

description: TTBAR production cross section.
description: Fermilab-Tevatron. Measurement of the TOP TOPBAR production cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV using Lepton plus Jets events with Semileptonic B-decays to Muons. The data come from a sample of integrated luminsoity 194 pb-1 collected between March 2002 and August 2003 with 20candidates (estimated background of 9.5 +- 1.1) from events with a high transve rse momentum electron or muon, three or more jets, and missing transverse energy. The analysis assumes a top quark mass of 175 GeV.
DOI: 10.17182/hepdata.42762.v1/t1
title: "Table 1" of "Measurement of the t anti-t Production Cross Section in p anti-p Collisions at s**(1/2) = 1.96-TeV"

description: Measured cross section where at least one B quark from the TOP quark decays is identified.
description: Fermilab-Tevatron. Measurement of the TOP TOPBAR pair production cross section in PBAR-P collisions at centre-of-mass energy of 1.96 TeV using a data sample with integrated luminosity 318 pb-1. Data were selected with (E NU JETS) and (MU NU JETS) final states in which at least one B quark from the TOP quark decays is identified using a secondary vertex-finding algorithm. Result assumes TOP quark mass of 178 GeV. Also given is the cross section with significance & gt; 5 sigma in the subsample where both B quarks are identified.
DOI: 10.5281/zenodo.17457701
title: Allocation Factors for Absolute Environmental Sustainability Assessment

description: This dataset includes allocation factors for 163 economic sectors across 44 countries and 5 Rest-of-World regions to determine environmental sustainability thresholds.

The allocation factors are calculated using four economic allocation methods, based on direct or total, and on consumption- or production-based value generated by each sector.

A related publication will be linked once available.

The code to calculate the allocation factors based on EXIOBASE 3 data is available on GitHub: https://github.com/RWTH-LTT/pbaesa
DOI: 10.5281/zenodo.17457702
title: Allocation Factors for Absolute Environmental Sustainability Assessment

description: This dataset includes allocation factors for 163 economic sectors across 44 countries and 5 Rest-of-World regions to determine environmental sustainability thresholds.

The allocation factors are calculated using four economic allocation methods, based on direct or total, and on consumption- or production-based value generated by each sector.

A related publication will be linked once available.

The code to calculate the allocation factors based on EXIOBASE 3 data is available on GitHub: https://github.com/RWTH-LTT/pbaesa
DOI: 10.17182/hepdata.42762.v1/t2
title: "Table 2" of "Measurement of the t anti-t Production Cross Section in p anti-p Collisions at s**(1/2) = 1.96-TeV"

description: Measured cross section where both B quarks from the TOP quark decays are identified.
description: Fermilab-Tevatron. Measurement of the TOP TOPBAR pair production cross section in PBAR-P collisions at centre-of-mass energy of 1.96 TeV using a data sample with integrated luminosity 318 pb-1. Data were selected with (E NU JETS) and (MU NU JETS) final states in which at least one B quark from the TOP quark decays is identified using a secondary vertex-finding algorithm. Result assumes TOP quark mass of 178 GeV. Also given is the cross section with significance & gt; 5 sigma in the subsample where both B quarks are identified.
DOI: 10.17182/hepdata.42763.v1/t1
title: "Table 1" of "Measurement of the ratios of the Z/G* + &gt;= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV"

description: Ratio of the cross sections.
description: Fermilab Tevatron. Measurements of the ratio of the production cross section for events with Z0/GAMMA* plus associated JETS to the total inclusive Z0/GAMMA* cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV. Thedata consist of 14000 Z0/GAMMA*--& gt; E+E- candidates corresponding to a total int egrated luminosity of 0.4 fb-1.
DOI: 10.17182/hepdata.42763.v1/t2
title: "Table 2" of "Measurement of the ratios of the Z/G* + &gt;= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV"

description: Number of observed events per 5 GeV bin for the &gt;=`1Jet sample. Data read from plots.
description: Fermilab Tevatron. Measurements of the ratio of the production cross section for events with Z0/GAMMA* plus associated JETS to the total inclusive Z0/GAMMA* cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV. Thedata consist of 14000 Z0/GAMMA*--& gt; E+E- candidates corresponding to a total int egrated luminosity of 0.4 fb-1.
DOI: 10.15468/dl.d54vfh
title: Occurrence Download

description: A dataset containing 141 species occurrences available in GBIF matching the query:
{
 "and" : [
 "BasisOfRecord is Human Observation",
 "Country is Philippines",
 "HasCoordinate is true",
 "HasGeospatialIssue is false",
 "TaxonKey is Chrysocolaptes haematribon",
 "Year 2000-2009"
 ]
}

 The dataset includes 141 records from 2 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015097-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.42763.v1/t3
title: "Table 3" of "Measurement of the ratios of the Z/G* + &gt;= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV"

description: Number of observed events per 5 GeV bin for the &gt;=2Jet sample. Data read from plots.
description: Fermilab Tevatron. Measurements of the ratio of the production cross section for events with Z0/GAMMA* plus associated JETS to the total inclusive Z0/GAMMA* cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV. Thedata consist of 14000 Z0/GAMMA*--& gt; E+E- candidates corresponding to a total int egrated luminosity of 0.4 fb-1.
DOI: 10.17182/hepdata.42763.v1/t4
title: "Table 4" of "Measurement of the ratios of the Z/G* + &gt;= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV"

description: Number of observed events per 5 GeV bin for the &gt;=3Jet sample. Data read from plots.
description: Fermilab Tevatron. Measurements of the ratio of the production cross section for events with Z0/GAMMA* plus associated JETS to the total inclusive Z0/GAMMA* cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV. Thedata consist of 14000 Z0/GAMMA*--& gt; E+E- candidates corresponding to a total int egrated luminosity of 0.4 fb-1.
DOI: 10.17182/hepdata.42764.v1/t1
title: "Table 1" of "Measurement of the cross section for t anti-t production in p anti-p collisions using the kinematics of lepton + jets events"

description: TTBAR production cross section.
description: Fermilab-Tevatron. Measurement of the TOP TOPBAR production cross section in PBAR P collisions at a centre-of-mass energy of 1.96 TeV using the Kinematicsof Lepton+Jets events requiring one isolated lepton with ET & gt;= 20 GeV, missing transverse energy & gt;= 20 Gev, and three jets with ET & gt;= 15 GeV. The data come from a sample of integrated luminsoity 194(+-11) pb-1 collected between March 2002 and September 2003. The analysis uses an artificial neural network technique to discriminate between background and top topbar production and assumes a top quark mass of 175 GeV.
DOI: 10.17182/hepdata.42774.v1/t1
title: "Table 1" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for HARD events at a centre of massenergy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t2
title: "Table 2" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for MB events at a centre of mass energy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t3
title: "Table 3" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for SOFT events at a centre of massenergy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t4
title: "Table 4" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for HARD events at a centre of massenergy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t5
title: "Table 5" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for MB events at a centre of mass energy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t6
title: "Table 6" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: K0S inclusive invariant PT distribution for SOFT events at a centre of massenergy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t7
title: "Table 7" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for HARD events at a centre of mass energy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t8
title: "Table 8" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for MB events at a centre of mass energy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t10
title: "Table 10" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for HARD events at a centre of mass energy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t11
title: "Table 11" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for MB events at a centre of mass energy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t12
title: "Table 12" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for SOFT events at a centre of mass energy 630 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t9
title: "Table 9" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: LAMBDA inclusive invariant PT distribution for SOFT events at a centre of mass energy 1800 GeV.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t13
title: "Table 13" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of K0S at a centre of mass 1800 GeV for the MB data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t14
title: "Table 14" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of LAMBDA at a centre of mass 1800 GeV for the MB data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t15
title: "Table 15" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of K0S at a centre of mass 1800 GeV for the SOFT data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t16
title: "Table 16" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of LAMBDA at a centre of mass 1800 GeV for the SOFT data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t17
title: "Table 17" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of K0S at a centre of mass 1800 GeV for the HARD data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.
DOI: 10.17182/hepdata.42774.v1/t18
title: "Table 18" of "K0(s) and Lambda0 production studies in p anti-p collisions at s**(1/2) = 1800 and 630-GeV"

description: Average PT of LAMBDA at a centre of mass 1800 GeV for the HARD data sample.
description: Fermilab-Tevatron. Study of the production of K0S and LAMBDA in elastic PBAR P collisions at centre of mass energies 1800 and 630 GeV. The data are dividedinto Minimum Bias (MB), SOFT and HARD events. SOFT events are defined as having no cluster of jet energy & gt; 1.1 GeV. HARD events are those which have at least o ne cluster of jet energy & gt; 1.1 GeV. Jets are defined by a cone algorithm with R = 0.7. The 1800 GeV data are collected in Runs 1A(1992-93), 1B(1995-95) and 1C(1995-96) and the 630 GeV data in run 1C.. Numerical values supplied by N.Moggi.