U. Gensch
CERN
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Featured researches published by U. Gensch.
Nuclear Physics | 1973
P. Bosetti; H. Grässler; H. Kirk; M. Matziolis; U. Gensch; P. Kostka; K. Böckmann; G.J. Bossen; J. Lowsky; M. Rost; T. Besliu; V.T. Cocconi; P.F. Dalpiaz; P. Duinker; S. Matsumoto; D.R.O. Morrison; R. Stroynowski; H. Wahl; T. Coghen; W. Zielinski; S. Brandt; M. Bardadin-Otwinowska; T. Hofmokl
Abstract Invariant single-particle cross sections for pion and proton production in π ± p interactions at 8 and 16 GeV/ c are presented in terms of integrated distributions as functions of x , reduced rapidity ζ and p ⊥ 2 , and also in terms of double differential cross sections E d 2 σ /(d x d p ⊥ 2 ) and d ζ d p ⊥ 2 ). A comparison of π ± and π − induced reactions is made and the energy dependence is discussed. It is shown that the single-particle structure function cannot be factorized in its dependece on transverse and longitudinal momentum. For the beam-unlike pion, there is an indication for factorizability in terms of rapidity and transverse momentum in a small central region.
Nuclear Physics | 1975
P. Bosetti; G. Otter; G. Rudolph; H.H. Seyfert; U. Gensch; J. Klabuhn; K. Böckmann; R. Hartmann; J. Lowsky; G. Zobernig; V.T. Cocconi; M.J. Counihan; J.D. Hansen; S. Humble; G. Kellner; D.R.O. Morrison; P. Schmid; R. Stroynowski; E. Leitner; J. Stiewe; P.J. Dornan; B. Pollock; P.R. Thornton; J. M. MacNaughton; M. Markytan; J. Strauss
Abstract A comparison is made of the low-mass three-meson systems (πππ), (Kππ), (π K K ) and ( K K K ) diffractively produced in the reaction meson + proton → three mesons + proton. Several striking similarities and a few important differences are observed: (i) the reactions are consistent with the assumption that the three mesons decay entirely into a 0− meson and a 0+, 1− or 2+ resonance; (ii) the three-meson mass spectra have a peak ≈ 250 MeV above the effective threshold Meff of the dominant decay mode and then fall off approximately as (mass)−3;(iii) the average spin 〈J〉 = 0.55 + 1.1 Qeff, where Qeff = M - Meff; (iv) the average orbital angular momentum 〈l〉 increases according to 〈l〉 = 0.75 Qeff; (v) the three-meson states are produced dominantly in unnatural spin-parity states and no evidence for their being resonant is found; (vi) the only natural spin-parity states found are the well-established 2+ resonances A2 and K∗ (1420); they have similar properties to the non-resonant unnatural parity states except for a dip at t = 0 in the dσ/dt distributions; (vii) both the unnatural and natural spin-parity states are produced mostly by an exchange of natural parity; (viii) there is evidence for two types of production mechanism with different polarization properties, one approximately conserving helicity in the t-channel and the other in the s-channel.
Nuclear Physics | 1974
Edmond L. Berger; V.T. Cocconi; M.J. Counihan; T. Coghen; U. Gensch; V. Karimäki; G. Kellner; A. Kotański; D. Kuhn; D.R.O. Morrison; P. Schmidt; D. Sotiriou; R. Stroynowski; F.A. Triantis; H. Wahl
Abstract Charged particle multiplicity cross sections for 100 GeV/ c π − p inelastic interactions are presented and compared with results at other energies. The results for multiplicities n ⪖ 4 show a consistent trend in their energy dependence. The two-prong cross section curve differs as it tends to flatten off at the higher energies. The zero-prong cross section values decrease steeply as p lab −1.1 . The results for n ⩾ 2 for π − p and pp reactions appear to lie on a “universal” curve if nσ n / σ inel is plotted against 〈 n 〉/ n . This “scaling” rule is equivalent to KNO scaling, but the plot suggested here is more useful in studying low multiplicities. An interpretation in terms of a two-component model and a possible extrapolation to higher energies are proposed.
Nuclear Physics | 1975
H. Grässler; H. Kirk; R. Schulte; U. Gensch; J. Klabuhn; H. Hofmann; J. Lowsky; B.U. Stöcker; Edmond L. Berger; M.J. Counihan; S. Humble; G. Kellner; V. Karimäki; D. Kuhn; D.R.O. Morrison; P. Schmid; K. Dziunikowska; W. Zielinski; T. Hirose; J. Stiewe; M. Szczekowski
Abstract We study the multiplicity distributions and the correlations of charged particles produced forward and backward in the centre-of-mass system. The correlations are small but significant. This type of analysis shows clearly the presence of the diffractive component of the inelastic cross section, amounting to about 15% of it. It is also apparent that KNO multiplicity scaling is not satisfied.
European Physical Journal C | 1983
R. Göttgens; J. M. Kohli; P. Sixel; U. Gensch; H. Vogt; Y. Goldschmidt-Clermont; D. R. O. Morrison; R. T. Ross; S. Squarcia; J. Chwastowski; M. W. Krasny; L. Suszycki; W. Zielinski; P. Girtler; D. Kuhn; K.W.J. Barnham; P. R. S. Wright; M. Zomorrodian; D. I. Patalakha; A. M. Moissev; J. MacNaughton; F. Mandl; M. Markytan; J. Mittendorfer; M. Bardadin-Otwinowska; A. Jacholkowska; M. Szczekowski
AbstractThe inclusive proton diffraction dissociation cross sections in 16, 32, and 110 GeV/cK−p interactions are determined from the spike nearx=1 in the inclusive negative particle spectra and are compared to those obtained inK−p interactions using other selection methods at various energies. The same procedure is applied to events containing aV0 in order to obtain the cross section for diffractive
Nuclear Physics | 1974
P. Bosetti; H. Kirk; R. Schulte; R. Steinberg; U. Gensch; H. Nowak; H.J. Schreiber; H. Vogt; M. Walter; G.J. Bossen; H. Plothow; E. Propach; B.U. Stöcker; T. Besliu; K. Böckmann; P. Duinker; S. Matsumoto; D.R.O. Morrison; H. Schiller; H. Wahl; J. Bartke; J. Łoskiewicz; R. Blaschke; S. Brandt; M. Bardadin-Otwinowska; A. Zieminski
Nuclear Physics | 1973
P. Bosetti; M. Deutschmann; H. Kirk; R. Speth; H.J. Schreiber; H. Vogt; K. Böckmann; M. Rost; U. Stöcker; V.T. Cocconi; U. Gensch; G.T. Jones; D. Kuhn; D.R.O. Morrison; D. Sotiriou; R. Stroynowski; H. Wahl; A. Eskreys; L. Suszycki; T. Hirose; J. Stiewe; M. Bardadin-Otwinowska; T. Hofmokl
s\bar s
European Physical Journal C | 1984
E.G. Boos; A. M. Mosienko; N. A. Pokrovsky; H. Bärwolf; G. Bohm; U. Gensch; P. Kostka; Wolfgang Lohmann; Th. Naumann; H. E. Roloff; Spiering; E. Denes; L. Diosy; T. Gemesy; L. Jenik; J. Krasnovszky; Gy. Pinter; I. Wagner; A.V. Bannikov; J. Bohm; Ya. V. Grishkevich; B. A. Khomenko; N.N. Khovanskij; Z. Krumstein; Yu. P. Merekov; V.I. Petrukhin; K. Safarik; G.A. Shelkov; L. G. Tkachev; L. S. Vertogradov
European Physical Journal C | 1988
H. Bärwolff; C. Dreher; W. Friebel; U. Gensch; H. E. Roloff; H. J. Schreiber; C. Spiering; E. Denes; Lajos Diósi; T. Gemesy; L. Jenik; J. Krasznovsky; Gy. Pinter; I. Wagner; A.V. Bannikov; J. Boehm; Yu. V. Grishkevich; B. A. Khomenko; Z. Krumstein; Yu. P. Merekov; V.I. Petrukhin; K. Safarik; G.A. Shelkov; L. G. Tkachev; L. S. Vertogradov; T. Soukup; A. Valkárová; S. Valkar; P. Zavada; V. G. Kristeva
production. While the total cross section for proton diffraction is found to be approximately constant in the energy range studied here, proton diffraction yielding an
Nuclear Physics | 1969
J. Bartsch; M. Deutschmann; M. Hermanns; E. Keppel; R. Speth; U. Gensch; C. Grote; D. Pose; H. Schiller; M. Bardadin-Otwinowska; V.T. Cocconi; R. Ely; J.D. Hansen; W. Kittel; K.P.C. Lindblom; D.R.O. Morrison; H. Tøfte; N.C. Barford; P.J. Dornan; M.E. Mermikides; M.J. Losty; B. Buschbeck-Czapp; M. Markytan; G. Otter; P. Porth; P. Schmid