Nuclear Instruments and Methods in Physics Research Section A:

1990

DOI: 10.1016/0168-9002(90)90250-a

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The construction of the L3 experiment

M. Aguilar-Benı́tez²,

et al.

Abstract: L

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Data and Monte Carlo2

Introduction2

Corrections For Detector Effects1

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Cited by 521 publications

(95 citation statements)

References 31 publications

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“…The data used for this analysis were collected by the L3 detector [6] at centre-of-mass energies √ s = 189 − 209 GeV, with a luminosity weighted average value of √ s = 198 GeV, and a total integrated luminosity of 560 pb −1 . Results on inclusive jet production at LEP for a smaller data sample at lower √ s were previously reported [7].…”

Section: Data and Monte Carlomentioning

confidence: 99%

Inclusive jet production in two-photon collisions at LEP

¹

,

²

,

et al. 2004

Physics Letters B

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Inclusive jet production, e + e − → e + e − jet X, is studied using 560 pb −1 of data collected at LEP with the L3 detector at centre-of-mass energies between 189 and 209 GeV. The inclusive differential cross section is measured using a k t jet algorithm as a function of the jet transverse momentum, p t , in the range 3 < p t < 50 GeV for a pseudorapidity, η, in the range −1 < η < 1. This cross section is well represented by a power law. For high p t , the measured cross section is significantly higher than the NLO QCD predictions, as already observed for inclusive π ± and π 0 production.

“…The data used for this analysis were collected by the L3 detector [6] at centre-of-mass energies √ s = 189 − 209 GeV, with a luminosity weighted average value of √ s = 198 GeV, and a total integrated luminosity of 560 pb −1 . Results on inclusive jet production at LEP for a smaller data sample at lower √ s were previously reported [7].…”

Section: Data and Monte Carlomentioning

confidence: 99%

Inclusive jet production in two-photon collisions at LEP

¹

,

²

,

et al. 2004

Physics Letters B

Self Cite

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Inclusive jet production, e + e − → e + e − jet X, is studied using 560 pb −1 of data collected at LEP with the L3 detector at centre-of-mass energies between 189 and 209 GeV. The inclusive differential cross section is measured using a k t jet algorithm as a function of the jet transverse momentum, p t , in the range 3 < p t < 50 GeV for a pseudorapidity, η, in the range −1 < η < 1. This cross section is well represented by a power law. For high p t , the measured cross section is significantly higher than the NLO QCD predictions, as already observed for inclusive π ± and π 0 production.

“…The data were collected using the L3 detector [6] at LEP during 1998. The integrated luminosity is 176.4 pb −1 at an average center-of-mass energy of 188.6 GeV.…”

Section: Data and Monte Carlo Samplesmentioning

confidence: 99%

Search for the standard model Higgs boson in e+e− interactions at GeV

et al. 1999

Physics Letters B

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A search for the Standard Model Higgs boson is carried out on 176.4 pb −1 of data collected by the L3 detector at a center-of-mass energy of 189 GeV. The data are consistent with the expectations of Standard Model processes and no evidence of a Higgs signal is observed. Combining the results of this search with those at lower center-of-mass energies, a lower limit on the mass of the Standard Model Higgs boson of 95.3 GeV is set at the 95% confidence level.

“…We report here measurements of event shape distributions and their moments using the data collected with the L3 detector [3]. We update the published results at √ s = 161, 172 and 183 GeV [4,5] with an improved selection method for hadronic events and present new results at √ s = 130, 136 and 189 GeV.…”

Section: Introductionmentioning

confidence: 74%

QCD studies in e+e− annihilation from 30 GeV to 189 GeV

et al. 2000

Physics Letters B

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We present results obtained from a study of the structure of hadronic events recorded by the L3 detector at various centre-of-mass energies. The distributions of event shape variables and the energy dependence of their mean values are measured from 30 GeV to 189 GeV and compared with various QCD models. The energy dependence of the moments of event shape variables is used to test a power law ansatz for the non-perturbative component. We obtain a universal value of the nonperturbative parameter α 0 = 0.537 ± 0.073. From a comparison with resummed O(α 2 s ) QCD calculations, we determine the strong coupling constant at each of the selected energies. The measurements demonstrate the running of α s as expected in QCD with a value of α s (m Z ) = 0.1215 ± 0.0012 (exp) ± 0.0061 (th).

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