Abstract:The purpose of this study was to identify through the Delphi Technique, important requirements of an information system development methodology. These requirements should satisfy the needs of actual organizations, regarding the strategic use of information technology. An initial listing of requirements was developed through a review of the related literature. The Delphi panel consisted of 31 brazilian specialists in information systems. Two rounds were employed to collect from this panel the most important req… Show more
“…(12). This figure is taken from [44] with the addition of the result from the VENUS experiment at √ s = 58 GeV [36] as well as the preliminary result from DELPHI at √ s = 206 GeV [49] . The dash-dotted line shown in Fig.…”
Section: Discussion and Estimate Of Next-to-mlla Terms Of The Order Omentioning
confidence: 99%
“…The total uncertainty (statistics and systematics combined) on δ bℓ quoted in their analysis is about a factor two larger than those quoted by SLD [42,45] and OPAL [41], and if we assume a similar relative precision also for δ cℓ , by comparison with the SLD and OPAL total uncertainties we get for DELPHI δ cℓ = 1.64 ± 1.2. Our weighted average in Table 1 would change to δ cℓ = 6 There are published results on the measurements of N ch c and N ch ℓ also at LEP2 energies [43,44,49]. Unfortunately, the limited statistics available at each energy did not allow the efficient c-quark tagging, comparable to that at the Z 0 peak.…”
Section: Appendix B B1 On the Measurement Of δ Cℓmentioning
The perturbative QCD approach to multiparticle production predicts a characteristic suppression of particle multiplicity in a heavy quark jet as compared to a light quark jet. In the Modified Leading Logarithmic Approximation (MLLA) the multiplicity difference δ Qℓ between heavy and light quark jets is derived in terms of a few other experimentally measured quantities. The earlier prediction for b-quarks needs revision in the light of new experimental results and the improvement in the understanding of the experimental data. We now find δ bℓ = 4.4 ± 0.4. The updated MLLA results on δ bℓ and δ cℓ are compared with the present data from e + e − annihilation. Their expected energy independence is confirmed within the energy range between 29 and 200 GeV; the absolute values are now in better agreement with experiment than in the previous analysis, and the remaining difference can be attributed largely to next-to-MLLA contributions, an important subset of which are identified and evaluated.
“…(12). This figure is taken from [44] with the addition of the result from the VENUS experiment at √ s = 58 GeV [36] as well as the preliminary result from DELPHI at √ s = 206 GeV [49] . The dash-dotted line shown in Fig.…”
Section: Discussion and Estimate Of Next-to-mlla Terms Of The Order Omentioning
confidence: 99%
“…The total uncertainty (statistics and systematics combined) on δ bℓ quoted in their analysis is about a factor two larger than those quoted by SLD [42,45] and OPAL [41], and if we assume a similar relative precision also for δ cℓ , by comparison with the SLD and OPAL total uncertainties we get for DELPHI δ cℓ = 1.64 ± 1.2. Our weighted average in Table 1 would change to δ cℓ = 6 There are published results on the measurements of N ch c and N ch ℓ also at LEP2 energies [43,44,49]. Unfortunately, the limited statistics available at each energy did not allow the efficient c-quark tagging, comparable to that at the Z 0 peak.…”
Section: Appendix B B1 On the Measurement Of δ Cℓmentioning
The perturbative QCD approach to multiparticle production predicts a characteristic suppression of particle multiplicity in a heavy quark jet as compared to a light quark jet. In the Modified Leading Logarithmic Approximation (MLLA) the multiplicity difference δ Qℓ between heavy and light quark jets is derived in terms of a few other experimentally measured quantities. The earlier prediction for b-quarks needs revision in the light of new experimental results and the improvement in the understanding of the experimental data. We now find δ bℓ = 4.4 ± 0.4. The updated MLLA results on δ bℓ and δ cℓ are compared with the present data from e + e − annihilation. Their expected energy independence is confirmed within the energy range between 29 and 200 GeV; the absolute values are now in better agreement with experiment than in the previous analysis, and the remaining difference can be attributed largely to next-to-MLLA contributions, an important subset of which are identified and evaluated.
“…In this Section, I consider the recent results on hadron multiplicities from fragmentation of heavy and light quarks [6][7][8]. The study of the quark content in multiparticle production provides one of the basic tests of QCD.…”
Section: Hadronisation Of Heavy and Light Quarksmentioning
confidence: 99%
“…In Refs. [6] and [8], a study of the fragmentation of heavy b-quark and light quarks (l = u, d, s) is performed. The measurements of the difference in charge particle multiplicities, δ bl = n bb − n ll , for bb and ll events in e + e − annihilation at the centre-of-mass energies above the Z 0 peak are carried out.…”
Section: Hadronisation Of Heavy and Light Quarksmentioning
The recent results on hadron multiplicities in heavy and light quark fragmentation, multiplicity local fluctuations and multiparticle correlations submitted to the Conference are reviewed.
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