Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where V. Lubimov is active.

Publication


Featured researches published by V. Lubimov.


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 | 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 | 1987

B meson decays into charmonium states

H. Albrecht; A.A. Andam; U. Binder; P. Böckmann; R. Gläser; G. Harder; A. Krüger; A. Nippe; M. Schäfer; W. Schmidt-Parzefall; H. Schröder; H. Schulz; R. Wurth; A. Yagil; J.P. Donker; A. Drescher; D. Kamp; H. Kolanoski; U. Matthiesen; H. Scheck; B. Spaan; J. Spengler; D. Wegener; J. C. Gabriel; T. Ruf; K.R. Schubert; J. Stiewe; K. Strahl; R. Waldi; K.W. Edwards

Abstract Using the ARGUS detector at the e +e− storage ring DORIS II, we have studied the colour-suppressed decays B → J ψ X and B→ψ′ X. We find the inclusive branching ratios for these two channels to be (1.07±0.16±0.19) % and (0.46±0.17±0.11) %, respectively. From a sample of reconstructed exclusive events the masses of the B0 and B+ mesons are determined to be (5279.5±1.6±3.0) MeV c 2 and (5278.5±1.8±3.0) MeV c 2 , respectively. Branching ratios are determined from five events of the type B 0 → J ψ K ∗0 and three of B+→J/ψ K+. In the same data sample a search for B0→e+e−, μ+μ− and μ±e∓ leads to upper limits for such decays.


Physics Letters B | 1990

Study of inclusive semileptonic B meson decays

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

Abstract Using the ARGUS detector at the e + e − storage ring DORIS-II, we have measured the inclusive semileptonic decays of B-mesons into electrons and muons. The data originate from 220.5 events/pb on the ϒ(4S) resonance. We find BR (B→e + v e X = (10.3 ± 0.6 ± 0.2)% and BR (B→ μ + v μ X) = (10.0 ± 0.6 ± 0.2)% using the model of Altarelli et al. for extrapolating over all lepton momenta, and BR (B→e + v e X) = (9.9±0.6)%, BR(B→ μ + v μ X) = (9.7±0.6)% using the model of Grinstein et al. For semileptonic decays into baryons, we obtain an upper limit of BR ( B → p e + v X ) CL ) .


Physics Letters B | 1990

Determination of the tau-neutrino helicity

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

Abstract Using the ARGUS detector at the DORIS II e + e − storage ring we measured for the first time the τ neutrino helicity from a parity violating asymmetry in the τ decay into three charged pions. From the measured asymmetry we derived the normalized product of the axial and vector coupling constant 2 g A g v / ( g A 2 + g V 2 ) = 1.14±0.34 −0.17 0.34 , which is in good agreement with the standard model prediction.


Physics Letters B | 1989

Observation of the D∗0(2459) IN e+e− annihilation

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; 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; U. Volland; H. Wegener; W. Funk

Abstract Using the ARGUS detector at the DORIS II storage ring at DESY, we have observed a charmed meson of mass (2455±3±5) MeV/c2, decaying to D + π − . The natural width of this state is determined to be (15 +13+5 −10−10 ) MeV c 2 . The fragmentation function is hard, as expected for a leading charmed particle from nonresonant e + e − annihilation. Analysis of the decay angular distribution supports the hypothesis that the observed state is an L =1 excited charmed meson with spin-parity 2 + .


Physics Letters B | 1987

Evidence for the decay τ−→ντωπ−

H. Albrecht; U. Binder; P. Böckmann; R. Gläser; G. Harder; I. Lembke-Koppitz; W. Schmidt-Parzefall; H. Schröder; H. Schulz; R. Wurth; A. Yagil; J.P. Donker; A. Drescher; D. Kamp; U. Matthiesen; H. Scheck; B. Spaan; J. Spengler; D. Wegener; J. C. Gabriel; K.R. Schubert; J. Stiewe; K. Strahl; R. Waldi; S. Weseler; K.W. Edwards; W.R. Frisken; D.J. Gilkinson; D.M. Gingrich; H. Kapitza

Abstract Using the ARGUS detector at DORIS II, we have analyzed tau decays into π − π − π + π 0 ν τ . The branching ratio was determined to be (4.2±0.5±0.9)%. From a study of the three pion sub-system, we find evidence for the decay τ − → ωπ − ν τ with a branching ratio of (1.5±0.3±0.3)%. The ωπ − system is found to be predominantly in a J P =1 − state. There is no evidence for second-class axial-vector currents. The spectral function for the ωπ − final state is in agreement with a prediction based on CVC and σ e + e −→ ωπ 0 .

Collaboration


Dive into the V. Lubimov's collaboration.

Top Co-Authors

Avatar

D. Wegener

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

B. Spaan

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

H. Kolanoski

Humboldt University of Berlin

View shared research outputs
Top Co-Authors

Avatar

R. Mankel

Humboldt University of Berlin

View shared research outputs
Top Co-Authors

Avatar

C. Hast

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

A. Lindner

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

R.D. Appuhn

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

A. Walther

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar
Researchain Logo
Decentralizing Knowledge