cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.55309.v1/t3
title: "Table 3" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DQ**2 for inclusive jet production using the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t4
title: "Table 4" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DQ**2 for inclusive jet production using the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t5
title: "Table 5" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 125 to 250 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t7
title: "Table 7" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 500 to 1000 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.15468/dl.sttdm5
title: Occurrence Download

description: A dataset containing 181 species occurrences available in GBIF matching the query:
{
 "and" : [
 "OccurrenceStatus is Present",
 "TaxonKey is Aloe ciliaris"
 ]
}

 The dataset includes 181 records from 55 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015202-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.55309.v1/t10
title: "Table 10" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 5000 to 100000 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t11
title: "Table 11" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 125 to 250 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t13
title: "Table 13" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 500 to 1000 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t6
title: "Table 6" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 250 to 500 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t8
title: "Table 8" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 1000 to 2000 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t9
title: "Table 9" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 2000 to 5000 GeV for the anti-KT jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t12
title: "Table 12" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 250 to 500 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t14
title: "Table 14" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 1000 to 2000 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t15
title: "Table 15" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 2000 to 5000 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55309.v1/t16
title: "Table 16" of "Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms"

description: The measured differential cross section DSIG/DET for inclusive jet production in the Q**2 region 5000 to 100000 GeV for the SIScone jet algorithm.
description: DESY-HERA. Measurement of the differential inclusive-jet cross sections in neutral current deep inelastic scattering of 27.5 electrons and positrons on 920 GeV proton at a centre of mass energy 319 GeV using the anti-KT and SIScone jet algorithm in the Breit frame. The data, with an integrated luminosity of 81.7 pb-1 (16.7 pb-1 E- P, 65.0 pb-1 E+ P), were collected during the 1998- 2000 running periods. Values of the strong coupling constant ALPHAS have been extracted from the data. In the tables of cross sections the first DSYS error is the uncorrelated systematic error and the second is the jet-energy-scale uncertainty. The angle GAMMA(H) is the angle of the scattered quark in the quark-parton model and is reconstructed using the hadronic final state.
DOI: 10.17182/hepdata.55315.v1/t1
title: "Table 1" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: The K+ double-differential cross section at each of the 5 beam energies intgerated over momentum bins of width +- 12 MeV/c. Note the errors do not include the 7 PCT systematic uncertainty coming from the normalization.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55315.v1/t2
title: "Table 2" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: Total cross section for the P P --&gt; K+ P LAMBDA.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55315.v1/t4
title: "Table 4" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: Total cross section for the P P --&gt; K+ N SIGMA+ from the K+ PI+ coincidence data sample.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55315.v1/t5
title: "Table 5" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: Total cross section for the P P --&gt; K+ N SIGMA+ from the K+ P missing mass spectra data sample. Note that in this case it is difficult to quantify the systematic errors (see discussion in text of paper).;.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55315.v1/t6
title: "Table 6" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: Upper limit estimates for the P P --&gt; K+ N SIGMA+ total cross section.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55317.v1/t1
title: "Table 1" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Differential cross section for the K- P --&gt; GAMMA LAMBDA reaction at thelower beam momenta.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55317.v1/t2
title: "Table 2" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Differential cross section for the K- P --&gt; GAMMA LAMBDA reaction at thehigher beam momenta.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55315.v1/t3
title: "Table 3" of "The energy dependence of the pp-&gt;K+ n Sigma+ reaction close to threshold"

description: Total cross section for the P P --&gt; K+ P SIGMA0.
description: COSY Accelerator Julich. Measurement of the cross sections for the reaction P P --&gt; K+ N SIGMA+ at four energies (1.826, 1.920, 1.958 and 2.020 GeV) close to threshold.
DOI: 10.17182/hepdata.55317.v1/t3
title: "Table 3" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Differential cross section for the K- P --&gt; GAMMA SIGMA0 reaction at thelower beam momenta.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55317.v1/t4
title: "Table 4" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Differential cross section for the K- P --&gt; GAMMA SIGMA0 reaction at thehigher beam momenta.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55317.v1/t5
title: "Table 5" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Legendre polynomial coefficients for the K- P --&gt; GAMMA LAMBDA reaction.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55317.v1/t6
title: "Table 6" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Legendre polynomial coefficients for the K- P --&gt; GAMMA SIGMA0 reaction.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55317.v1/t7
title: "Table 7" of "Measurement of $K^- p$ radiative capture to $\gamma \Lambda$ and $\gamma \Sigma^0$ for $p_{K^-}$ between 514 and 750 MeV/$c$"

description: Total cross section as a function of beam momenta and centre of massenergy.
description: BNL-AGS. Measurement of the differential cross sections in the radiativereactions K- P --&gt;GAMMA LAMBDA and K- P --&gt; GAMMA SIGMA0 at incident K- momentabetween 514 and 750 MeV.
DOI: 10.17182/hepdata.55368.v1/t1
title: "Table 1" of "Scaled momentum spectra in deep inelastic scattering at HERA"

description: Bin averaged scaled momentum spectra in the Q**2 ranges 160 to 320 and 320 to 640 GeV**2.
description: DESY-HERA. Measurement of charged particle production in neutral current deep inelastic scattering of 27.5 GeV electrons and positrons on 820 and 920 GeV protons equivelent to centre of mass energies 300 and 318 GeV. Scaled momentum distributions in the Breit frame are presented in the Q**2 range 10 to 41000 GeV**2. The data which have atotal integrated luminosity of 0.44 fb-1 were collected from 1995 to 2007.
DOI: 10.17182/hepdata.55368.v1/t2
title: "Table 2" of "Scaled momentum spectra in deep inelastic scattering at HERA"

description: Bin averaged scaled momentum spectra in the Q**2 ranges 640 to 1280 and 1280 to 2560 GeV**2.
description: DESY-HERA. Measurement of charged particle production in neutral current deep inelastic scattering of 27.5 GeV electrons and positrons on 820 and 920 GeV protons equivelent to centre of mass energies 300 and 318 GeV. Scaled momentum distributions in the Breit frame are presented in the Q**2 range 10 to 41000 GeV**2. The data which have atotal integrated luminosity of 0.44 fb-1 were collected from 1995 to 2007.
DOI: 10.17182/hepdata.55368.v1/t3
title: "Table 3" of "Scaled momentum spectra in deep inelastic scattering at HERA"

description: Bin averaged scaled momentum spectra in the Q**2 ranges 2560 to 5120 and 51200 to 10240 GeV**2.
description: DESY-HERA. Measurement of charged particle production in neutral current deep inelastic scattering of 27.5 GeV electrons and positrons on 820 and 920 GeV protons equivelent to centre of mass energies 300 and 318 GeV. Scaled momentum distributions in the Breit frame are presented in the Q**2 range 10 to 41000 GeV**2. The data which have atotal integrated luminosity of 0.44 fb-1 were collected from 1995 to 2007.