C. W. Darden
University of South Carolina
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Featured researches published by C. W. Darden.
Physics Letters B | 1984
H. Albrecht; G. Drews; H. Hasemann; A. Philipp; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Selonke; R. Wurth; A. Drescher; B. Gräwe; W. Hofmann; A. Markees; U. Matthiesen; J. Spengler; D. Wegener; R. Heller; K.R. Schubert; J. Stiewe; R. Waldi; S. Weseler; Kasper Edwards; W. R. Frisken; Ch. Fukunaga; M. Goddard; P. Kim; R. S. Orr; P. M. Patel; J. D. Prentice; H. Seywerd
Abstract The reaction e + e − → ϒ ′ → ϒπ + π − , with ϒ → anything, has been measured using the ARGUS detector at DORIS . We obtain a mass difference M ( ϒ ′) − M ( ϒ ) = (562 ± 3) MeV and a decay branching ratio BR( ϒ ′→ ϒπ + π − )=(17.9±0.9±2.1)%. The invariant mass spectrum of the π + π − system differs from phase space, but is well described by a matrix element of the form ( M ππ 2 − λM π 2 ) with λ =2.6±0.5. We also report preliminary results on the exclusive decay ϒ′ → ϒπ + π − , with ϒ → e + e − , and obtain BR( ϒ → e + e − ) = (2.8 ± 0.4 ± 04±0.3)%.
European Physical Journal A | 1990
H. Albrecht; H. Ehrlichmann; G. Harder; A. Krüger; A. Nau; A. W. Nilsson; A. Nippe; T. Oest; M. Reidenbach; M. Schäfer; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Sefkow; R. Wurth; R.D. Appuhn; A. Drescher; C. Hast; G. Herrera; H. Kolanoski; A. Lange; A. Lindner; R. Mankel; H. Scheck; M. Schieber; G. Schweda; B. Spaan; A. Walther; D. Wegener; M. Paulini
Using the ARGUS detector at thee+e− storage ring DORIS II, we have measuredB decays into exclusive final states containing aD orD* meson plus several pions, or containing aJ/ψ or ψ′ meson plus a strange particle. Some of these channels have not been seen before, while others represent updated measurements of previous results. The branching ratios are compared with the predictions of the model of Bauer, Stech and Wirbel. Using the cleanest decay channels, the mass of the charged and neutralB meson are found to bemB−=(5280.5±1.0±2.0) MeV/c2 andmB0=(5279.6±0.7±2.0) MeV/c2 respectively, yielding a mass differencemB0−mB−=(−0.9±1.2±0.5) MeV/c2.
Physics Letters B | 1988
H. Albrecht; B. Bostjancic; H. Seywerd; R. Gläser; A. Babaev; T.-S. Yoon; P. M. Patel; V. Shevchenko; R. Kutschke; G. Harder; K.W. McLean; J.P. Donker; A. Yagil; G. Schweda; S. Ball; D. Coppage; B.Paul Padley; H. Schulz; P. Kim; J. Stiewe; Klaus R. Schubert; R. Wurth; L. Jönsson; C. W. Darden; V. Lyubimov; V. Ryltsov; S. Kanekal; B. Spaan; U. Binder; A. Semenov
Abstract Using the ARGUS detector at the e + e − storage ring DORIS II, we have observed the decay τ − → π − π − π − π + π + ν τ in tau-pair events produced at center-or-mass energies between 9.4 and 10.6 GeV. From the 5π invariant mass distribution we derive an upper limit of m ( ν τ ) c 2 at the 95% confidence level. The branching ratio for this decay channel is found to be (0.064±0.023±0.01)%.
European Physical Journal A | 1991
H. Albrecht; H. Ehrlichmann; R. Gläser; G. Harder; A. Krüger; A. Nau; A. W. Nilsson; A. Nippe; T. Oest; M. Reidenbach; M. Schäfer; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Sefkow; R. Wurth; R.D. Appuhn; A. Drescher; C. Hast; G. Herrera; H. Kolanoski; A. Lange; A. Lindner; R. Mankel; H. Scheck; M. Schieber; G. Schweda; B. Spaan; A. Walther; D. Wegener
The reactionγγ→π+π−π+π− has been studied with the ARGUS detector. The rate in the invariant mass region below 1.8 GeV/c2 is found to be largely due toρ0ρ0 production. A spin-parity analysis shows a dominance of the partial wave (JP,Jz)=(2+, 2) with a small admixture fromJP=0+. The contribution of negative parity states is consistent with zero. The large ratio of cross sectionsσ(γγ→ρ0ρ0)/σ(γγ→ρ+ρ−)≃4, and the dominance of theJP=2+ wave in the reactionγγ→ρ0ρ0 is a signature consistent with the production of an exotic (I=2) resonance.
European Physical Journal C | 1986
H. Albrecht; U. Binder; P. Böckmann; R. Gläser; G. Harder; I. Lembke-Koppitz; A. Philipp; W. Schmidt-Parzefall; H. Schröder; H. Schulz; R. Wurth; A. Yagil; J.P. Donker; A. Drescher; D. Kamp; U. Mattiesen; H. Scheck; B. Spaan; J. Spengler; D. Wegener; J. C. Gabriel; K.R. Schubert; J. Stiewe; K. Strahl; R. Waldi; S. Weseler; Kasper Edwards; W. R. Frisken; Ch. Fukunaga; D.J. Gilkinson
We report a study of the decay τ−→τ−τ+τ−vτ using the ARGUS detector at the DORIS II storage ring. Tau pairs were produced bye+e− annihilation at centre-of-mass energies near 10 GeV. We have observed about 1,700 events, corresponding to a branching ratio for τ−→τ−τ+τ−vτ of (5.6±0.7)%. The dominant mode for this decay is observed to beρ0π− in aJp=1+ spin state. Theρ0π− mass spectrum shows a broad enhancement near 1.10 GeV/c2, which has the properties expected for theA1.
European Physical Journal A | 1991
H. Albrecht; H. Ehrlichmann; T. Hamacher; G. Harder; A. Krüger; A. Nau; A. Nippe; M. Reidenbach; M. Schäfer; H. Schröder; H. Schulz; F. Sefkow; R. Wurth; R.D. Appuhn; C. Hast; G. Herrera; H. Kolanoski; A. Lange; A. Lindner; R. Mankel; M. Schieber; G. Schweda; T. Siegmund; B. Spaan; H. Thurn; A. Walther; D. Wegener; M. Paulini; K. Reim; U. Volland
Using the ARGUS detector at thee+e− storage ring DORIS II at DESY, we have measured the inclusive production ofD0,D+ andD*(2010)+ mesons inB decays and in nonresonante+e− annihilation around 10.6 GeV. The inclusive branching ratios forB decays toD0,D+ andD*+ mesons are found to be (52.2±8.2±3.5)%, (27.2±6.3±3.5)% and (34.8±6.0±3.5)% respectively. Thus,D0 andD+ production account for about 70% of the charm produced inB decays, neglectingb→u contributions to the total width. The production cross sections and momentum spectra for continuume+e− annihilation are also presented.
Physics Letters B | 1992
H. Albrecht; H. Ehrlichmann; T. Hamacher; A. Krüger; A. Nau; A. Nippe; M. Reidenbach; M. Schäfer; H. Schröder; H. Schulz; F. Sefkow; R. Wurth; R.D. Appuhn; C. Hast; G. Herrera; H. Kolanoski; A. Lange; A. Lindner; R. Mankel; M. Schieber; T. Siegmund; B. Spaan; H. Thurn; D. Töpfer; A. Walther; D. Wegener; M. Paulini; K. Reim; U. Volland; H. Wegener
Abstract Using the ARGUS detector at the e + e − storage ring DORIS II at DESY, we have observed parity violation in the decay Λ ± c → Λπ ± . We measure the coefficient of parity violation, α Λ c , to be −0.96±0.42. In addition, we measure σ BR ( Λ + c → Λπ + and σ BR ( Λ + c → Σ 0 π + ) to be, respectively, (2.2±0.3±0.4) pb and (2.0±0.7±0.4) pb.
European Physical Journal C | 1989
H. Albrecht; P. Böckmann; R. Gläser; G. Harder; A. Krüger; A. Nippe; M. Reidenbach; M. Schäfer; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Sefkow; J. Spengler; R. Wurth; A. Yagil; R.D. Appuhn; A. Drescher; C. Hast; G. Herrera; D. Kamp; H. Kolanoski; A. Lindner; R. Mankel; H. Scheck; G. Schweda; B. Spaan; A. Walther; D. Wegener; W. Funk; J. C. Gabriel
AbstractUsing the ARGUS detector at thee+e− storage ring DORIS II, we have investigated inclusive production of π±,K±,Ks0 and
European Physical Journal A | 1988
H. Albrecht; P. Böckmann; R. Gläser; G. Harder; A. Krüger; A. Nippe; M. Schäfer; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Sefkow; J. Spengler; R. Wurth; A. Yagil; R.D. Appuhn; A. Drescher; D. Kamp; H. Kolanoski; U. Matthiesen; H. Scheck; G. Schweda; B. Spaan; A. Walther; D. Wegener; J. C. Gabriel; T. Ruf; K.R. Schubert; J. Stiewe; K. Strahl; R. Waldi
Physics Letters B | 1985
H. Albrecht; D.B. MacFarlane; H. Seywerd; D. Coppage; N.N. Brown; T.-S. Yoon; R.S. Orr; P.M. Patel; R. Kutschke; G. Harder; H. Kapitza; I. Lembke-Koppitz; B.Paul Padley; H. Schulz; P.C.H. Kim; V. Ryltsov; J. Stiewe; K.R. Schubert; R. Wurth; L. Jönsson; A. Babaev; C. W. Darden; A. Philipp; S. Kanekal; Y. Oku; U. Binder; K.W. McLean; A. Semenov; J.C. Yun; A. Drescher
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