Measurement Of Anomalous Dimuons Produced In Electron Positron Annihilations PDF Download

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Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L/sub H/. --]. Charged Hadron + 2. Nu., . Nu. + N. Gamma., Tau. --]. Nu. /sub Tau/e−. Nu. /sub E−/, . Nu. /sub Tau/. Mu Nu. /sub. Mu. /, Rare Modes, Cross Sections].

Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L/sub H/. --]. Charged Hadron + 2. Nu., . Nu. + N. Gamma., Tau. --]. Nu. /sub Tau/e−. Nu. /sub E−/, . Nu. /sub Tau/. Mu Nu. /sub. Mu. /, Rare Modes, Cross Sections].
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Download Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L/sub H/. --]. Charged Hadron + 2. Nu., . Nu. + N. Gamma., Tau. --]. Nu. /sub Tau/e−. Nu. /sub E−/, . Nu. /sub Tau/. Mu Nu. /sub. Mu. /, Rare Modes, Cross Sections]. Book in PDF, ePub and Kindle

Results of studies of anomalous electron-muon and electron-hadron events produced in electron-positron annihilation are presented. The data for this work were obtained with a lead-glass counter system, which was added to one octant of the Stanford Linear Accelerator Center-Lawrence Berkeley Laboratory magnetic detector at the electron-positron storage ring SPEAR. The lead-glass counter system provides good electron identification for part of the magnetic detector. The events under study have two detected charged particles and any number of detected photons. One detected charged particle is identified as an electron in the lead-glass counter system. The other detected charged particle is identified as a muon or hadron in the magnetic detector. Anomalous events are events which are not subject to conventional explanations; examples of conventional explanations are misidentification of particles or the decay of ordinary or strange hadrons. These data confirm previous observations of anomalous lepton production at SPEAR and DESY. The data corrected for charm background are consistent with heavy lepton production and decay. The branching ratio for the heavy lepton to decay into an electron and two neutrinos was measured to be 0.21 +- 0.05. The branching ratio for the heavy lepton to decay into one charged hadron, one neutrino and any number of photons was measured to be 0.28 +- 0.13. They are consistent with the theoretical values within the errors.


Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L

Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L
Author:
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Release: 1978
Genre:
ISBN:

Download Anomalous Electron--muon and Electron--hadron Production in Electron--positron Annihilation. [Branching Ratio L Book in PDF, ePub and Kindle

Results of studies of anomalous electron-muon and electron-hadron events produced in electron-positron annihilation are presented. The data for this work were obtained with a lead-glass counter system, which was added to one octant of the Stanford Linear Accelerator Center-Lawrence Berkeley Laboratory magnetic detector at the electron-positron storage ring SPEAR. The lead-glass counter system provides good electron identification for part of the magnetic detector. The events under study have two detected charged particles and any number of detected photons. One detected charged particle is identified as an electron in the lead-glass counter system. The other detected charged particle is identified as a muon or hadron in the magnetic detector. Anomalous events are events which are not subject to conventional explanations; examples of conventional explanations are misidentification of particles or the decay of ordinary or strange hadrons. These data confirm previous observations of anomalous lepton production at SPEAR and DESY. The data corrected for charm background are consistent with heavy lepton production and decay. The branching ratio for the heavy lepton to decay into an electron and two neutrinos was measured to be 0.21 +- 0.05. The branching ratio for the heavy lepton to decay into one charged hadron, one neutrino and any number of photons was measured to be 0.28 +- 0.13. They are consistent with the theoretical values within the errors.


Status of the Fermilab Muon (g-2) Experiment

Status of the Fermilab Muon (g-2) Experiment
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The New Muon (g-2) Collaboration at Fermilab has proposed to measure the anomalous magnetic moment of the muon, a{sub {mu}}, a factor of four better than was done in E821 at the Brookhaven AGS, which obtained a{sub {mu}} = [116592089(63)] x 10−11 ± 0.54 ppm. The last digit of a{sub {mu}} is changed from the published value owing to a new value of the ratio of the muon-to-proton magnetic moment that has become available. At present there appears to be a difference between the Standard-Model value and the measured value, at the ≈= 3 standard deviation level when electron-positron annihilation data are used to determine the lowest-order hadronic piece of the Standard Model contribution. The improved experiment, along with further advances in the determination of the hadronic contribution, should clarify this difference. Because of its ability to constrain the interpretation of discoveries made at the LHC, the improved measurement will be of significant value, whatever discoveries may come from the LHC.