P. Strolin
CERN
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Featured researches published by P. Strolin.
Physics Letters B | 1972
G. Barbiellini; M. Bozzo; P. Darriulat; G. Diambrini Palazzi; G. De Zorzi; A. Fainberg; M.I. Ferrero; M. Holder; A. McFarland; G. Maderni; S. Orito; J. Pilcher; C. Rubbia; A. Santroni; G. Sette; A. Staude; P. Strolin; K. Tittel
Abstract We have investigated the above processes at the CERN Intersecting Storage Rings (ISR). Results show a marked change of the slope parameter b ( t , s ) = (d/d t ) ln (d σ /d t ) around − t ≈ 0.10 GeV 2 . The s − and t − dependence of b ( t , s ) have been observed over the interval 460 GeV 2 s 2 and 0.02 GeV 2 t 2 .
Physics Letters B | 1974
A. Böhm; M. Bozzo; R. Ellis; H. Foeth; M.I. Ferrero; G. Maderni; B. Naroska; C. Rubbia; G. Sette; A. Staude; P. Strolin; G. De Zorzi
Abstract We have investigated the pp elastic scattering at the CERN Intersecting Storage Rings (ISR). We report results for centre-of-mass scattering angles between 30 and 100 mrad and for centre-of-mass energies of 23.5,30.7, 44.9 and 53 GeV. The elastic differential cross-section shows a diffraction-like shape with a sharp minimum at about t = −1.4 GeV 2 .
Physics Letters B | 1971
M. Holder; E. Radermacher; A. Staude; G. Barbiellini; P. Darriulat; M. Hansroul; S. Orito; P. Palazzi; A. Santroni; P. Strolin; K. Tittel; J. Pilcher; C. Rubbia; G. De Zorzi; M. Macri; G. Sette; C. Grosso-Pilcher; A. Fainberg; G. Maderni
Abstract Small angle elastic scattering events have been observed at the CERN Intersecting Storage Rings. Directions of both particles as well as the collision vertex are reconstructed with the help of four sets of spark chambers, two for each of the two arms. The elastic nature of the events is demonstrated by a collinearity requirement. We find values for the (diffraction) slope parameter in disagreement with the simple linear extrapolation of lower energy (Surpukov) data.
Physics Letters B | 1971
M. Holder; E. Radermacher; A. Staude; G. Barbiellini; P. Darriulat; P. Palazzi; A. Santroni; P. Strolin; K. Tittel; J. Pilcher; C. Rubbia; M. Bozzo; G. De Zorzi; M. Macri; S. Orito; G. Sette; A. Fainberg; C. Grosso-Pilcher; G. Maderni
Abstract This work extends our previous investigations at the CERN Intersecting Storage Rings, with improved statistics at three different energies, wider angular range and a better control over systematic errors. Values for the (diffraction) shape parameter b are given.
Nuclear Physics | 1978
L. Baksay; L. Baum; A. Böhm; A. Derevshikov; G. De Zorzi; H.J. Giesen; H. Hilscher; J. G. Layter; P. McIntyre; F. Muller; B. Naroska; D.D. Reeder; Lucia Rossi; C. Rubbia; H. Rykaczewski; D. Schinzel; G. Sette; A. Staude; P. Strolin; G. Tarnopolsky; V. L. Telegdi; G. Trilling; R. Voss
Measurements of the total cross section have been performed at the ISR with c.m. energies between 23.5 GeV and 62.5 GeV. Two independent experimental methods have been applied, a measurement of total interaction rate and of small angle elastic scattering. Both experiments give consistent results showing that the total cross section increases by (11.8±1.5) % over the ISR energy range. n nThis experiment has also measured the slope of the forward diffraction peak in elastic scattering at small momentum transfer. The elastic cross section shows the same relative rise as the total cross section, and the ratio λ of elastic to total cross section approaches a constant value of λ=0.178±0.003.
Physics Letters B | 1975
R. Webb; G. Trilling; V. Telegdi; P. Strolin; B. C. Shen; P.E. Schlein; J. Rander; B. Naroska; T. O. Meyer; W. Marsh; W. Lockman; J. G. Layter; A. Kernan; M. Hansroul; S.Y. Fung; H. Foeth; R. Ellis; A. Derevshikov; M. Bozzo; A. Böhm; L. Baksay
The single diffraction dissociation process pp → (pπ+π−)p has been studied at the CERN ISR at √s = 45 GeV and 0.1 < −t < 0.6 GeV2. The reaction is dominated by nucleon resonance production: pp → pN (1520) and pp → pN(1688) with cross-sections (0.25 ± 0.08) mb and (0.56 ± 0.19) mb respectively.
Physics Letters B | 1971
M. Holder; E. Radermacher; A. Staude; G. Barbiellini; P. Darriulat; M. Hansroul; S. Orito; P. Palazzi; A. Santroni; P. Strolin; K. Tittel; J. Pilcher; C. Rubbia; G. De Zorzi; M. Macri; G. Sette; C. Grosso-Pilcher; A. Fainberg; G. Maderni
Abstract The absolute luminosity of the CERN Intersecting Storage Rings has been determined by the Van der Meer method. Combining the measurement with small angle proton-proton elastic events, we find σ elastic = (6.8±0.6)mb.
Physics Letters B | 1979
S. Erhan; W. Lockman; M. Medinnis; T. Meyer; J. Rander; P. Schlein; R. Webb; A. Boehm; H. Foeth; A. Staude; R. Ellis; B. Naroska; P. Strolin; J. Zsembery
Abstract Λ 0 s produced in the inclusive reaction pp → Λ° + X with √s = 53 and 62 GeV at the CERN Intersecting Storage Rings are observed to be polarized along the normal to the production plane. In the ranges of longitudinal and transverse momenta, 15–24 and 0.6-1.4 GeV/ c , respectively, the mean polarization is found to be −(0.357±0.055).
Physics Letters B | 1972
M. Holder; E. Radermacher; A. Staude; P. Darriulat; J. Deutsch; M. Hansroul; S. Orito; J E Pilcher; C. Rubbia; P. Strolin; K. Tittel; A. Fainberg; C. Grosso-Pilcher; M. Scire
Abstract The ratio | η oo / η +- | between the parameters η oo = A (K L → π o π o )/ A (K S → π o π o ) and η +- = A (K L → π + π - / A (K S → π + π - )) has been measured. The result | η oo / η +- | = 1.0 ± 0.06 is in good agreement with the pr prediction | η oo | = | η +- | of a number of models, for which the CP violation in the 2π channel is independent of the isospin of the final state.
Physics Letters B | 1972
G. Barbiellini; M. Bozzo; P. Darriulat; G. Diambrini-Palazzi; G. De Zorzi; M. Holder; A. McFarland; G. Maderni; P. Mery; S. Orito; J. Pilcher; C. Rubbia; G. Sette; A. Staude; P. Strolin; K. Tittel
The angular distribution of charged particles emitted between 47° and 90° in the centre of mass has been measured at the CERN Intersecting Storage Rings with a hodoscope of scintillation counters and for centre-of-mass energies Ecm = 30.2, 44.7 and 52.7 GeV. Data are compatible with distributions of the type 1/σinel × dσ/dΩ(θcm) = A(Ecm) sin−2 θcm. The values of A(Ecm) are about a factor of two greater than the predictions of scaling from data at Ecm=6.0 GeV. The shape of the angular distribution provides evidence for a flat distribution in the “rapidity” variable y = artanh(pL/E).