Showing 3 of 93 results
Multihadronic e+e− annihilation events at a center-of-mass energy of 29 GeV have been studied with both the original (PEP 5) Mark II and the upgraded Mark II detectors. Detector-corrected distributions from global shape analyses such as aplanarity, Q2-Q1, sphericity, thrust, minor value, oblateness, and jet masses, and inclusive charged-particle distributions including x, rapidity, p⊥, and particle flow are presented. These distributions are compared with predictions from various multihadron event models which use leading-logarithmic shower evolution or QCD matrix elements at the parton level and string or cluster fragmentation for hadronization. The new generation of parton-shower models gives, on the average, a better description of the data than the previous parton-shower models. The energy behavior of these models is compared to existing e+e− data. The predictions of the models at a center-of-mass energy of 93 GeV, roughly the expected mass of the Z0, are also presented.
Aplanarity distribution.
QX Distribution(QX=SQRT(3)*(Q3-Q2)).
The (Q2-Q1) distribution.
Sphericity distribution.
Thrust distribution.
The minor value distribution.
Oblateness distribution.
The invariant mass square of the broad jet.
The invariant mass square of the slim jet.
The mass square difference of the broad and slim jet.
The transverse momentum distribution with respect to the sphericity axis.
The transverse momentum distribution with respect to the sphericity axis.
The momentum distribution out of the event plane.
The transverse momentum distribution in the event plane with respect to the sphericity axis.
The scaled momentum distribution.
Rapidity distribution (folded around yrap=0).
The charged particle flow with respect to the sphericity axis.
The energy flow with respect to the sphericity axis.
Aplanarity distribution.
QX Distribution (QX=SQRT(3)*(Q3-Q2).
The (Q2-Q1) distributions.
Sphericity distribution.
Thrust distribution.
The minor value distribution.
Oblateness distribution.
The invariant mass square of the broad jet.
No description provided.
The mass square difference of the broad and slim jet.
The transverse momentum disribution with respect to the sphericity axis.
The transverse momentum distribution with respect to the sphericity axis.
The momentum distribution out of the event plane.
The transverse momentum distribution in the event plane with respect to the sphericity axis.
The scaled momentum distribution.
Rapidity distribution (folded around yrap=0).
The charged particle flow with respect to the sphericity axis.
No description provided.
Aplanarity distribution.
QX distribution (QX=SQRT(3)*(Q3-Q2).
The (Q2-Q1) distribution.
Sphericity distribution.
Thrust distribution.
The minor value distribution.
Oblateness distribution.
The invariant mass square of the broad jet.
The invariant mass square of the slim jet.
The mass square difference of the broad and slim jet.
The transverse momentum distribution with respect to the sphericity axis.
The transverse momentum distribution with respect to the sphericity axis.
The momentum distribution out of the event plane.
The transverse momentum distribution in the event plane with respect to the sphericity axis.
No description provided.
Rapidity distribution (folded around yrap=0).
The charged particle flow with respect to the sphericity axis.
The energy flow with respect to the sphericity axis.
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
Axis error includes +- 0.0/0.0 contribution (?////SYSTEMATIC ERRORS IN CORRECTIONSVARIOUS CORRECTIONS USING MONTE-CARLO SIMULATION).
We present results from a high momentum resolution measurement of the π − p elastic differential cross section near the η production threshold. By analysing the cusp discontinuity in the elastic cross section we deduce the non-spin-flip elastic amplitude and compare it with solutions from phase-shift analyses.
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Differential cross sections have been measured for the interactions p p → π − π + and p p → K − K + over a centre of mass angular range −0.95 ⩽ cos θ ∗ ⩽ 0.95 at 20 incident momenta between 0.79 and 2.43 GeV/ c . A magnetic spectrometer with wire spark chambers was used. Typically 2000 π − π + and 300 K − K + events were obtained at each momentum. Results are compared with those from related experiments.
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