R. Lestienne
École Polytechnique
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by R. Lestienne.
Nuclear Physics | 1973
R. Barloutaud; A. C. Borg; F. Brun; D. Denegri; C. Louedec; F. Pierre; M. Spiro; B. Drevillon; B. Chaurand; G. Labrosse; R. Lestienne; D. Linglin; R. Salmeron; T. P. Shah; K. Paler; R.J. Miller; J.J. Phelan
We have studied the Kππ system in the 14.3 GeV/c reactions K−p → K−π+π−p, K−p → K0π−π0 and K−p → K0π+π−n. The data have been obtained from a 500 000 picture exposure of the CERN 2m HBC. The first two final states are dominated by Q-production in the Kππ system; there is also an L-signal at M (Kππ) ∼ 1.75 GeV. The reaction cross sections are compared to K−p data at other energies. We discuss the Kππ mass dependence of the diffractive production slope. Evidence is presented for a Q−p versus Q+p differential cross section cross-over around |t| = 0.17 GeV2. A t-channel isospin analysis for the KN → K∗(890)πN channels in the Q-region shows that the I = 1 exchange amplitude is ⋍ 10% of the dominant I = 0 exchange amplitude. The Kππ decay distributions indicate a predominant JP = 1+ state in the Q-region, and an important JP = 2− contribution in the L-region. We find neither s-channel nor t-channel helicity conservation at the meson vertex in the Q- or L-regions. The Kπ angular correlation moments within the Kππ diffractive system are characteristic of Kπ elastic scattering, suggesting a π-exchange Deck-type production mechanism. There is evidence for a Kf0 and κπ contribution (where κ is the JP(Kπ) = 0+ state) to the diffractive Kππ system. A fit to the K−π+π− and K0π−π0 Dalitz-plot distributions for the Q-re gion indicates that the ratio of Kϱ to K∗π decay amplitudes decreases with increasing Kππ mass.
Nuclear Physics | 1973
D. Linglin; B. Chaurand; B. Drevillon; G. Labrosse; R. Lestienne; R. Salmeron; R.J. Miller; K. Paler; J.J. Phelan; T. P. Shah; R. Barloutaud; A. C. Borg; C. Louedec; F. Pierre; M. Spiro
Results are presented on a measurement of the I = 3/2 Kπ elastic scattering cross section by applying the Chew-Low extrapolation method in the reaction K−p → K−π−Δ++at14.3GeV/c. The magnitude of σ(K−π− → K−π−) is found to be about 3 mb at threshold and slowly falling with energy to about 1.5 mb at 2.8 GeV. The off-mass-shell moments of the differential elastic cross section are given. The absolute value of δ30 is found to be increasing slowly from 0° to 20° between threshold and 1.2 GeV.
Physics Letters B | 1973
K. Paler; T.P. Shah; R.J. Miller; J.J. Phelan; B. Chaurand; B. Drevillon; G. Labrosse; R. Lestienne; D. Linglin; R. Salmeron; R. Barloutaud; A. Borg; C. Louedec; F. Pierre; M. Spiro
Abstract New data from the reactions K − p → Λ + X and K − p → K 0 + K at 14 GeV /c are presented. From an analysis of the distributions of M X 2 within the framework of a triple Regge formalism we obtain the effective Regge trajectories corresponding to ϱ, K or K ∗ and nucleon exchange.
Nuclear Physics | 1974
F. Pierre; M. Barbadin-Otwinowska; R. Barloutaud; A. Borg; Y. Pons; M. Spiro; B. Chaurand; B. Drevillon; J.M. Gago; G. Labrosse; R. Lestienne; R. Salmeron; K. Paler; T.P. Shah; S.N. Tovey
Abstract Results are presented on γ production in K− p interactions at 14.3 GeV/c. The analysis is based on 2 541 fitted e+e− pairs in a hydrogen bubble chamber. The inclusive cross section for γ production is found to be (54.5 ± 1.8) mb. The average number of γs per inelastic event is 2.93 ± 0.12; it exhibits no strong dependence on charged multiplicity. From the PL and PT2 invariant distributions of the γ, a simple function describing the π° invariant distribution is determined.
Physics Letters B | 1974
K. Paler; T.P. Shah; S.N. Tovey; R.J. Miller; J.J. Phelan; N. M. Cason; P.H. Stuntebeck; N. Biswas; V.P. Kenney; W. D. Shephard; B. Chaurand; B. Drevillon; G. Labrosse; R. Lestienne; R. Salmeron; M. Bardadin-Otwinowska; A. Borg; C. Louedec; Y. Pons; H. Spiro
Abstract A test is made of the factorisation scheme proposed by Miettinen for the inclusive reaction π±p → Λ + X at 18.5 GeV/c and K−p→ Λ + X at 14.3 GeV/c. The test is applied to the lambda differential cross section and polarisation via a sum rule derived within the concepts of duality and exchange degeneracy, and SU3. The original scheme is found not to agree with the experimental data. A possible explanation of the disagreement is discussed.
Nuclear Physics | 1977
Y. Pons; D. Denegri; J.M. Laffaille; M. Spiro; B. Chaurand; G. Labrosse; R. Lestienne; K. Paler; C. Comber; S.N. Tovey
We discuss the structure of the momentum transfer distributions for the diffractive dissociation processes p → nπ+, p → Δ++π− and K− → K890∗0π−. In the near-threshold mass region a clear break of slope is found around t′KK ∼ 0.25 GeV2 for the two baryonic channels, whereas no comparable structure is seen for the mesonic system. The K → K∗π differential cross section exhibits a nearly exponential behaviour up to t′pp ∼ 0.6 GeV2, falling over three orders of magnitude. The slope variations and breaks are strongly correlated both to the mass region considered and to the decay angle of the fragmentation system.
Nuclear Physics | 1974
M. Bardadin-Otwinowska; R. Barloutaud; A. Borg; D. Denegri; F. Pierre; M. Spiro; B. Chaurand; B. Drevillon; G. Labrosse; R. Lestienne; D. Linglin; R. Salmeron; R.J. Miller; K. Paler; J.J. Phelan; T.P. Shah; S.N. Tovey
The reaction K−p→Δ++ + anything was studied at 14.3 GeV/c and is production mechanism was found to be consistent with one pion exchange at low momentum transfer. K−π− inelastic and total cross sections have been determined by a Chew-Low extrapolation method in the c.m. energy range from threshold to 2.8 GeV. Cross sections for various K−π− final states are presented.
Nuclear Physics | 1972
M. Deutschmann; M. Matziolis; P. Schmitz; K. Lanius; Ch. Spiering; H. Vogt; G.J. Bossen; M. Rost; B.U. Stöcker; W. Kittel; R. Stroynowski; J. Bartke; R. M. Lebedev; I.S. Saitov; S. Brandt; R. Lestienne; P. Daronian; R. Sosnowski; M. Szeptycka; W. Wójcik; A. Wróblewski
Abstract The reaction πp → p5π has been studied in six-prong events of π+p interactions at 5, 8 and 16 GeV/c and of π−p interactions at 5, 11 and 16 GeV/c, using the longitudinal phase space (LPS) technique. The energy dependence of cross sections in LPS sectors was found to depend on the charge and the baryon number “exchanged” between the primary pion and the group of forward-going secondary particles. Selection of certain LPS sectors greatly improves the separation of resonances from background. A strong correlation has been observed between fast forward beam-like pions and protons slow in the c.m.s. A simple interpretation of this observation is discussed.
Nuclear Physics | 1976
A. Borg; M. Bardadin-Otwinowska; R. Barloutaud; C. Louedec; F. Pierre; Y. Pons; M. Spiro; J.M. Gago; G. Labrosse; R. Lestienne; R. Salmeron; K. Paler; S.N. Tovey; C. Comber; T.P. Shah
Abstract The inclusive cross sections for π − , π 0 , π + and η production in K − p interactions at 14.3 GeV/ c are calculated. The invariant cross section distributions are presented and compared in the whole phase space for π + and π 0 , and in the backward c.m. region for π − . In the fragmentation regions, the charged pion production is analysed in terms of the triple-Regge model.
Nuclear Physics | 1974
S.N. Tovey; K. Paler; T.P. Shah; R.J. Miller; J.J. Phelan; B. Chaurand; B. Drevillon; J.M. Gago; G. Labrosse; R. Lestienne; R. Salmeron; R. Barloutaud; A. Borg; D. Denegri; F. Pierre; M. Spiro
Abstract We have measured the reaction K − p → pX at 14.3 GeV/ c , in the fragmentation region of the target proton. The differential cross section is studied as a function of momentum transfer and missing mass squared. In the triple-Regge limit, it is consistent with the dominance of a MMP coupling at large t but it is possible that couplings of the type PPP and ππ P also contribute at small | t | values.