cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.49386.v1/t3
title: "Table 3" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: No description provided.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t4
title: "Table 4" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: No description provided.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t5
title: "Table 5" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: No description provided.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t6
title: "Table 6" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Transverse energy flow outside the jets in the rapidity region abs(etarap*)&lt;1.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t7
title: "Table 7" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 3 to 6 GeV.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t10
title: "Table 10" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 12 to 20 GeV.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t11
title: "Table 11" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the mean ET of the jets.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t12
title: "Table 12" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Fraction of the transverse energy of the jets inside a cone of radious 0.5 around the jet axis as a function of the jet rapidity.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t13
title: "Table 13" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- &lt;0.8.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t14
title: "Table 14" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R for X(C=GAMMA)+- &gt; 0.8.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t8
title: "Table 8" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 6 to 9 GeV.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49386.v1/t9
title: "Table 9" of "Dijet production in photon-photon collisions at S**(1/2)(ee) = 161-GeV and 172-GeV"

description: Measured jet shape (PSI), corrected to the hadron level for each of the two highest ET jets as a function of the cone radius R in the region of mean ET from 9 to 12 GeV.
description: CERN-LEP. Measurement of 2-jet production in photon-photon collisions at centre-of mass energies of the incoming electron beams of 161 and 172 GeV.. X(C=GAMMA), which specifies the fraction of the photon& apos;s momentum participating in the hard scattering, and is used in the paper to identify & apos;direct& apos; and & apos;double-resolved& apos; events, is defined as: X(C=GAMMA)+=SUM_jets(E+Pz)/SUM_hads(E+Pz) and X(C=GAMMA)-=SUM_jets(E-Pz)/SUM_hads(E-Pz) where the summations are over the two jets and hadrons. In the tables X(C=GAMMA)+- implies that both X(C=GAMMA)s satisfy the limits.. The jet shape PSI is characterised by the fraction of the jet& apos;s transverse energy that lies inside and inner cone of radius R, concentric with the jet defining cone.. The numerical values of figure 4,5 and 7 are taken from the hztool routine hzc98113.
DOI: 10.17182/hepdata.49387.v1/t1
title: "Table 1" of "Measurement of W pair cross-sections in e+ e- interactions at S**(1/2) = 183-GeV and W decay branching fractions"

description: Cross section with LEPTON is evaluated under lepton universality assumption.
description: CERN-LEP. Measurement of the W-pair cross section in e+e- interactions at sqrt(s) = 183 GeV.
DOI: 10.17182/hepdata.49387.v1/t2
title: "Table 2" of "Measurement of W pair cross-sections in e+ e- interactions at S**(1/2) = 183-GeV and W decay branching fractions"

description: No description provided.
description: CERN-LEP. Measurement of the W-pair cross section in e+e- interactions at sqrt(s) = 183 GeV.
DOI: 10.17182/hepdata.49392.v1/t1
title: "Table 1" of "Study of the hadronic photon structure function F2(gamma) at LEP."

description: No description provided.
description: CERN-LEP. Measurement of the hadronic photon structure function, F2, in the reaction E+ E- --& gt; E+ E- HADRONS at centre-of-mass energy 91 GeV. Data correspond to integrated luminosity 140 pb-1 collected from 1991 to 1995. Two models, PHOJET(SET1) and TWOGAM(SET2) are used in the analysis.
DOI: 10.17182/hepdata.49392.v1/t2
title: "Table 2" of "Study of the hadronic photon structure function F2(gamma) at LEP."

description: No description provided.
description: CERN-LEP. Measurement of the hadronic photon structure function, F2, in the reaction E+ E- --& gt; E+ E- HADRONS at centre-of-mass energy 91 GeV. Data correspond to integrated luminosity 140 pb-1 collected from 1991 to 1995. Two models, PHOJET(SET1) and TWOGAM(SET2) are used in the analysis.
DOI: 10.17182/hepdata.49392.v1/t3
title: "Table 3" of "Study of the hadronic photon structure function F2(gamma) at LEP."

description: No description provided.
description: CERN-LEP. Measurement of the hadronic photon structure function, F2, in the reaction E+ E- --& gt; E+ E- HADRONS at centre-of-mass energy 91 GeV. Data correspond to integrated luminosity 140 pb-1 collected from 1991 to 1995. Two models, PHOJET(SET1) and TWOGAM(SET2) are used in the analysis.
DOI: 10.17182/hepdata.49410.v1/t1
title: "Table 1" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: Fragmentation function for 'uds-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t2
title: "Table 2" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: Fragmentation function for 'c-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t3
title: "Table 3" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: Fragmentation function for 'b-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t4
title: "Table 4" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: The inclusive fragmentation function.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t5
title: "Table 5" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: LN(1/X) distribution for 'uds-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t6
title: "Table 6" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: LN(1/X) distribution for 'c-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t7
title: "Table 7" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: LN(1/X) distribution for 'b-quark' events.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t8
title: "Table 8" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: The inclusive LN(1/X) distribution.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49410.v1/t9
title: "Table 9" of "Measurements of flavour dependent fragmentation functions in Z0 --&gt; q anti-q events."

description: Mean multiplicites of 'uds', 'c' and 'b' quark events and the inclusive multiplicity.
description: CERN-LEP. Measurement of the fragmentation functions for charged particles produced in E+ E- collisions at the Z0 resonance, separately for bottom(B), charm(C) and light(UDS) quark event samples, as well as for all flavours together. The results are based on data taken between 1990 and 1995 and use reconstructed D*+- mesons and secondary vertices to identify the different samples.
DOI: 10.17182/hepdata.49411.v1/t1
title: "Table 1" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t2
title: "Table 2" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t3
title: "Table 3" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t4
title: "Table 4" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t5
title: "Table 5" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t6
title: "Table 6" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.
DOI: 10.17182/hepdata.49411.v1/t7
title: "Table 7" of "Inclusive production of charged hadrons and K0(S) mesons in photon photon collisions."

description: No description provided.
description: CERN-LEP. Measurement of the differential production cross sections for charged hadrons and KOS mesons produced in the collisions of quasi-real photons from E+ E- collisions at centre-of-mass energies 161 and 172 GeV. Data are given asa function of PT and pseudorapidity.