A Search for Unconventional Tau Decays and Measurement of the Tau Production Cross Section in E+e- Annihilations at Spear

A Search for Unconventional Tau Decays and Measurement of the Tau Production Cross Section in E+e- Annihilations at Spear PDF Author:
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Category :
Languages : en
Pages : 0

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A Search for Unconventional Tau Decays and Measurement of the Tau Production Cross Section in E+e- Annihilations at SPEAR

A Search for Unconventional Tau Decays and Measurement of the Tau Production Cross Section in E+e- Annihilations at SPEAR PDF Author: Kenneth Gregory Hayes
Publisher:
ISBN:
Category : Annihilation reactions
Languages : en
Pages : 568

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Measurements of the Decays Tau−. --]. Rho−. Nu. /sub Tau/, Tau−. --]. Pi. −. Nu. /sub Tau/ and Tau−. --]. K*-(892). Nu. /sub Tau/ Using the MARK II Detector at SPEAR.

Measurements of the Decays Tau−. --]. Rho−. Nu. /sub Tau/, Tau−. --]. Pi. −. Nu. /sub Tau/ and Tau−. --]. K*-(892). Nu. /sub Tau/ Using the MARK II Detector at SPEAR. PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Measurements of the branching fractions for the Cabibbo favored decays tau− .-->. rho− .-->. .pi.−.nu./sub tau/ and the Cabibbo suppressed decay mode tau− .-->. K*− (892).nu./sub tau/ are presented. The energy dependence of the tautau− production cross section is obtained for the decays tau− .-->. rho−.nu./sub tau/ and these spectra agree well with the classification of the tau− as a spin-1/2 point particle. Fits to the production cross section yield a measurement of M/sub tau/ = (1787 +- 10) MeV/c2 for the tau mass. Ninety-five percent confidence upper limits for the forbidden decay tau− .-->. K*−(1430).nu./sub tau/ and the tau neutrino mass are presented.

Physics Briefs

Physics Briefs PDF Author:
Publisher:
ISBN:
Category : Physics
Languages : en
Pages : 788

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Decays of the Tau Lepton

Decays of the Tau Lepton PDF Author: Patricia Burchat
Publisher: Ann Arbor, Mich. : University Microfilms International
ISBN:
Category : Leptons (Nuclear physics)
Languages : en
Pages : 292

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Measurements of the Decays Tau−. --]. Rho−. Nu

Measurements of the Decays Tau−. --]. Rho−. Nu PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Measurements of the branching fractions for the Cabibbo favored decays tau− .-->. rho− .-->. .pi.−.nu./sub tau/ and the Cabibbo suppressed decay mode tau− .-->. K*− (892).nu./sub tau/ are presented. The energy dependence of the tautau− production cross section is obtained for the decays tau− .-->. rho−.nu./sub tau/ and these spectra agree well with the classification of the tau− as a spin-1/2 point particle. Fits to the production cross section yield a measurement of M/sub tau/ = (1787 +- 10) MeV/c2 for the tau mass. Ninety-five percent confidence upper limits for the forbidden decay tau− .-->. K*−(1430).nu./sub tau/ and the tau neutrino mass are presented.

Measurement of the Decays Tau−. --]. Rho−. Nu

Measurement of the Decays Tau−. --]. Rho−. Nu PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
Measurements of the branching fractions for the Cabibbo-favored decay tau− .-->. rho−.nu./sub tau/ and the Cabibbo-suppressed decay tau− .-->. K*−(892).nu./sub tau/ are presented. The energy dependence of the tautau− production cross section is measured with the aid of the decay tau− .-->. rho−.nu./sub tau/, which yields a measurement M/sub tau/ = (1790 +- 40) MeV. A 2 sigma upper limit for the forbidden decay tau− .-->. K*−(1430).nu./sub tau/ is also presented. 3 figures.

The production and decay of tau-leptons in e_1hn+e_1hn_346 [ee] annihilation at Petra energies

The production and decay of tau-leptons in e_1hn+e_1hn_346 [ee] annihilation at Petra energies PDF Author:
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Category :
Languages : de
Pages :

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Measurement of Cross-section (p Anti-p --] Z0) X BF (Z0 --] Tau Anti-tau) at S**(1/2)

Measurement of Cross-section (p Anti-p --] Z0) X BF (Z0 --] Tau Anti-tau) at S**(1/2) PDF Author: Silke Duensing
Publisher:
ISBN:
Category :
Languages : en
Pages : 129

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In this thesis the first measurement of {sigma}(p{bar p}) {yields} Z{sup 0} {yields} {tau}{bar {tau}} with the D0 detector at the Tevatron is presented. The tau pair candidates are recorded by the D0 detector using p{bar p} interactions at a center-of-mass energy of 1.96 TeV. Events in which one tau decays into a muon and the other tau final state is hadronic with one charged particle are selected for this analysis. The selection criteria for the hadronic tau decay are based on the tau final state, hence for two channels of one-prong taus: single charged pion ({tau}{sub {pi}}) and rho decays ({tau}{sub {rho}}). The selection is based on simple cuts on a number of discriminating variables and the cut values have been optimized for the best cross section measurement. Of hadronic tau candidates that have been reconstructed as {tau}{sub {pi}} candidates, 0.801 {+-} 0.017 {+-} 0.066 pass the selection cut; in the case of {tau}{sub {rho}} taus, the selection efficiency is 0.676 {+-} 0.009 {+-} 0.009. Of all QCD jets that are reconstructed as hadronic tau candidates, 0.0093 {+-} 0.0002 pass the {tau}{sub {pi}} selection cuts and 0.0122 {+-} 0.0002 the {tau}{sub {rho}} cuts. The cross section has been measured to be 274 {+-} 121 {+-} 40 {+-} 27 pb in the {mu}{tau}{sub {pi}} channel and 273 {+-} 40{sub -23}{sup +18} {+-} 27 pb in the {mu}{tau}{sub {rho}} channel, resulting in a combined measurement of {sigma}(p{bar p} {yields} Z{sup 0} {yields} {tau}{bar {tau}}) = 273 {+-} 38{sub -23}{sup +19} {+-} 27 pb which agrees with the SM prediction within errors. The errors are dominated by the statistical error as only the first data taken with the D0 detector in Run II was used. Due to the small set of tau candidates, the calorimeter energy scale could not yet be determined using data and this uncertainty is the largest systematic effect on the measurement. Another large contribution arises from the uncertainty of 10% on the luminosity measurement. This is expected to decrease significantly in the future. It was demonstrated that the currently available tools are sufficient to use tau leptons in the measurement of a SM process. This opens the door to the use of hadronic tau decays in the search for new particles, like SUSY particles, that decay preferentially to tau leptons in a number of models or the Higgs boson of either the SM or extended model. Doing physics at the Tevatron as the accelerator at the current energy frontier is our current best hope to find the yet elusive Higgs boson and will allow to either find proof of physics beyond the Standard Model or tighten the constraints on these models.

Tau Lepton Physics - Proceedings Of The Second Workshop

Tau Lepton Physics - Proceedings Of The Second Workshop PDF Author: K K Gan
Publisher: World Scientific
ISBN: 9814553433
Category :
Languages : en
Pages : 590

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The II International Workshop on Tau Lepton Physics was held in Ohio, USA in September 1992. Its purpose is to gather the experts on tau lepton physics to examine the current understanding of the tau lepton physics and to assess future prospects. A particular emphasis of the Workshop was a detailed examination of the '1-prong problem': the discrepancy between the inclusive measurement of one-charged-particle decay branching ratio and the sum of the exclusive decays. The Workshop also stimulated new ideas on tests of the Standard Model using the third generation lepton and assessed the future prospects of the lepton physics.