J. von Krogh
Heidelberg University
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Featured researches published by J. von Krogh.
Physics Letters B | 1973
F.J. Hasert; S. Kabe; W. Krenz; J. von Krogh; D. Lanske; J. Morfin; K. Schultze; H. Weerts; G.H. Bertrand-Coremans; J. Sacton; W. Van Doninck; P. Vilain; U. Camerini; D. Cundy; R. Baldi; I. Danilchenko; W.F. Fry; D. Haidt; S. Natali; P. Musset; B. Osculati; R.B. Palmer; J.B.M. Pattison; D.H. Perkins; A. Pullia; A. Rousset; W. Venus; H. Wachsmuth; V. Brisson; B. Degrange
Abstract Events induced by neutral particles and producing hadrons, but no muon or electron, have been observed in the CERN neutrino experiment. These events behave as expected if they arise from neutral current induced processes. The rates relative to the corresponding charged current processes are evaluated.
Physics Letters B | 1988
S. Bethke; B. Naroska; F. Foster; K. Ambrus; F. K. Loebinger; S. L. Cartwright; K. Stephens; K. H. Hellenbrand; R. Marshall; J. von Krogh; M. Minowa; J. A. J. Skard; L. Smolik; H. von der Schmitt; J. Spitzer; M. Zimmer; T. Greenshaw; Roger Barlow; P. Steffen; G. Heinzelmann; J. Heintze; G. Hughes; J. Chrin; J. Hagemann; F. Ould-Saada; M. Kuhlen; A.A. Macbeth; U. Schneekloth; E. Elsen; P.G. Murphy
The energy dependence of the relative production rate of three-jet events is studied in hadronic e+e− annihilation events at center of mass energies between 22 and 46.7 GeV. Three-jet events are defined by a jet finding algorithm which is closely related to the definition of resolvable jets used in O(αs2) perturbative QCD calculations, where the relative production rate of three-jet events is roughly proportional to the size of the strong coupling strength. The production rates of three-jet events in the data decrease significantly with increasing centre of mass energy. The experimental rates, which are independent of fragmentation model calculations, can be directly compared to theoretically calculated jet production rates and are in good agreement with the QCD expectations of a running coupling strength. The hypothesis of an energy independent coupling constant can be excluded with a significance of four standard derivations.
European Physical Journal A | 1986
W. Bartel; L. Becker; R. Felst; D. Haidt; G. Knies; H. Krehbiel; P. Laurikainen; N. Magnussen; R. Meinke; B. Naroska; J.E. Olsson; D. Schmidt; G. Dietrich; T. Greenshaw; J. Hagemann; G. Heinzelmann; H. Kado; C. Kleinwort; M. Kuhlen; A. Petersen; R. Ramcke; U. Schneekloth; G. Weber; K. Ambrus; S. Bethke; A. Dieckmann; E. Elsen; J. Heintze; K. H. Hellenbrand; S. Komamiya
Hadronic jet production bye+e−-annihilation has been studied in the energy range of 14.0–46.7 GeV. The data have been analysed in terms of a cluster algorithm and other topological quantities. The results are compared with 2nd order QCD calculations which incorporate models for the fragmentation of quarks and gluons into hadrons. At the higher energies we observe more spherical and 4-jet like events than predicted by these calculations. We cannot achieve a simultaneous description of the observed 3- and 4-jet production by adjusting the strong coupling constant αs or the fragmentation parameters of the 2nd order QCD models. The observed excess of spherical events can partially be explained by the production of multi-parton events expected from higher order QCD contributions. Consequences of the presented results for the value of αs, determined in previous analyses, are discussed. QCD parton shower models, including soft gluon interference, are able to describe the observed number of spherical events.
Physics Letters B | 1973
F.J. Hasert; H. Faissner; W. Krenz; J. von Krogh; D. Lanske; J. Morfin; K. Schultze; H. Weerts; G.H. Bertrand-Coremans; J. Lemonne; J. Sacton; W. Van Doninck; P. Vilain; C. Baltay; D. Cundy; D. Haidt; M. Jaffre; P. Musset; A. Pullia; S. Natali; J.B.M. Pattison; D.H. Perkins; A. Rousset; W. Venus; H. Wachsmuth; V. Brisson; B. Degrange; M. Haguenauer; L. Kluberg; U. Nguyen-Khac
Abstract One possible event of the process ν − μ + e − → v − μ + e − has been observed. The various background processes are discussed and the event interpreted in terms of the Weinberg theory. The 90% confidence limits on the Weinberg parameter are 0.1 2 θ W
Physics Letters B | 1980
W. Bartel; S. Orito; B. Naroska; F. Foster; C. Yanagisawa; J. Allison; G. Heinzelmann; Y. Watanabe; I. P. Duerdoth; P. Lennert; L.H. O'Neill; K. Stephens; P. Dittmann; R. Marshall; M. Minowa; D.C. Darvill; W.L. Yen; G. Weber; H. Drumm; S. Yamada; P. Steffen; Bt King; J. Heintze; G. Hughes; T. Canzler; Jf Hassard; T. Nozaki; H. Wriedt; F. K. Loebinger; S. Kawabata
Abstract Topological distributions of charged and neutral hadrons from the reaction e+e− → multihadrons are studied at √s of about 30 GeV. An excess of planar events is observed at a rate which cannot be explained by statistical fluctuations in the standard two-jet process. The planar events, mostly consisting of a slim jet on one side and a broader jet on the other, are shown actually to possess three-jet structure by demonstrating that the broader jet itself consists of two collinear jets in its own rest system. Detailed agreement between data and predictions is obtained if the process e + e − →q q g is taken into account. This strongly suggests gluon bremsstrahlung as the origin of the planar three-jet events. By comparison of the data with the qqg-model we obtain a value for the strong coupling constant of αS(q2 = 0.17 ± 0.04.
Physics Letters B | 1973
T. Eichten; H. Faissner; F.J. Hasert; S. Kabe; W. Krenz; J. von Krogh; J. Morfin; K. Schultze; G.H. Bertrand-Coremans; J. Sacton; W. Van Doninck; P. Vilain; D. Cundy; D. Haidt; M. Jaffre; S. Natali; P. Musset; J.B.M. Pattison; D.H. Perkins; A. Pullia; A. Rousset; W. Venus; H. Wachsmuth; V. Brisson; B. Degrange; M. Haguenauer; L. Kluberg; U. Nguyen-Khac; P. Petiau; E. Bellotti
Abstract The v and v nucleon total cross-sections have been determined as a function of energy using a sample of 2500 v and 950 v event. The results are compared with predictions of scaling and charge symmetry hypotheses.
Physics Letters B | 1979
W. Bartel; T. Canzler; D. Cords; P. Dittmann; R. Eichler; R. Felst; E. Gadermann; D. Haidt; S. Kawabata; H. Krehbiel; B. Naroska; L.H. O'Neill; J.E. Olsson; P. Steffen; W.L. Yen; E. Elsen; M. Helm; A. Petersen; H. Riege; P. Warming; G. Weber; H. Drumm; W. Farr; J. Heintze; G. Heinzelmann; R.D. Heuer; J. von Krogh; P. Lennert; H. Matsumura; T. Nosaki
Abstract The cross section for the process e+e− → multihadrons has been measured at the highest PETRA energies. We measure R (the total cross section in units of the point-like e+e- → μ+μ- cross section) to be 2.9 ± 0.7, 4.0 ± 0.5, 4.6 ± 0.4 and 4.2 ± 0.6 at s of 22, 27.7, 30 and 31.6 GeV, respectively. The observed average multiplicity, together with existing low energy data, indicate a rapid increase in multiplicity with increasing energy.
Physics Letters B | 1981
W. Bartel; D. Cords; P. Dittmann; R. Eichler; R. Felst; D. Haidt; H. Krehbiel; B. Naroska; L.H. O'Neill; P. Steffen; H. Wenninger; Y. Zhang; E. Elsen; M. Helm; A. Petersen; P. Warming; G. Weber; S. Bethke; H. Drumm; J. Heintze; G. Heinzelmann; K. H. Hellenbrand; R.D. Heuer; J. von Krogh; P. Lennert; S. Kawabata; H. Matsumura; T. Nozaki; J. Olsson; H. Rieseberg
Abstract Data on hadron production by e + e − -annihilation at c.m. energies between 30 GeV and 36 GeV are presented and compared with two models both based on first-order QCD but using different schemes for the fragmentation of quarks and gluons into hadrons. In one model the fragmentation proceeds along the parton momenta, in the other along the colour-anticolour axes. The data are reproduced better by fragmentation along the colour axes.
Physics Letters B | 1978
P.C. Bosetti; H. Deden; M. Deutschmann; P. Fritze; H. Grässler; W. Krenz; J. Morfin; P. Schmitz; R. Schulte; K. Schultze; H. Seyfert; K. Böckmann; H. Emans; C. Geich-Gimbel; R. Hartmann; E. Heilmann; T. P. Kokott; B. Nellen; R. Pech; R. Rödel; V.T. Cocconi; B. Conforto; D. Cundy; J. Figiel; W. F. Fry; A. Grant; D. Haidt; P.O. Hulth; G. Kellner; D.J. Kocher
Abstract In 70 000 photos taken in BEBC during an experiment in which the 400 GeV proton beam of the CERN SPS was dumped into a massive Cu target 820 m upstream of BEBC, 70 interactions induced by neutral primaries above 10 GeV were observed. In 11 events the secondary charged lepton is an e − , in four events an e + . This number of electron events cannot be due to electron neutrinos from conventional sources (K, Λ, Σ − decays). The flux of the additional (prompt) neutrinos is evaluated. Possible origins are discussed in terms of charmed particles, τs, and as yet undiscovered particles. Limits are given on axion production.
Nuclear Physics | 1974
F.J. Hasert; S. Kabe; W. Krenz; J. von Krogh; D. Lanske; J. Morfin; K. Schultze; H. Weerts; G.H. Bertrand-Coremans; J. Sacton; W. Van Doninck; P. Vilain; R. Baldi; U. Camerini; D. Cundy; I. Danilchenko; W.F. Fry; D. Haidt; S. Natali; P. Musset; B. Osculati; R.B. Palmer; J.B.M. Pattison; D.H. Perkins; A. Pullia; A. Rousset; W. Venus; H. Wachsmuth; V. Brisson; B. Degrange
Events induced by neutral particles and producing only hadrons, but no muon or electron, have been observed in the heavy liquid bubble chamber Gargamelle exposed to neutrino (v) and antineutrino (v) beams at CERN. A study of the various sources which could give rise to such events reveals that less than 20% could be attributed to neutrons or KL°. The events behave as expected if they arise from neutral current processes induced by neutrinos and antineutrinos. The ratio of the number of these events to the number of corresponding events with charged lepton is 0.22 ± 0.04 for v and 0.43 ± 0.12 for v.