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Featured researches published by H. Schulz.


Physics Letters B | 1987

Observation of B0-B0 mixing

H. Albrecht; D.B. MacFarlane; H. Seywerd; R. Gläser; A. Babaev; T.-S. Yoon; P.M. Patel; R. Kutschke; G. Harder; K.W. McLean; J.P. Donker; A. Yagil; R.S. Orr; D. Coppage; B.Paul Padley; H. Schulz; P.C.H. Kim; J. Stiewe; K.R. Schubert; R. Wurth; L. Jönsson; C.W. Darden; V. Ryltsov; S. Kanekal; V. Chistilin; B. Spaan; U. Binder; A. Semenov; J.C. Yun; A. Drescher

Abstract Using the ARGUS detector at the DORIS II storage ring we have searched in three different ways for B0- B 0 mixing in ϒ (4S) decays. One explicitly mixed event, a decay ϒ (4S)→B0B0, has been completely reconstructed. Furthermore, we observe a 4.0 standard deviation signal of 24.8 events with like-sign lepton pairs and a 3.0 standard deviation signal of 4.1 events containing one reconstructed B0( B 0) and an additional fast l+(l)−. This leads to the conclusion that B0- B 0 mixing is substantial. For the mixing parameter we obtain r=0.21±0.08.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1989

Argus: A universal detector at DORIS II

H. Albrecht; U. Binder; P. Böckmann; G. Drews; R. Gläser; G. Harder; H. Hasemann; A. Krolzig; E. Michel; W. Reinsch; W. Schmidt-Parzefall; H. Schröder; H. Schulz; F. Selonke; E. Steinmann; R. Wurth; A. Drescher; B. Gräwe; W. Hofmann; D. Kamp; A. Markees; U. Matthiesen; H. Scheck; B. Spaan; J. Spengler; D. Wegener; R. Heller; K.R. Schubert; J. Stiewe; K. Strahl

Abstract The detector ARGUS has been designed as a universal tool to investigate final states from e + e − annihilation processes in the energy range of the ϒ resonances. ARGUS started operation in October 1982 and has since successfully taken data at the ϒ(1S), ϒ(2S) and ϒ(4S) energies, and in the nearby continuum. The detector combines excellent charged particle identification and good photon energy resolution over more than 90% of the full solid angle. A particle originating from the interaction vertex and leaving the beam tube traverses the following components: the vertex drift chamber, the main drift chamber which determines its momentum and specific ionization, the time-of-flight system through which its velocity is determined, and the electromagnetic calorimeter. Muons pass through the magnet coils and the flux return yoke and finally hit the muon chamber system which surrounds the detector. The momentum resolution of ARGUS is σ (p T ) P T = (0.01 2 + (0.009p T [ GeV /c]) 2 ) 1 2 , the photon energy resolution in the barrel shower counters is σ (E) E = ( 0.072 2 +0.065 2 E[ GeV ] ) 1 2 . Combining the information from all p devices, more than 80% of all charged hadrons can be recognized unambiguously. The electron-hadron and muon-hadron rejection rates are 1:200 and 1:50 respectively.


Physics Letters B | 1990

Search for hadronic b→u decays

H. Albrecht; W. Funk; G. Harder; A. Babaev; K. Reim; L. Jönsson; C. Geyer; Sally Seidel; B. Spaan; R.D. Appuhn; C. E. K. Charlesworth; S. Werner; A. Nippe; S. Khan; V. Shevchenko; K.W. Edwards; M. Paulini; Yu. Zaitsev; B. Fominykh; V. Chistilin; R. Waldi; T. Ruf; G. Herrera; R. Childers; G. Schweda; W. Hofmann; J. Stiewe; V. Lyubimov; A. Drescher; M. Schäfer

Using the ARGUS detector at the e+e− storage ring DORIS II at DESY, we searched for b→u transitions in exclusive hadronic B meson decays. A systematic analysis of B decays into pions has been performed for decay modes with 2–7 pions in the final state. In none of the decays a positive signal was observed. The upper limits obtained on various branching ratios are consistent with the current model predictions.


Physics Letters B | 1990

Observation of Semileptonic Charmless B Meson Decays

H. Albrecht; W. Funk; G. Harder; A. Babaev; K. Reim; L. Jönsson; C. Geyer; Sally Seidel; B. Spaan; R.D. Appuhn; C. E. K. Charlesworth; S. Werner; A. Nippe; S. Khan; V. Shevchenko; K.W. Edwards; M. Paulini; Yu. Zaitsev; B. Fominykh; V. Chistilin; R. Waldi; T. Ruf; G. Herrera; R. Childers; G. Schweda; W. Hofmann; J. Stiewe; V. Lyubimov; A. Drescher; M. Schäfer

Abstract A detailed study of the lepton momentum spectrum in υ (4 S ) decays has been made using the ARGUS detector at the DORIS II e + e − storage ring at DESY. In the region from 2.3 to 2.6 GeV/ c , which is above the endpoint for contributions from B decays via b → c transitions, we observe 41±10 events in excess of known backgrounds. These events are interpreted as a signal for b → u transitions. A model dependent value of 0.10±0.01 is obtained for the ratio of Cabibbo-Kobayashi-Maskawa matrix elements | V ub |/| V cv| , using the Altarelli et al. model.


Physics Letters B | 1987

Measurement of the decay

H. Albrecht; H. Ehrlichmann; T. Hamacher; A. Krüger; A. Nau; A. Nippe; Stefanie Nowak; M. Reidenbach; M. Schäfer; H. Schröder; H. Schulz; M. Walter; R. Wurth; R.D. Appuhn; C. Hast; G. Herrera; H. Kolanoski; A. Lange; A. Lindner; Rainer Mankel; M. Schieber; T. Siegmund; B. Spaan; H. Thurn; D. Töpfer; A. Walther; D. Wegener; M. Paulini; K. Reim; H. Wegener

Using the ARGUS detector at the e + e − storage ring DORIS II at DESY we have investigated the decays B 0 → D ∗− e + v and B 0 →D ∗− μ + ν. The B 0 mesons were produced in 39600 ϒ(4 S )→ B 0 B 0 decays. Assuming electron-muon universality we obtain a branching ratio BR ( B 0 → D ∗− e + v)= BR ( B 0 → D ∗− γm + ν)=(7.0±1.2±1.9)% .


Physics Letters B | 1984

Branching ratio and mass spectrum of the decay ϒ′ → ϒπ+π−

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)%.


Physics Letters B | 1992

A measurement of the tau mass

H. Albrecht; H. Ehrlichmann; T. Hamacher; R. P. Hofmann; T. Kirchhoff; A. Nau; S. Nowak; H. Schröder; H. Schulz; M. Walter; R. Wurth; R.D. Appuhn; C. Hast; 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; Hans Wegener; R. Mundt; T. Oest; R. Reiner

Using the ARGUS detector at the DORIS II storage ring, a new measurement of the mass of the τ lepton has been obtained. An analysis of the tau pseudomass spectrum for decays of the type τ− → π−π−π+ντ finds mτ = 1776.3±2.4±1.4 MeV/c2. This result also leads to an improvement of the upper limit on the ντ mass to mντ < 31 MeV/c2 at the 95% confidence level.


European Physical Journal A | 1990

Exclusive hadronic decays ofB mesons

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

Observation of charmless B meson decays

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; R. Mankel; U. Matthiesen; H. Scheck; G. Schweda; B. Spaan; A. Walther; D. Wegener; J. C. Gabriel; T. Ruf; S. Schael; K.R. Schubert; J. Stiewe

Abstract Using the ARGUS detector at the e + e − storage ring DORIS II, we have observed charmless decays of B mesons into the final states ppπ ± and ppπ + π − . The significance of the signal corresponds to more than five standard deviations. The branching ratios are (5.2±1.4±1.9)×10 −4 for the three-body and (6.0±2.0±2.2)×10 −4 for the four-body final state. These decays cannot proceed via the dominant b→c transitions, and we show that they are not the result of penguin-type processes. Thus, the observed decays must represent b→u quark transitions. Consequently, the Kobayashi-Maskawa matrix element V ub is non-zero.


Physics Letters B | 1988

An improved upper limit on the ντ-mass from the decay π−→π−π−π−π+π+ντ

H. Albrecht; B. Bostjancic; R. Gläser; I. Gorelov; J.A. McKenna; R.C. Fernholz; R. Kutschke; G. Harder; H. Kapitza; H. Schulz; G. Schweda; S. Ball; D.B. MacFarlane; P. Krizan; J.A. Parsons; V. Soloshenko; J. Stiewe; Klaus R. Schubert; R. Wurth; B.Paul Padley; D.M. Gingrich; J. C. Gabriel; V. Lyubimov; V. Ryltsov; V. Chistilin; B. Spaan; U. Binder; A. Semenov; J.P. Donker; A. Drescher

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)%.

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B. Spaan

Technical University of Dortmund

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D. Wegener

Technical University of Dortmund

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H. Kolanoski

Humboldt University of Berlin

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C. Hast

Technical University of Dortmund

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A. Lindner

Technical University of Dortmund

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R. Mankel

Humboldt University of Berlin

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M. Schieber

Technical University of Dortmund

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R.D. Appuhn

Technical University of Dortmund

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H. Thurn

Technical University of Dortmund

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A. Walther

Technical University of Dortmund

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