0000000000134985

AUTHOR

L. M. Mundim

showing 8 related works from this author

Updated precision measurement of the average lifetime of B hadrons

1996

The measurement of the average lifetime of B hadrons using inclusively reconstructed secondary vertices has been updated using both an improved processing of previous data and additional statistics from new data. This has reduced the statistical and systematic uncertainties and gives \tau_{\mathrm{B}} = 1.582 \pm 0.011\ \mathrm{(stat.)} \pm 0.027\ \mathrm{(syst.)}\ \mathrm{ps.} Combining this result with the previous result based on charged particle impact parameter distributions yields \tau_{\mathrm{B}} = 1.575 \pm 0.010\ \mathrm{(stat.)} \pm 0.026\ \mathrm{(syst.)}\ \mathrm{ps.}

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadron01 natural sciencesb taggingPartícules (Física nuclear)030218 nuclear medicine & medical imagingNuclear physics03 medical and health sciencesinclusive reconstruction0302 clinical medicine0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentDELPHIPhysics010308 nuclear & particles physicsLARGE ELECTRON POSITRON COLLIDERCharged particleB hadrons lifetimeDELPHI; B hadrons lifetime; inclusive reconstruction; b taggingPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearAstrophysics::Earth and Planetary AstrophysicsImpact parameterParticle Physics - Experiment
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A measurement of the Tau topological branching ratios

2001

Using data collected in the DELPHI detector at LEP-1, measurements of the inclusive tau branching ratios for decay modes containing one, three, or five charged particles have been performed, giving the following results: B_1 = B(\tau^- -> (particle)^- \geq 0pi^0 \geq 0K^0 \nu_\tau(\bar{\nu})) = (85.316 +/- 0.093 +/- 0.049)%; B_3 = B(\tau^- -> 2h^-h^+ \geq 0pi^0 \geq 0K^0 \nu_\tau) = (14.569 +/- 0.093 +/- 0.048)%; B_5 = B(\tau^- -> 3h^-2h^+ \geq 0pi^0 \geq 0K^0 \nu_\tau) = (0.115 +/- 0.013 +/- 0.006)%, where h is either a charged pi or K meson. The first quoted uncertainties are statistical and the second systematic.

Particle physicsPhysics and Astronomy (miscellaneous)MesonPAIR PRODUCTIONENERGIESFOS: Physical sciencesBranching (polymer chemistry)01 natural sciencesCROSS-SECTIONSHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)BHABHA SCATTERINGMONTE-CARLOMONTE-CARLO; RADIATIVE-CORRECTIONS; BHABHA SCATTERING; PARTICLE PHYSICS; DELPHI DETECTOR; PAIR PRODUCTION; CROSS-SECTIONS; CP-INVARIANCE; ENERGIES; DECAY0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONS010306 general physicsEngineering (miscellaneous)DELPHIPhysicshigh energy collider010308 nuclear & particles physicsLEPDELPHI DETECTORCharged particleFIS/01 - FISICA SPERIMENTALEPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearCP-INVARIANCEDECAYParticle Physics - Experiment
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Search for exclusive decays of the Lambda_b baryon and measurement of its mass

1996

A search for fully reconstructed \lb beauty baryons is performed using about 3 million Z decays collected with the DELPHI detector at LEP. The analysis relies on the combined use of the accurate tracking and of the hadron identification capabilities of DELPHI. A total of four events has been found, three in the \lc\ppm channel and one in the \lc\a1m channel over a small background. The \lb beauty baryon mass is measured to be (~ 5668 \pm 16~ ({\rm stat.}) \pm 8~({\rm syst.})~)~ \mv.

Nuclear and High Energy PhysicsParticle physicsHadronCombined useLambdaTracking (particle physics)01 natural sciencesPartícules (Física nuclear)Nuclear physicsbeauty baryon0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentDetectors de radiacióDELPHIPhysics010308 nuclear & particles physicsDetectorLARGE ELECTRON POSITRON COLLIDERBaryonDELPHI; beauty baryon; particle identificationPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::Experimentparticle identificationParticle Physics - Experiment
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A Precise Measurement of the Tau Lepton Lifetime

1996

The tau lepton lifetime has been measured using three different methods with the DELPHI detector. Two measurements of one-prong decays are combined, accounting for correlations, giving a result of \tau_\tau = 291.8 \pm 3.3 \mbox{ (stat.)} \pm 2.0 \mbox{(sys.) fs} while the decay length distribution of three-prong decays gives the result \tau_{\tau} = 286.7 \pm 4.9 \mbox{ (stat.)} \pm 3.3 \mbox{ (sys.) fs}. Combining the results presented here with previous DELPHI measurements, we get \tau_{\tau} = 291.4 \pm 3.0 fs and find that the ratio of the coupling constant for tau decay relative to that for muon decay is 0.990 \pm 0.009, compatible with lepton universality.

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilation01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)tau lepton lifetimeNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsZ-DECAYSDELPHICoupling constantPhysicsMuon010308 nuclear & particles physicsDELPHI; tau lepton lifetime; one-prong; three-prongLARGE ELECTRON POSITRON COLLIDERthree-prongYield (chemistry)PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIone-prongDecay lengthPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearVertex detectorParticle Physics - ExperimentLepton
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A measurement of αs from the scaling violation in e+e- annihilation

1997

The hadronic fragmentation functions of the various quark flavours and of gluons are measured in a study of the inclusive hadron production from $\zz$ decays with the DELPHI detector and are compared with the fragmentation functions measured elsewhere at energies between 14 GeV and 91 GeV. A large scaling violation is observed, which is used to extract the strong coupling constant from a fit using a numerical integration of the second order DGLAP evolution equations. The result is \begin{displaymath} \alpha_s(M_Z) = 0.124^{+0.006}_{-0.007}(exp)\pm 0.009 (theory) \end{displaymath} where the first error represents the experimental uncertainty and the second error is due to the factorization a…

QuarkNuclear and High Energy PhysicsParticle physicsE+E ANNIHILATIONElectron–positron annihilationFRAGMENTATION FUNCTIONSHadronHADRONIC-Z-DECAYS; JET PRODUCTION-RATES; E+E ANNIHILATION; FRAGMENTATION FUNCTIONS; ENERGY CORRELATIONS; PERTURBATIVE QCD; RESONANCE; EVOLUTION; PARTICLE; TESTS01 natural sciencesPartícules (Física nuclear)Nuclear physicsRenormalizationViolació CP (Física nuclear)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PERTURBATIVE QCD010306 general physicsNuclear ExperimentScalingDetectors de radiacióDELPHIPhysicsAnnihilation010308 nuclear & particles physicsJET PRODUCTION-RATESHigh Energy Physics::PhenomenologyPerturbative QCDRESONANCELARGE ELECTRON POSITRON COLLIDEREVOLUTIONDGLAPENERGY CORRELATIONSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHITESTSPARTICLE PHYSICSHigh Energy Physics::ExperimentPARTICLEParticle Physics - ExperimentHADRONIC-Z-DECAYS
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Measurement of the spin density matrix for the rho(0), K*(0)(892) and phi produced in Z(0) decays

1997

The spin density matrix elements for the rho(0), K-*0(892) and phi produced in hadronic Z(0) decays are measured in the DELPHI detector. There is no evidence for spin alignment of the K-*0(892) and phi, in the region x(p) less than or equal to 0.3 (x(p) = p/p(beam)), where rho(00) = 0.33 +/- 0.05 and rho(00) = 0.30 +/- 0.04, respectively. In the fragmentation region, x(p) greater than or equal to 0.4, there is some indication for spin alignment of the rho(0) and K-*0(892), since rho(00) = 0.43 +/- 0.05 and rho(00) = 0.46 +/- 0.08, respectively. These values are compared with those found in meson-induced hadronic reactions. For the phi, rho(00) = 0.30 +/- 0.04 for x(p) greater than or equal …

Nuclear and High Energy PhysicsMesonElectron–positron annihilationD-STARHadronANNIHILATIONSPartícules (Física nuclear)QUARK FRAGMENTATION; D-STAR; ANNIHILATIONS; HADRONS; MESONSNuclear physicsAngular distribution[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Matrix elementSpin densityDetectors de radiacióDELPHIPhysicsHADRONSD-STARQUARK FRAGMENTATIONLARGE ELECTRON POSITRON COLLIDERMESONSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIMass spectrumPARTICLE PHYSICSAtomic physicsParticle Physics - ExperimentPHYSICS LETTERS B
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Search for pair production of heavy objects in 4-jet events at sqrt {s}$=130-136 GeV

1996

Results are presented of a search for pair production of heavy objects decaying into four hadronic jets, as expected for example from associated or pair production of MSSM Higgs bosons, hA or H$^+$H$^-$, using a data sample of $5.9\,$pb$^{-1}$ of $e^+ e^-$ collisions at $\sqrt{s}=130$-$136\,{\mathrm {GeV}}$ collected with the DELPHI detector at LEP in November 1995. The data and expectations from standard processes agree after four-jet selections. An analysis based on $b$-tagging finds no hA candidate with high mass. A study optimized to search for H$^+$H$^-$ events with mass in the 40-50$\,{\mathrm{GeV}}/c^2$ range also finds no candidate. Finally a comparison is made with a recent ALEPH a…

Particle physicsAlephPhysics and Astronomy (miscellaneous)ENERGIESElectron–positron annihilationHadronHIGGS BOSONSJet (particle physics)Partícules (Física nuclear)DECAYSNuclear physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors de radiacióBosonDELPHIPhysicsHigh Energy Physics::PhenomenologySupersymmetryLARGE ELECTRON POSITRON COLLIDERHIGGS BOSONS; ENERGIES; DECAYSPair productionPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIHiggs bosonPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle Physics - Experiment
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Measurement of the transverse spin correlation in Z → τ+ τ- decays

1997

The measurement of the correlation between the transverse spin components of tau(+)tau(-) pairs collected during 1992 to 1994 with the DELPHI detector at LEP1 is presented. A value C-TT = 0.87 +/- 0.20 (stat.)(-0.12)(+0.10) (syst.) was obtained for the correlation parameter, in agreement with the Standard Model expectation. (C) 1997 Published by Elsevier Science B.V.

QuarkNuclear and High Energy PhysicsParticle physicsLUND MONTE-CARLOElectron–positron annihilationLEP-SLC ENERGIES01 natural sciencesPartícules (Física nuclear)JET FRAGMENTATIONStandard ModelNuclear physicsPHYSICS0103 physical sciencesRADIATIVE-CORRECTIONS010306 general physicsNuclear ExperimentDetectors de radiacióLUND MONTE-CARLO; LEP-SLC ENERGIES; RADIATIVE-CORRECTIONS; JET FRAGMENTATION; TAU-POLARIZATION; SIMULATION; PHYSICS; QUARKSpin-½DELPHIPhysics010308 nuclear & particles physicsTAU-POLARIZATIONQUARKCenter (category theory)LARGE ELECTRON POSITRON COLLIDERTransverse planePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHISIMULATIONPARTICLE PHYSICSHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary Astrophysics
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