cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.12253.v1/t39
title: "Table 39" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t40
title: "Table 40" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t41
title: "Table 41" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t42
title: "Table 42" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t43
title: "Table 43" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t44
title: "Table 44" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t45
title: "Table 45" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.17182/hepdata.12253.v1/t46
title: "Table 46" of "A kinematically complete measurement of the proton structure function F2 in the resonance region and evaluation of its moments."

description: No description provided.
description: Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV and have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolution of its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
Jefferson Lab-CEBAF. Measurement of the structure function F2 from the inclusive cross sections measured in interactions of electrons with a liquid hydrogen target. The data are collected with electron beam energies 1.5, 2.5, 4.0, 4.2 and 4.4 GeV andd have W & lt; 2.5 GeV and momentum transfers Q**2 below 4.5 GeV**2. The authors combine these data with other world data to study the Q**2 evolutionof its moments and higher twist effects.. PART 1 contains data with Q**2 from 0.225 to 1 Gev**2.. PART 2 contains data with Q**2 from 1 to 2 Gev**2.. PART 3 contains data with Q**2 from 2 to 3 Gev**2.. PART 4 contains data with Q**2 from 3 to 4 Gev**2.. PART 5 contains data with Q**2 from 4 to 4.725 Gev**2.. Numerical values suppied by M Osipenko.. This data were taken in Run Period E1 in Hall-B.
DOI: 10.15468/dl.cxcufp
title: Occurrence Download

description: A dataset containing 174 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Lechea maritima maritima"
 ]
}

 The dataset includes 174 records from 13 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0014881-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.12261.v1/t2
title: "Table 2" of "First measurement of the quark to photon fragmentation function"

description: 2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t3
title: "Table 3" of "First measurement of the quark to photon fragmentation function"

description: 2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t5
title: "Table 5" of "First measurement of the quark to photon fragmentation function"

description: 3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t6
title: "Table 6" of "First measurement of the quark to photon fragmentation function"

description: 3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t1
title: "Table 1" of "First measurement of the quark to photon fragmentation function"

description: 2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t4
title: "Table 4" of "First measurement of the quark to photon fragmentation function"

description: 2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t7
title: "Table 7" of "First measurement of the quark to photon fragmentation function"

description: 3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t9
title: "Table 9" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t10
title: "Table 10" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t11
title: "Table 11" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t12
title: "Table 12" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t13
title: "Table 13" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t14
title: "Table 14" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t15
title: "Table 15" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.17182/hepdata.12261.v1/t16
title: "Table 16" of "First measurement of the quark to photon fragmentation function"

description: No description provided.
description: CERN-ALEPH. First measurement of the quark-to-photon fragmentation function. Hard photons treated & apos;democratically& apos; as other particles formed hadron jets.. DURHAM E0 algorithm used for particle clustering. Two-jets normalized differential rate was used for extraction of the quark-to-photon fragmentation function.
DOI: 10.48597/p48z-72fj
title: Measurement of Mercury at Kosetice (NAOK)

description: Measurement of Mercury at Kosetice (NAOK)