2013
DOI: 10.1103/physrevd.88.032011
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Production of charged pions, kaons, and protons ine+eannihilations into hadrons ats=10.54

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Cited by 67 publications
(35 citation statements)
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“…In order to tune the shower and light quark hadronization parameters we used data on jet rates and event shapes for centre-of-mass energies between 14 and 44 GeV [40][41][42][43], at LEP1 and SLD [42][43][44][45][46][47] and LEP2 [42,43,46,47], particle multiplicities [44,45] and spectra [44,45,[48][49][50][51][52][53][54][55][56][57][58][59][60] at LEP 1, identified particle spectra below the Υ(4S) from Babar [61], the charged particle multiplicity and distributions from [62][63][64][65][66][67] for centre-of-mass energies between 14 and 61 GeV, the charged particle multiplicity [68,69] and particle spectra [68,70,71] in light quark events at LEP1 and SLD, the charged particle multiplicity in light quark events at LEP2 [72,73], the cha...…”
Section: Tuningmentioning
confidence: 99%
“…In order to tune the shower and light quark hadronization parameters we used data on jet rates and event shapes for centre-of-mass energies between 14 and 44 GeV [40][41][42][43], at LEP1 and SLD [42][43][44][45][46][47] and LEP2 [42,43,46,47], particle multiplicities [44,45] and spectra [44,45,[48][49][50][51][52][53][54][55][56][57][58][59][60] at LEP 1, identified particle spectra below the Υ(4S) from Babar [61], the charged particle multiplicity and distributions from [62][63][64][65][66][67] for centre-of-mass energies between 14 and 61 GeV, the charged particle multiplicity [68,69] and particle spectra [68,70,71] in light quark events at LEP1 and SLD, the charged particle multiplicity in light quark events at LEP2 [72,73], the cha...…”
Section: Tuningmentioning
confidence: 99%
“…Fragmentation processes have been studied in leptonhadron and hadron-hadron scattering, as well as in e þ e − annihilation, which provides the cleanest environment since no hadrons are present in the initial state. Due to the large amount of experimental data collected at several e þ e − facilities, mainly LEP [1][2][3] and SLC [4][5][6] at high energies, and, recently, PEP-II [7] and KEKB [8] at the center-of-mass energy ffiffi ffi s p ∼ 10 GeV, the unpolarized functions are presently well known.…”
Section: Introductionmentioning
confidence: 99%
“…These include data for hadron production in: single-inclusive annihilation (SIA) (recently measured by BELLE [3, 4] and BABAR [5]), semi-inclusive deep-inelastic scattering (SIDIS) (recently measured by HERMES [6] and COMPASS [7, 8]) and proton-(anti)proton ( pp ) collisions (measured, e.g., by CDF [9, 10] at the Tevatron, STAR [11] and PHENIX [12] at RHIC and CMS [13, 14] and ALICE [15] at the LHC). These measurements span a wide range in energy and momentum fraction and are sensitive to different partonic combinations.…”
Section: Introductionmentioning
confidence: 99%