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Featured researches published by J. Engler.


Physica Scripta | 1981

Cello-A New Detector at PETRA

Mina-Jacqueline Schachter; H-J Behrend; J. H. Field; V. Schröder; H. Sindt; W.D. Apel; J. Bodenkamp; D. Chrobaczek; J. Engler; D.C. Fries; G. Flügge; F. Mönnig; H. Müller; H. Randoll; G. Schmidt; H. Schneider; W. de Boer; G. Buschhorn; G. Grindhammer; P. Grosse-Wiesmann; B. Gunderson; C. Kiesling; R. Kotthaus; H. Lierl; D. Lüers; T. Meyer; L. Moss; H. Oberlack; P. Schacht; A. Snyder

A description of the design characteristics of CELLO, a large 4Π magnetic detector at PETRA, is given and first results of beam operation are presented.


European Physical Journal A | 1992

An Experimental study of the process gamma gamma ---> pi+ pi-

H.-J. Behrend; M. Iacovacci; F. Le Diberder; T. Weihrich; G.G. Winter; P. Grosse-Wiesmann; H. Schneider; J. Haissinski; J. Meyer; M. Davier; J. Fuster; G. Flügge; V. Blobel; B. Stella; D.C. Fries; C. Milstene; G. Grindhammer; G. D'Agostini; J. Ahme; H. Muller; W. de Boer; H. Spitzer; W. Wiedenmann; W.D. Apel; G. Alexander; F. Ferrarotto; J. Engler; V. Schroeder; S. Scholz; M. Feindt

Using the CELLO detector, we have measured cross sections for the processγγ→π+π− in the mass range 0.75–1.9 GeV/c2. A partial wave fit to the data indicates the presence of a sizeableS-wave amplitude with signs of resonant behaviour. Values for the γγ width of thef2(1270) are given, showing the model-dependence of this quantity. At higher dipion masses, the model of Brodsky and Lepage is found to give an order of magnitude description of the data.


Physics Letters B | 1982

Scalar lepton search with the CELLO detector at PETRA

H.-J. Behrend; D. Fournier; F. Le Diberder; W.D. Apel; R. Aleksan; P. Grosse-Wiesmann; H. Schneider; M.-J. Schachter; S. Banerjee; V. Journé; M. Davier; M. Rivoal; G. Flügge; J. Engler; G. Grindhammer; G. D'Agostini; U. Mallik; A. Snyder; H. Müller; V. Schröder; W. de Boer; D. Chrobaczek; B. Gunderson; J.P. Pansart; F. Pierre; D.C. Fries; H. Randoll; Y. Lavagne; F. Kapusta; G. Schmidt

Abstract We report on the search for “supersymmetric” scalar leptons conducted with the CELLO detector, at the PETRA e + e − storage ring. 11.1 pb −1 of high energy data were analysed ( 33 GeV s GeV ). At a 95% c.l., the existence of a scalar e is ruled out for masses between 2 GeV and 16.8 GeV; correspondingly, a scalar μ is excluded between 3.3 GeV and 16 GeV, and a scalar τ between 6 GeV and 15.3 GeV, as well as between the τ mass and 3.8 GeV.


Archive | 1991

A measurement of the π0, η and η′ electromagnetic form factors

H.-J. Behrend; L. Criegee; J. H. Field; G. Franke; H. Jung; J. Meyer; O. Podobrin; V. Schröder; G.G. Winter; P. Bussey; A. Campbell; D. Hendry; S. J. Lumsdon; I.O. Skillicorn; J. Ahme; V. Blobel; M. Feindt; H. Fenner; J. Harjes; J. H. Köhne; J. H. Peters; H. Spitzer; T. Weihrich; W.D. Apel; J. Engler; G. Flügge; D.C. Fries; J. Fuster; K. Gamerdinger; P. Grosse-Wiesmann

We present measurement of the π0γ*γ, ηγ*γ and η′γ*γ form factors. The π0-form factor is for the first time observed in the space-like region. The transition form factor of the η-meson is determined from its decay modes π+π−π0, π+π−γ and the neutral decay mode γγ. The decay of the η′ is observed in the decay channels ργ, ηπ+π− with η→γγ and in the four charged prong final state stemming from ηπ+π− with the η decaying into π+π−(π0/γ). All form factors agree well with a simple ρ-pole predicted by the vector meson dominance model and also with the QCD inspired Brodsky-Lepage model.


Physics Letters B | 1983

Investigation of two photon final states in e+e− annihilation at <√s⪢ = 34.2 GeV

H.-J. Behrend; Ch. Chen; H. Fenner; U. Gümpel; M.-J. Schachter; V. Schröder; H. Sindt; G. D'Agostini; W.D. Apel; S. Banerjee; J. Bodenkamp; J. Engler; G. Flügge; D.C. Fries; W. Fues; K. Gamerdinger; G. Hopp; H. Küster; H. Müller; H. Randoll; G. Schmidt; H. Schneider; W. de Boer; G. Buschhorn; G. Grindhammer; P. Grosse-Wiesmann; B. Gunderson; C. Kiesling; R. Kotthaus; U. Kruse

Abstract Two photon final states in e + e − annihilation have been analyzed at CM energies around 34 GeV. Good agreement with QED is observed. Lower limits for the QED cutoff parameters of Λ + > 59 GeV and Λ - > 44 GeV are determined. A search for two photons with missing energy yields an upper limit for the production of neutral particles which decay into a photon and a non-interacting particle. Constraints on the mass and the coupling strength of supersymmetric photinos are discussed.


Physics Letters B | 1982

Measurement of e+e−→τ+τ− at high energy and properties of the τ lepton

H.-J. Behrend; Ch. Chen; H. Fenner; J. H. Field; V. Schröder; H. Sindt; G. D'Agostini; W.D. Apel; S. Banerjee; J. Bodenkamp; D. Chrobaczek; J. Engler; G. Flügge; D.C. Fries; W. Fues; K. Gamerdinger; G. Hopp; H. Küster; H. Müller; H. Randoll; G. Schmidt; H. Schneider; W. de Boer; G. Buschhorn; G. Grindhammer; P. Grosse-Wiesmann; B. Gunderson; C. Kiesling; R. Kotthaus; U. Kruse

Abstract The e+e−→τ+τ− process has been measured using the CELLO detector at a mean total centre of mass energy of 34.2 GeV using essentially all the decay channels of the τ lepton. The measured cross section yields Rτ=1.03±0.05 (stat)±0.07 (syst). Topological branching fraction are given for τ → 1, 3 or 5 charged tracks. The angular distribution shows a clear 1 + cos2θ dependance with a forward-backward asymmetry of -0.103 ± 0.052 corresponding to an axial-vector coupling aτ of the τ to the weak neutral current given by aτ=−1.12 ± 0.57.


Physics Letters B | 1984

Search for new heavy quarks in

H.-J. Behrend; F. Le Diberder; P. Grosse-Wiesmann; M. Davier; G. D'Agostini; D.C. Fries; H. Fenner; P. Bussey; P. Schacht; J. Haissinski; W. Fues; Y. Ducros; J. Grunhaus; J.M. Scarr; L. Poggioli; D. Lüers; M. Goldberg; R. George; L. Criegee; G. Bonneaud; W. Zimmermann; W. de Boer; H. Spitzer; Y. Lavagne; J.P. Pansart; P. Colas; J.F. Grivaz; G. Bella; D. Fournier; A. Gaidot

Abstract The total e + e − annihilation onto hadron has been measured at CM energies between 33.00 and 36.72 GeV and between 38.66 and 46.78 GeV in steps of 20 and 30 MeV respectively. The average of the ratio R = σ ( e + e − → hadrons )/ σ is 〈 R 〉=3.85±0.12 and 〈 R 〉=4.04±0.10 for the two energy ranges. The systematic error on 〈 R 〉 is 0.31. Both values are consistent with the expectation for the known coloured quarks u, d, s, c and b. No evidence was found for the production of new quarks. If the largest fluctuation in R is interpreted as a narrow resonance, it corresponds to a product of the electronic width and the hadronic branching ratio Γ ee B had >2.9 keV at the 95% confidence level, well below the value expected for the toponium vector ground state with charge 2 3 e . The observed number of aplanar final states rules out the continuum production of a a new heavy flavour with pointlike cross section up to a CM energy of 45.4 GeV for a quarck charge of 1 3 e . and up to 46.6 GeV for 2 3 e at the 95% confidence level.


Physics Letters B | 1984

e^+e^-

H.-J. Behrend; H. Fenner; M.-J. Schachter; V. Schröder; H. Sindt; O. Achterberg; G. D'Agostini; W.D. Apel; J. Engler; G. Flügge; B. Forstbauer; D.C. Fries; W. Fues; K. Gamerdinger; Th. Henkes; G. Hopp; M. Krüger; H. Küster; H. Müller; H. Randoll; G. Schmidt; H. Schneider; W. de Boer; G. Buschhorn; G. Grindhammer; P. Grosse-Wiesmann; B. Gunderson; C. Kiesling; R. Kotthaus; U. Kruse

Abstract Hadronic events obtained with the CELLO detector at PETRA are compared with second order QCD predictions using different models for the fragmentation of quarks and gluons into hadrons. We find that the model dependence in the determination of the strong coupling constant persists when going from first to second order QCD calculations.


Physics Letters B | 1989

collisions up to 46.78 GeV cm energy

H.-J. Behrend; L. Criegee; J.B. Dainton; J. H. Field; G. Franke; H. Jung; J. Meyer; V. Schröder; G.G. Winter; P. Bussey; Craig Buttar; A.J. Campbell; D. Hendry; J.M. Scarr; I.O. Skillicorn; K. M. Smith; J. Ahme; V. Blobel; W. Brehm; M. Feindt; H. Fenner; J. Harjes; J. H. Peters; O. Podobrin; H. Spitzer; W.D. Apel; J. Engler; G. Flügge; D.C. Fries; J. Fuster

Abstract The reaction e + e − → τ + τ − has been studied at centre of mass energies between 14.0 and 46.8 GeV with the CELLO detector at the PETRA e + e − collider. We present results for the cross section σ τ and the charge asymmetry A τ . The results are in good agreement with the standard model. We have also measured the topological decay rates BR 1 , BR 3 and BR 5 for the inclusive decay of the τ lepton into one, three and five charge particles. The results confirm and improve earlier CELLO measurements at other energies. We find for the combined values at all energies BR 1 = (84.9 ± 0.4 ± 0.3)%, BR 3 = (15.0 ± 0.4 ± 0.3)% and BR 5 = (0.16 ± 0.13 ± 0.04)%.


Physics Letters B | 1982

On the model dependence of the determination of the strong coupling constant in second order QCD from e+e−-annihilation into hadrons

H.-J. Behrend; Ch. Chen; J. H. Field; U. Gümpel; V. Schröder; H. Sindt; W.D. Apel; S. Banerjee; J. Bodenkamp; D. Chrobaczek; J. Engler; G. Flügge; D.C. Fries; W. Fues; G. Hopp; H. Küster; H. Müller; H. Randoll; G. Schmidt; H. Schneider; W. de Boer; G. Buschhorn; G. Grindhammer; P. Grosse-Wiesmann; B. Gunderson; C. Kiesling; R. Kotthaus; U. Kruse; H. Lierl; D. Lüers

Abstract The topology of hadronic e + e − annihilation events has been analysed using the sphericity tensor and a cluster method. Comparison with quark models including gluon bremsstrahlung yields good agreement with the data. The strong-coupling constant is determined in 1st order QCD to be α S =0.19±0.04 (stat) ± 0.04 (syst.) at 22 GeV and α S =0.16 ±0.02± 0.03 at 34 GeV. The differential cross section with respect to the energy fraction carried by the most energetic parton agrees with the prediction of QCD, but cannot be reproduced by a scalar gluon model. These results are stable against variations of the transverse momentum distribution of the fragmentation function within the quoted errors.

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W.D. Apel

Karlsruhe Institute of Technology

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D.C. Fries

Karlsruhe Institute of Technology

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H. Fenner

University of Hamburg

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G. Flügge

RWTH Aachen University

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G.G. Winter

Sapienza University of Rome

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G. Franke

Karlsruhe Institute of Technology

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L. Criegee

Karlsruhe Institute of Technology

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V. Blobel

University of Hamburg

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