CERN Accelerating science

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000374322 003__ SzGeCERN
000374322 005__ 20211029041045.0
000374322 0248_ $$aoai:cds.cern.ch:374322$$pcerncds:hep-ex$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
000374322 0247_ $$2DOI$$a10.1016/S0370-2693(98)01553-6
000374322 035__ $$9CERN annual report$$a98-1016
000374322 035__ $$9INSPEC$$a6200232
000374322 035__ $$9SLAC$$a3911748
000374322 035__ $$9SPIRES$$a3911748
000374322 035__ $$9Inspire$$a480847
000374322 037__ $$9arXiv$$ahep-ex/9812017$$chep-ex
000374322 037__ $$aCERN-EP-98-175
000374322 041__ $$aeng
000374322 084__ $$2CERN Library$$aEP-1998-175
000374322 088__ $$99812017
000374322 088__ $$aCERN-EP-98-175
000374322 100__ $$aAbbiendi, G.
000374322 245__ $$aA measurement of the $\tau^{-} \to e^{-} \overline{\nu}_{e}\nu_{\tau}$ branching ratio
000374322 260__ $$c1999
000374322 269__ $$aGeneva$$bCERN$$c6 Nov 1998
000374322 300__ $$a17 p
000374322 340__ $$apaper
000374322 500__ $$9arXiv$$a16 pages, LaTeX, 5 eps figs included, submitted to Physics Letters B Report-no: CERN-EP/98-175
000374322 520__ $$aThe branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).
000374322 520__ $$aThe branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).
000374322 520__ $$aThe branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).
000374322 520__ $$aThe branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).
000374322 520__ $$aThe branching ratio for the decay tau->e nue nutau has been measured using Z0 decay data collected by the OPAL experiment at LEP. In total 33073 tau->e nue nutau candidates were identified from a sample of 186197 selected tau decays, giving a branching ratio of 17.81 +- 0.09(stat) +_ 0.06(sys)%. This result is combined with other measurements to test e-mu and mu-tau universality in charged-current weak interactions. Additionally, the strong coupling constant alpha_s has been extracted and evolved to the Z0 mass scale, giving alpha_s = 0.1204 +- 0.0011(exp) +- 0.0019(theory).
000374322 520__ $$9Elsevier$$aThe branching ratio for the decay τ − → e − ν ̄ e ν τ has been measured using Z 0 decay data collected by the OPAL experiment at LEP. In total 33 073 τ − → e − ν ̄ e ν τ candidates were identified from a sample of 186 197 selected τ decays, giving a branching ratio of B (τ − → e − ν ̄ e ν τ )=(17.81±0.09 (stat) ±0.06 (syst) )% . This result is combined with other measurements to test e - μ and μ - τ universality in charged-current weak interactions. Additionally, the strong coupling constant α s ( m τ 2 ) has been extracted from B (τ − → e − ν ̄ e ν τ ) and evolved to the Z 0 mass scale, giving α s ( m Z 2 )=0.1204±0.0011 (exp)±0.0019 (theory).
000374322 542__ $$fCopyright @ unknown. Published by Elsevier B.V.
000374322 595__ $$aCERN-EP
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000374322 65017 $$2SzGeCERN$$aParticle Physics - Experiment
000374322 6531_ $$9CERN$$ae- nubar(e) nu(tau)
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000374322 700__ $$aAckerstaff, K.
000374322 700__ $$aAlexander, G.
000374322 700__ $$aAllison, John
000374322 700__ $$aAltekamp, N.
000374322 700__ $$aAnderson, K.J.
000374322 700__ $$aAnderson, S.
000374322 700__ $$aArcelli, S.
000374322 700__ $$aAsai, S.
000374322 700__ $$aAshby, S.F.
000374322 700__ $$aAxen, D.
000374322 700__ $$aAzuelos, G.
000374322 700__ $$aBall, A.H.
000374322 700__ $$aBarberio, E.
000374322 700__ $$aBarlow, Roger J.
000374322 700__ $$aBartoldus, R.
000374322 700__ $$aBatley, J.R.
000374322 700__ $$aBaumann, S.
000374322 700__ $$aBechtluft, J.
000374322 700__ $$aBehnke, T.
000374322 700__ $$aBell, Kenneth Watson
000374322 700__ $$aBella, G.
000374322 700__ $$aBellerive, A.
000374322 700__ $$aBentvelsen, S.
000374322 700__ $$aBethke, S.
000374322 700__ $$aBetts, S.
000374322 700__ $$aBiebel, O.
000374322 700__ $$aBiguzzi, A.
000374322 700__ $$aBird, S.D.
000374322 700__ $$aBlobel, V.
000374322 700__ $$aBloodworth, I.J.
000374322 700__ $$aBock, P.
000374322 700__ $$aBohme, J.
000374322 700__ $$aBonacorsi, D.
000374322 700__ $$aBoutemeur, M.
000374322 700__ $$aBraibant, S.
000374322 700__ $$aBright-Thomas, P.
000374322 700__ $$aBrigliadori, L.
000374322 700__ $$aBrown, Robert M.
000374322 700__ $$aBurckhart, H.J.
000374322 700__ $$aCapiluppi, P.
000374322 700__ $$aCarnegie, R.K.
000374322 700__ $$aCarter, A.A.
000374322 700__ $$aCarter, J.R.
000374322 700__ $$aChang, C.Y.
000374322 700__ $$aCharlton, David G.
000374322 700__ $$aChrisman, D.
000374322 700__ $$aCiocca, C.
000374322 700__ $$aClarke, P.E.L.
000374322 700__ $$aClay, E.
000374322 700__ $$aCohen, I.
000374322 700__ $$aConboy, J.E.
000374322 700__ $$aCooke, O.C.
000374322 700__ $$aCouyoumtzelis, C.
000374322 700__ $$aCoxe, R.L.
000374322 700__ $$aCuffiani, M.
000374322 700__ $$aDado, S.
000374322 700__ $$aDallavalle, G.Marco
000374322 700__ $$aDavis, R.
000374322 700__ $$aDe Jong, S.
000374322 700__ $$ade Roeck, A.
000374322 700__ $$aDervan, P.
000374322 700__ $$aDesch, K.
000374322 700__ $$aDienes, B.
000374322 700__ $$aDixit, M.S.
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000374322 700__ $$aDuerdoth, I.P.
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000374322 700__ $$aEtzion, E.
000374322 700__ $$aFabbri, F.
000374322 700__ $$aFanti, M.
000374322 700__ $$aFaust, A.A.
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000374322 700__ $$aFierro, M.
000374322 700__ $$aFleck, I.
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000374322 700__ $$aFurtjes, A.
000374322 700__ $$aFutyan, D.I.
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000374322 700__ $$aGascon-Shotkin, S.M.
000374322 700__ $$aGaycken, G.
000374322 700__ $$aGeich-Gimbel, C.
000374322 700__ $$aGiacomelli, G.
000374322 700__ $$aGiacomelli, P.
000374322 700__ $$aGibson, V.
000374322 700__ $$aGibson, W.R.
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000374322 700__ $$aGlenzinski, D.
000374322 700__ $$aGoldberg, J.
000374322 700__ $$aGorn, W.
000374322 700__ $$aGrandi, C.
000374322 700__ $$aGraham, K.
000374322 700__ $$aGross, E.
000374322 700__ $$aGrunhaus, J.
000374322 700__ $$aGruwe, M.
000374322 700__ $$aHanson, G.G.
000374322 700__ $$aHansroul, M.
000374322 700__ $$aHapke, M.
000374322 700__ $$aHarder, K.
000374322 700__ $$aHarel, A.
000374322 700__ $$aHargrove, C.K.
000374322 700__ $$aHartmann, C.
000374322 700__ $$aHauschild, M.
000374322 700__ $$aHawkes, C.M.
000374322 700__ $$aHawkings, R.
000374322 700__ $$aHemingway, R.J.
000374322 700__ $$aHerndon, M.
000374322 700__ $$aHerten, G.
000374322 700__ $$aHeuer, R.D.
000374322 700__ $$aHildreth, M.D.
000374322 700__ $$aHill, J.C.
000374322 700__ $$aHobson, P.R.
000374322 700__ $$aHoch, M.
000374322 700__ $$aHocker, James Andrew
000374322 700__ $$aHoffman, Kara Dion
000374322 700__ $$aHomer, R.J.
000374322 700__ $$aHonma, A.K.
000374322 700__ $$aHorvath, D.
000374322 700__ $$aHossain, K.R.
000374322 700__ $$aHoward, R.
000374322 700__ $$aHuntemeyer, P.
000374322 700__ $$aIgo-Kemenes, P.
000374322 700__ $$aImrie, D.C.
000374322 700__ $$aIshii, K.
000374322 700__ $$aJacob, F.R.
000374322 700__ $$aJawahery, A.
000374322 700__ $$aJeremie, H.
000374322 700__ $$aJimack, M.
000374322 700__ $$aJones, C.R.
000374322 700__ $$aJovanovic, P.
000374322 700__ $$aJunk, T.R.
000374322 700__ $$aKarlen, D.
000374322 700__ $$aKartvelishvili, V.
000374322 700__ $$aKawagoe, K.
000374322 700__ $$aKawamoto, T.
000374322 700__ $$aKayal, P.I.
000374322 700__ $$aKeeler, R.K.
000374322 700__ $$aKellogg, R.G.
000374322 700__ $$aKennedy, B.W.
000374322 700__ $$aKim, D.H.
000374322 700__ $$aKlier, A.
000374322 700__ $$aKluth, S.
000374322 700__ $$aKobayashi, T.
000374322 700__ $$aKobel, M.
000374322 700__ $$aKoetke, D.S.
000374322 700__ $$aKokott, T.P.
000374322 700__ $$aKolrep, M.
000374322 700__ $$aKomamiya, S.
000374322 700__ $$aKowalewski, Robert V.
000374322 700__ $$aKress, T.
000374322 700__ $$aKrieger, P.
000374322 700__ $$avon Krogh, J.
000374322 700__ $$aKuhl, T.
000374322 700__ $$aKyberd, P.
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000374322 700__ $$aLazic, D.
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000374322 700__ $$aLellouch, D.
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000374322 700__ $$aLloyd, S.L.
000374322 700__ $$aLoebinger, F.K.
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000374322 700__ $$aLosty, M.J.
000374322 700__ $$aLudwig, J.
000374322 700__ $$aLui, D.
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000374322 700__ $$aMattig, Peter
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000374322 700__ $$aMckigney, E.A.
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000374322 700__ $$aPerez-Ochoa, R.
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000374322 700__ $$aRobertson, S.
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000374322 700__ $$aSurrow, B.
000374322 700__ $$aTalbot, S.D.
000374322 700__ $$aTanaka, S.
000374322 700__ $$aTaras, P.
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000374322 700__ $$avon Torne, E.
000374322 700__ $$aTorrence, E.
000374322 700__ $$aTowers, S.
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000374322 700__ $$aTurcot, A.S.
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000374322 700__ $$aVan Kooten, Rick J.
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