B.R. Kumar
CERN
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Featured researches published by B.R. Kumar.
Nuclear Physics | 1982
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; H.J. Bautsch; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves
Abstract We present results on photoproduction of ϱ 0 and ω in the reactions γ p→ π + π − p and γ p→ π + π − π 0 p by tagged photons in the energy ranges 20 to 70 GeV and 20 to 45 GeV, respectively. The production of the ϱ 0 shows dominantly the characteristics of a diffractive process with respect to the E γ and t dependence of the cross section and the spin density matrix. The ϱ 0 photoproduction yields on average over the photon energy range a total cross section of σ ( γ p→ ϱ 0 p) = 9.4±0.1 μ b with an additional systematic error of ±1 μ b, and average slope parameters of the t distribution d σ /d t ≈exp(− b | t | + ct 2 ), of b =9.1±0.1 GeV −2 and c = 3.1 ±±0.2 GeV −4 . The shape of the ϱ 0 peak in the π + π − invariant spectra shows a skewing similar to that observed at lower energies. The photoproduction of ω is also consistent with a diffractive process and has a cross section of σ ( γ p→ ω p) = 1.2± 0.1 μ b with an additional systematic error of ±0.2 μ b. The average slope parameters of the t distribution are b =8.3 ± 1.3 GeV −2 and c = 3.4±2.6 GeV −4 .
Nuclear Physics | 1981
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves
Abstract Measurements of the reaction γ p → p π + π − π + π − are presented, in which π + π − π + π − systems with masses up to 3 GeV are produced from fragmentation of the incident photon. The reaction is dominated by production of the large peak of the ϱ′(1600) meson and, at higher masses ≳2 GeV, y production of jet-like 4 π systems. The ϱ′(1600) meson is produced by a predominantly s -channel helicity conserving mechanism. At higher masses there are also indications of ϱπ peaks, of masses 1.3 GeV (the A 2 meson) and 1.75 GeV, produced with a recoiling π meson by a mechanism consistent with the Deck effect.
Physics Letters B | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.-P. Duffy; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; M. Górski
Inclusive D0 photoproduction is observed in Kπ+π− and K+π−π0. Evidence is presented for an associated (CD) production mechanism. Cross section estimates and limits are given for D and D mesons.
Physics Letters B | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; H.J. Bautsch; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; William Galbraith; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves; B. Grossetête; P.G. Hampson
Abstract A dipion enhancement of mass 1.59 GeV and width 0.23 GeV is observed in the channel γp→π + π − p. The spin-parity of the enhancement is consistent with being 1 − .
Physics Letters B | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves; B. Grossetête
Abstract An analysis is presented of the channel γp→π + π − π 0 π 0 p. Evidence is found for an ωπ 0 enhancement of mass ≈1.25 GeV and width ≈0.3 GeV. The enhancement is a mixed spin-parity state with 1 − dominant.
Nuclear Physics | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; D. d'Almagne; G. de Rosny; Bernd Diekmann; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves; B. Grossetête
The reaction γp→K+K−p has been investigated with photons in the energy range of 20<Eγ<36 GeV and with K+K− pairs in the mass range of MK+K−<2.0 GeV. The production of the φ(1019) contributes with a cross section σ(γp → φp) × BR(φ→K+K−) = 240±6 nb with an additional systematic error of ±20 nb. In the higher mass range of 1.05<MK+K−<2.0 GeV the production of K+K− pairs yields a cross section σ(γp→K+K−p) = 160±8 nb with an additional systematic error of +40−30 nb.
Nuclear Physics | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves; B. Grossetête
Measurements of ω and η production in the reaction γp→π+π−π+π−π0p are presented, showihg that the ωπ+π− channel is made up of an enhancement at ∼1.7 GeV of width ∼0.5 GeV, which is consistent with being a 1− state, together with a distribution at higher masses containing higher angular momentum terms. The ηπ+π− final state is produced with a similar cross section and also shows a low-mass enhancement.
Nuclear Physics | 1981
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves
Results are presented on inclusive φ photoproduction for incident energies between 25 and 70 GeV. Distributions in Feynman x, pT and decay angles are presented and interpreted in terms of quark fusion models. We demonstrate a similarity with the corresponding pion-induced reaction and obtain information on the hadronic nature of the photon.
Nuclear Physics | 1980
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves
Abstract We report on diffractive production of 6 π systems with a continuum of masses from 2 to 5 GeV/c 2 in the reaction γ p→ π + π − π + π − π + π - p. The event structure is compared in detail with Monte Carlo studies of p T limited phase space, and with the jets observed in hadronic systems produced by electron-positron annihilation. Strong similarities are found. For this jet-like structure of the 6 π system the axis is consistent with being along the incident photon direction.
Nuclear Physics | 1982
D. Aston; M. Atkinson; R. Bailey; A. H. Ball; B. Bouquet; G.R. Brookes; J. Bröring; P. Bussey; D. Clarke; A.B. Clegg; B. D'Almagne; G. de Rosny; Bernd Diekmann; A. Donnachie; M. Draper; B. Drevillon; I. P. Duerdoth; J.P. Dufey; R.J. Ellison; D. Ezra; P. Feller; A. Ferrer; P.J. Flynn; F. Friese; William Galbraith; R. George; S.D.M. Gill; M. Goldberg; S. Goodman; W. Graves
Abstract Results are presented on the inclusive photoproduction of λ and λ for incident photon energies between 25 and 70 GeV. The slope parameter of the pT2 distribution is found to be 2.83±0.1 GeV−2 for λ and 3.28±0.25 GeV−2 for λ . The xF distributions, measured in the range −0.2 to 0.7, show that while λ are produced centrally, λ production extends to more negative values of xF; the shapes show no energy dependence and are similar to those in pion-induced reactions. The polarization of the produced λ is less than 10%. The results are discussed in terms of vector dominance and quark fusion models.