I. Brock
University of Bonn
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Featured researches published by I. Brock.
Physics Letters B | 1987
P. Avery; D. Besson; T. J. V. Bowcock; R. T. Giles; J. F. Hassard; K. Kinoshita; F. M. Pipkin; Richard Wilson; J. Wolinski; Di Xiao; Thomas R. Gentile; P. Haas; M. Hempstead; T. Jensen; H. Kagan; R. Kass; S. Behrends; Jan M. Guida; Joan A. Guida; F. Morrow; R. Poling; E. H. Thorndike; P. Tipton; M. S. Alam; N. Katayama; I. J. Kim; C. R. Sun; V. Tanikella; D. Bortoletto; A. Chen
Abstract We have set upper limits for rare exclusive decays of B mesons arising from higher order processes in the standard model of electroweak interactions. Such decays may occur via “penguin diagrams” in B decay. We also set an upper limit on a lepton-number-violating decay mode of the neutral B meson.
Journal of Instrumentation | 2009
S. Duarte Pinto; M. Villa; M. Alfonsi; I. Brock; G. Croci; E. David; R. De Oliveira; L. Ropelewski; M. Van Stenis
In 2008, a triple GEM detector prototype with an area of ~ 2000 cm2 has been constructed, based on foils of 66 × 66 cm. GEMs of such dimensions had not been made before, and innovations to the existing technology were introduced to build this detector. This paper discusses these innovations and presents further work on large area GEM development. A single-mask technique overcomes the cumbersome practice of alignment of two masks, which limits the achievable lateral size. The holes obtained with this technique are conical, and have a so-called rim, a small insulating clearance around the hole in the substrate. Further refinements of this technique allow greater control over the shape of holes and the size of rims. Also, an improvement in homogeneity over large areas is expected. Simulation studies have been done to examine the effect of hole shape on the behavior of GEMs. Such studies can help understanding how to use new enhancements of the technique to optimize performance. Many potential applications for large area GEMs foresee large production volumes. Production issues have been studied, and single-mask GEMs turn out to be much more suitable for large scale production than standard GEMs.
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
Journal of Instrumentation | 2009
S. Duarte Pinto; M. Villa; M. Alfonsi; I. Brock; G. Croci; E. David; R. De Oliveira; L. Ropelewski; M. Van Stenis; H. Taureg
ieee nuclear science symposium | 2009
Serge Duarte Pinto; M. Alfonsi; I. Brock; G. Croci; E. David; R. Oliveira; L. Ropelewski; Miranda van Stenis; H. Taureg; Marco Villa
\Gamma _{ee} (\Upsilon (1S)) = 1.34 \pm 0.03 \pm 0.06keV
nuclear science symposium and medical imaging conference | 2010
Serge Duarte Pinto; M. Alfonsi; I. Brock; G. Croci; E. David; R. Oliveira; L. Ropelewski; Miranda van Stenis; H. Taureg; Marco Villa
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
and
arXiv: High Energy Physics - Experiment | 2009
I. Brock
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
\Gamma _{ee} (\Upsilon (2S)) = 0.56 \pm 0.04 \pm 0.02keV.
Journal of Physics: Conference Series | 2014
Péter Kövesárki; I. Brock