G. Glaser
University of Würzburg
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European Physical Journal A | 1988
Z. Jakubowski; C. Peck; H. Marsiske; A. Engler; A. C. König; F. H. Heimlich; P. Zschorsch; G. Drews; U. Strohbusch; D. Sievers; R.W. Kraemer; K. Wachs; C. Pegel; H. Kilian; R.T. Van de Walle; T. Kiel; B. Niczyporuk; J. Tompkins; B. van Uitert; K. Fairfield; R. Cowan; H. W. Bartels; F. Messing; G. Glaser; F. C. Porter; G. Conforto; P. Schmitt; S. Lowe; Daniel Marlow; K. Graaf
AbstractUsing the Crystal Ball detector operating at the DORIS II storage ring we have measured the leptonic partial widthsГee of the Υ(1S) and Υ(2S) resonances. We find
Physics Letters B | 1991
D. Antreasyan; H. W. Bartels; D. Besset; Ch Bieler; J. K. Bienlein; A. Bizzeti; E.D. Bloom; I. Brock; K. Brockmüller; R. Cabenda; A.M. Cartacci; M. Cavalli-Sforza; R. Clare; A. Compagnucci; G. Conforto; S. Cooper; R. Cowan; D. Coyne; A. Engler; K. Fairfield; G. Folger; A. Fridman; J. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; K. Graaf; F. H. Heimlich; F.H. Heinsius; R. Hofstadter
European Physical Journal C | 1990
D. Antreasyan; H. W. Bartels; D. Besset; Ch. Bieler; J. K. Bienlein; Andrea Bizzeti; E. D. Bloom; I. Brock; K. Brockmüller; R. Cabenda; A.M. Cartacci; M. Cavalli-Sforza; R. Clare; A. Compagnucci; G. Conforto; S. Cooper; R. Cowan; D. Coyne; A. Engler; K. Fairfield; G. Folger; A. Fridman; J. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; K. Graaf; F. H. Heimlich; F.-H. Heinsius; R. Hofstadter
\Gamma _{ee} (\Upsilon (1S)) = 1.34 \pm 0.03 \pm 0.06keV
European Physical Journal A | 1990
M. Kobel; C. Peck; H. Marsiske; M. Reidenbach; A. Engler; A. C. König; F. H. Heimlich; P. Zschorsch; U. Strohbusch; D. Sievers; K. Wachs; H. Kilian; R.T. Van de Walle; W. Maschmann; T. Kiel; B. Niczyporuk; J. Tompkins; Dc Williams; B. van Uitert; H. Janssen; K. Fairfield; R. Cowan; F. C. Porter; F. Messing; G. Glaser; G. Conforto; P. Schmitt; S. Lowe; K. Karch; Daniel Marlow
European Physical Journal A | 1990
C. Bieler; C. Peck; H. Marsiske; H. Janssen; A. Engler; A. C. König; F. H. Heimlich; P. Zschorsch; U. Strohbusch; D. Sievers; K. Wachs; H. Kilian; R.T. Van de Walle; T. Kiel; B. Niczyporuk; J. Tompkins; B. van Uitert; K. Fairfield; R. Cowan; H. W. Bartels; F. Messing; G. Glaser; F. C. Porter; G. Conforto; P. Schmitt; S. Lowe; Daniel Marlow; K. Graaf; G. Folger; K. Karch
and
Physical Review D | 1990
H. Marsiske; D. Antreasyan; H. W. Bartels; D. Besset; C. Bieler; J. K. Bienlein; Andrea Bizzeti; E. D. Bloom; Brock I I; K. Brockmüller; R. Cabenda; A.M. Cartacci; M. Cavalli-Sforza; R. Clare; A. Compagnucci; G. Conforto; S. Cooper; R. Cowan; D. Coyne; A. Engler; K. Fairfield; G. Folger; A. Fridman; D. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; K. Graaf; F. H. Heimlich; F.-H. Heinsius
Physical Review D | 1988
Dc Williams; D. Antreasyan; H. W. Bartels; D. Besset; C. Bieler; J. K. Bienlein; Andrea Bizzeti; E. D. Bloom; Brock I I; K. Brockmüller; R. Cabenda; A.M. Cartacci; M. Cavalli-Sforza; R. Clare; A. Compagnucci; G. Conforto; S. Cooper; R. Cowan; D. Coyne; G. Drews; A. Engler; K. Fairfield; G. Folger; A. Fridman; J. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; F. H. Heimlich; R. Hofstadter
\Gamma _{ee} (\Upsilon (2S)) = 0.56 \pm 0.04 \pm 0.02keV.
Physical Review D | 1987
D. Antreasyan; H. W. Bartels; D. Besset; C. Bieler; J. K. Bienlein; Andrea Bizzeti; E. D. Bloom; Brock I I; K. Brockmüller; R. Cabenda; A.M. Cartacci; M. Cavalli-Sforza; R. Clare; G. Conforto; S. Cooper; R. Cowan; D. Coyne; G. Drews; C. Edwards; A. Engler; K. Fairfield; G. Folger; A. Fridman; J. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; F. H. Heimlich; R. Hofstadter; J. Irion
Physics Letters B | 1991
Andrea Bizzeti; G. Glaser; Dc Williams; K. Graaf; H. Meyer; W. Koch; R. Hofstadter; H. Janssen; D. Coyne; A.M. Cartacci; A. C. König; F. H. Heimlich; B. Niczyporuk; U. Volland; G. Conforto; B. Monteleoni; C. Bieler; Z. Jakubowski; A. Voigt; P. Schmitt; G. Godfrey; T. Skwarnicki; S. Keh; B. Lurz; A. Fridman; G. Folger; P. G. Pelfer; W.J. Metzger; K. Wachs; S. Cooper
The effect onГee of applying different prescriptions for radiative corrections is discussed. We also measureR, the ratio of non-resonant hadronic cross section to the Born cross section of μ pair production, at c.m. energyW=9.39 GeV to beR=3.48±0.04±0.16.
Physical Review D | 1988
D. Williams; D. Antreasyan; H. W. Bartels; D. Besset; C. Bieler; J. K. Bienlein; A. Bizzeti; E. D. Bloom; I. Brock; K. Brockm̈ller; R. Cabenda; A. Cartacci; M. Cavalli-Sforza; R. Clare; A. Compagnucci; G. Conforto; S. Cooper; R. Cowan; D. Coyne; G. Drews; A. Engler; K. Fairfield; G. Folger; A. Fridman; J. Gaiser; D. Gelphman; G. Glaser; G. Godfrey; F. H. Heimlich; R. Hofstadter
Abstract The Crystal Ball detector at the DORIS II storage ring at DESY has been used to measure the branching ratios for the decay modes τ ± →h ± π 0 ν and τ ± →h ± π 0 π 0 ν , where h ± is any charged hadron. The results are BR( τ ± → h ± π 0 ν ) = (22.0±0.8±1.9)%, BR( τ ± → h ± π 0 π 0 ν ) = (5.7±0.5 +1.0 −1.7 )%. The first result is in good agreement with the present world average. The decay mode h ± π 0 π 0 ν is reconstructed in τ decays for the first time. Its branching ratio, however, is somewhat lower than the corresponding world average, and therefore tends to increase the one-prong problem.