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Featured researches published by J. Litt.


Physics Letters B | 1973

Measurements of the proton--proton total cross section by means of Coulomb scattering at the CERN Intersecting Storage Rings.

U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae; J. Allaby; W. Bartel; M.M. Block; G. Cocconi; A.N. Diddens; R. Dobinson; J. Litt; A.M. Wetherell

Abstract Proton-proton elastic scattering has been measured at the CERN Intersecting Storage Rings in the four-momentum transfer range 0.001 ⩽… t …⩽ 0.015 GeV 2 at centre-of-mass energies of 23 and 31 GeV. The detection of Coulomb scattering and of its interference with nuclear scattering leads to the determination of the real part of the nuclear amplitude and of the total proton-proton cross section by the optical theorem.


Physics Letters B | 1971

Measurements of small angle proton-proton elastic scattering at the CERN intersecting storage rings

U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae; J. Allaby; W. Bartel; G. Cocconi; A.N. Diddens; R. Dobinson; V. Elings; J. Litt; L.S. Rochester; A.M. Wetherell

Abstract Proton-proton elastic scattering has been measured over the angular range 7 to 16 mrad at centre-of-mass energies of 31, 45 and 53 GeV using the CERN Intersecting Storage Rings. The results indicate that the diffraction peak has continued to shrink with increasing energy, but not as fast as suggested by the results at lower energies.


Nuclear Physics | 1973

Proton proton elastic scattering and nucleon resonance production at high-energies

J. Allaby; A.N. Diddens; R. Dobinson; A. Klovning; J. Litt; L.S. Rochester; K. Schlüpmann; A.M. Wetherell; U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae

Abstract Angular distributions of proton-proton elastic scattering have been measured for incident beam momenta of 10.0, 12.0, 14.2 and 24.0 GeV/ c over a range of lab scattering angles from 12 to 152 mrad. This is equivalent to a range of four-momentum transfer squared from about 0.1 to 6.7 GeV 2 at the highest momentum. Nucleon resonance production in the two-body reaction p + p → p + X has been studied at 24.0 GeV/ c incident momentum from 13.5 to 112 mrad by measuring the proton momentum spectra from the elastic peak down to a momentum corresponding to a missing mass of about 2.6 GeV. The new data are compared with previous results and theoretical models.


Nuclear Physics | 1982

Photoproduction of ϱ0 and ω on hydrogen at photon energies of 20 to 70 GeV

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

The reaction γp → pπ+π−π+π− for photon energies from 25 to 70 GeV

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 | 1971

Energy dependence of the structure in high energy proton-proton elastic scattering

J. Allaby; A.N. Diddens; R.W. Robinson; A. Klovning; J. Litt; L.S. Rochester; K. Schlüpmann; A.M. Wetherell; U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae

Abstract The angular distribution of proton-proton elastic scattering has been measured for incident beam momenta of 10.0, 12.0, 14.2 and 24.0 GeV/c over a range of laboratory scattering angles from 12 to about 140 mrad. The results are compared with the fourth power of the electromagnetic form of the proton.


Physics Letters B | 1980

Photoproduction of charmed D mesons at γ energies of 40–70 GeV

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 | 1971

Momentum transfer dependence of nucleon resonance production in proton-proton collisions at 24 GeV/c

U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae; J. Allaby; A.N. Diddens; R.W. Robinson; A. Klovning; J. Litt; L.S. Rochester; K. Schlüpmann; A.M. Wetherell

Abstract Nucleon resonance production in the two-body reaction p + p → p + N ∗ has been studied at 24 GeV/ c incident momentum for angles from 12 to 117 mrad by measuring proton momentum spectra from the elastic peak down to a momentum corresponding to a missing mass of about 2.6 GeV.


Physics Letters B | 1980

Observation of the ϱ′(1600) in the channel γp→π+π−p☆

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 − .


Nuclear Physics | 1975

Momentum spectra of secondary particles produced in proton--proton collisions at 14.2, 19.2, and 24.0 GeV/c

U. Amaldi; R. Biancastelli; C. Bosio; G. Matthiae; J. Allaby; A.N. Diddens; R. Dobinson; A. Klovning; J. Litt; L.S. Rochester; K. Schlüpmann; A.M. Wetherell

Results on charged particle yields in proton-proton collisions at 14.2, 19.2 and 24.0 GeV/c for secondary momenta above 4 GeV/c and lab angles between 10 and 150 mrad are reported. Cross sections for inclusive reactions involving the production of π± K±, p and p are presented. The general features of the dependence of the data on transverse and longitudinal momentum, missing mass, and four-momentum transfer are described and the approach to limiting distributions in the 10 to 30 GeV energy range is discussed.

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