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Featured researches published by C. Daum.


Nuclear Physics | 1981

Diffractive Production of Strange Mesons at 63-{GeV}

C. Daum; L. Hertzberger; W. Hoogland; S. Peters; P. Van Deurzen; V. Chabaud; Antonio Gonzalez-Arroyo; B. Hyams; H. Tiecke; P. Weilhammer; A. Dwurazny; G. Polok; M. Rozanska; K. Rybicki; M. Turala; J. Turnau; H. Becker; G. Blanar; M. Cerrada; H. Dietl; J. Gallivan; R. Klanner; E. Lorenz; G. Lütjens; G. Lutz; W. Männer; U. Stierlin; I. Blakey; M. G. Bowler; R. Cashmore

Abstract Nearly 200 000 examples of the diffractive process K − p → K − π − π + p at 63 GeV have been obtained using a two magnet spectrometer equipped with Cerenkov counters for secondary particle identification. In addition some 2000 examples of the process K − p → ω K − p have been obtained. The K ππ data have been subjected to partial-wave analysis. The dominant J P = 1 + system couples to K ∗ π , in both S and D waves, ϱ K, κπ and e K. The data confirm the existence of two J P = 1 + Q mesons and their masses, widths and branching ratios are given. The ifωK data show that the couplings of the Q mesons to ω K are approximately equal to the couplings to ϱ 0 K. The two 1 + nonets expected in the quark model are discussed in the light of this and other recent experiments. There is strong evidence for a broad J P = 0 − resonance at about 1.46 GeV. At higher masses, structure in the J P = 2 − partial waves establishes the existence of at least one J P = 2 − L meson.


Nuclear Physics | 1981

Diffractive production of 3π states at 63 and 94 GeV

C. Daum; M. Glaubman; F. J. Wickens; L. Hertzberger; P. Van Deurzen; W. Männer; G. Blanar; B. Hyams; H. Dietl; C. Damerell; G. Lütjens; I. Blakey; R. Klanner; G. Thompson; A. R. Gillman; G. Polok; W. Spalding; C. Hardwick; B. Alper; U. Stierlin; G. Lutz; R. Cashmore; M. Rozanska; K. Rybicki; A. Dwurazny; H. Becker; W. Hoogland; P. Weilhammer; J. Loken; M. Turala

Diffractive production of the 3π system has been studied at 63 and 94 GeV using a two magnet spectrometer with high, uniform acceptance. The total number of events used in the analysis is ∼600 000. The A2 meson is shown to be diffractively produced. The existence of a resonant component in both the 1+ and 2− enhancements is established and resonance parameters for the corresponding A1 and A3 mesons are given. There are several indications in the data of states which would correspond to radial excitations in the quark model.


Nuclear Physics | 1971

ELASTIC SCATTERING OF POSITIVE KAONS ON POLARIZED PROTONS BETWEEN 0.87 AND 2.74 GeV/c. RESULTS AND PHASE-SHIFT ANALYSIS.

Michael Albrow; S. Andersson; Almehed; B. Bošnjaković; C. Daum; F.C. Erné; Y. Kimura; J.P. Lagnaux; J.C. Sens; F. Udo; F. Wagner

Abstract Polarization and differential cross-section data at 16 momenta between 0.86 and 2.74 GeV/ c are presented. (Preliminary data on some of the momenta have been published earlier.) In an energy-independent phase-shift analysis from threshold up to 2.5 GeV/ c , resonant-like as well as non-resonant solutions are found for the P 3 wave. An helicity flip-non-flip decomposition of the partial waves partly supports the indications found in the analyses of other reactions that the pomeron is built up mainly from s -channel helicity non-flip contributions.


Physics Letters B | 1992

Measurement of the mass and width of the charmed meson D∗+ (2010)

S. Barlag; H. Becker; A. Bożek; T. Böhringer; M. Bosman; V. Castillo; V. Chabaud; C. Damerell; C. Daum; H. Dietl; A. R. Gillman; R. Gilmore; T. Gooch; L. Görlich; P. Gras; Z. Hajduk; E. Higon; D.P. Kelsey; R. Klanner; S. Kwan; B. Lücking; G. Lütjens; G. Lutz; J. Malos; W. Männer; E. Neugebauer; H. Palka; M. Pepé; J. Richardson; K. Rybicki

Abstract Using a high-resolution silicon vertex detector we have observed a very clean signal of 127 D∗+. After a careful study of the experimental resolution of our apparatus we have measured m( D ∗++ )−m( D 0 ) = 145.39±0.06±0.03 MeV . We have also obtained a 90% CL upper limit to γ(D∗+) of 131 keV.


Nuclear Physics | 1981

Inclusive φ-meson production in 93 and 63 GeV hadron interactions

C. Daum; L. Hertzberger; W. Hoogland; R. T. Jongerius; S. Peters; P. Van Deurzen; V. Chabaud; A. Gonzales-Arroyo; B. Hyams; H. Tiecke; P. Weilhammer; A. Dwurazny; G. Polok; M. Rozanska; K. Rybicki; M. Turala; J. Turnau; H. Becker; G. Blanar; M. Cerrada; H. Dietl; J. Gallivan; R. Klanner; E. Lorenz; G. Lütjens; G. Lutz; W. Männer; U. Stierlin; I. Blakey; M. G. Bowler

Abstract The inclusive reactions h+p→φ+X, (h=π±,,K±,p±), are studied for 0⪅xF⪅0.3 and p⊥ ⩽ 1 GeV at 93 and and 63 GeV incident momentum. Differential cross sections dσ/dp⊥2 anddσ/dxF are presented and are compared with predictions of the naive parton model.


Nuclear Physics | 1970

Polarization in elastic proton-proton scattering between 0.86 and 2.74 GeV/c

Michael Albrow; S. Andersson; Almehed; B. Bošnjaković; C. Daum; F.C. Erné; J.P. Lagnaux; J.C. Sens; F. Udo

Abstract Polarization and differential cross section data for elastic proton-proton scattering between 0.86 and 2.74 GeV/ c are presented. A comparison is made with existing phase-shift analyses.


Physics Letters B | 1990

Production of the charmed baryon Λ+c in π−Cu and K−Cu interactions at 230 GeV

S. Barlag; M. Pepé; T. Gooch; F. J. Wickens; E. Neugebauer; L. Görlich; T. Böhringer; W. Männer; C. Damerell; B. Lücking; H. Dietl; G. Lütjens; S.J. Watts; R. Gilmore; Z. Hajduk; T. Zeludziewicz; S. Kwan; H. Tiecke; A. R. Gillman; J. Malos; H.J. Seebrunner; H. Palka; U. Stierlin; G. Lutz; P. Gras; V. Castillo; M. Bosman; H. Becker; G. Waltermann; K. Rybicki

Abstract We present results from the NA32 experiment at CERN on the production characteristics of the charmed baryon Λ + c in 230 GeV π − Cu and K − Cu interactions. A high resolution vertex detector consisting of change-coupled devices and silicon microstrip detectors allowed the selection of a very clean sample of 154 Λ + c → pK − π + (and charge conjugate) decays. Results on differential and integrated cross sections are given.


Physics Letters B | 1987

Measurement of the lifetime of the charmed baryon Λc

S. Barlag; H. Becker; T. Böhringer; M. Bosman; V. Castillo; V. Chabaud; C. Damerell; C. Daum; H. Dietl; A. R. Gillman; R. Gilmore; T. Gooch; L. Görlich; P. Gras; Z. Hajduk; E. Higon; D.P. Kelsey; R. Klanner; S. Kwan; B. Lücking; G. Lütjens; Vera Luth; G. Lutz; J. Malos; W. Männer; E. Neugebauer; H. Palka; M. Pepé; J. Richardson; K. Rybicki

Abstract We present results on a sample of Λc decays obtained in the NA32 experiment in 1985 using charge-coupled devices for vertex reconstruction and a trigger on Λc→pK−π+ (and charge conjugate). We observe a distinct peak at the Λc mass on zero background. The lifetime of the Λc is determined to be (1.4±0.30.5±0.3)x10−13 s based on a sample of 14 events.


Physics Letters B | 1980

Experimental proof of the existence of the A1 meson

C. Daum; L. Hertzberger; W. Hoogland; S. Peters; P. Van Deurzen; V. Chabaud; B. Hyams; H. Tiecke; P. Weilhammer; A. Dwurazny; G. Polok; M. Rozanska; M. Turala; J. Turnau; H. Becker; G. Blanar; M. Cerrada; H. Dietl; J. Gallivan; M. Glaubmann; R. Klanner; E. Lorenz; G. Lütjens; G. Lutz; W. Männer; U. Stierlin; I. Blakey; M. G. Bowler; R. Cashmore; J. Loken

Abstract In partial wave analyses of the ( π − π − π + ) system, substantial shape changes of the 1 + S ( ϱπ ) intensity as a function of t , and relative phase changes of ≈ 90°, provide compelling evidence for a resonant A 1 of mass ≈ 1280 MeV and width ≈ 300 MeV.


European Physical Journal C | 1990

Measurement of various decay modes of charmed particlesD0,D+,D s + andΛ s c

S. Barlag; H. Becker; T. Böhringer; M. Bosman; V. Castillo; V. Chabaud; C. Damerell; C. Daum; H. Dietl; A. R. Gillman; R. Gilmore; T. Gooch; L. Görlich; P. Gras; Z. Hajduk; E. Higon; D.P. Kelsey; R. Klanner; S. Kwan; B. Lücking; G. Lütjens; G. Lutz; J. Malos; W. Männer; E. Neugebauer; H. Palka; M. Pepé; J. Richardson; K. Rybicki; H.J. Seebrunner

In the CERN NA 32 experiment a high-resolution silicon vertex detector and a purely topological approach have been used to investigate various decays of charmed particles. We observe ∼620 fully reconstructed decays ofD0 in 12 channels and determine the branching ratios. For fourD0 decay modes involving a single (unseen) π0 the small and narrowD*+−D0 mass difference is used to measure their branching ratios. We also observe ∼280 fully reconstructedD+ decays in 10 channels, ∼90Ds+ decays in 11 channels as well as 160Λsc and 18 decay channels ofD+. For theDs+, we measure the branching fractions within a subset of 16 three- and five-prong decay channels. For theΛsc, we determine the branching fractions within a sample of 11 three- and five-prong decay channels, nearly all involving a proton.

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Z. Hajduk

Polish Academy of Sciences

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