B.S. Nielsen
CERN
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Featured researches published by B.S. Nielsen.
European Physical Journal C | 1987
T. Åkesson; M. Albrow; S. Almehed; O. Benary; H. Bøggild; O. Botner; H. Breuker; A. A. Carter; J. R. Carter; Y. Choi; W. Cleland; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; G. Damgaard; C. Fabjan; U. Goerlach; K.H. Hansen; V. Hedberg; G. Jarlskog; S. Katsanevas; N. J. Kjaer; R. Kroeger; K. Kulka; D. Lissauer; B. Lörstad; Athanasios Markou; N. A. McCubbin; U. Mjörnmark; R. Møller
AbstractIn a study ofpp collisions atn
Nuclear Physics | 1986
T. Åkesson; M. Albrow; S. Almehed; Richard Batley; O. Benary; H. Bøggild; O. Botner; H. Breuker; V. Burkert; R. Carosi; A. A. Carter; J. R. Carter; P. Cecil; S. U. Chung; W. Cleland; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; P. Dam; G. Damgaard; W.M. Evans; C. Fabjan; P. Frandsen; S. Frankel; W. Frati; M.D. Gibson; U. Goerlach; M. J. Goodrick; K.H. Hansen
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985
T. Åkesson; R. Batley; O. Benary; J.C. Berset; O. Botner; M. Burns; W.E. Cleland; S. Dagan; P. Dam; G. Delavallade; A. Di Ciaccio; G. Di Tore; C. Fabjan; H. Gordon; M. Harris; P Jeffreys; G. Kesseler; J. Lindsay; D. Lissauer; W. Molzon; B.S. Nielsen; L. Olsen; Y. Oren; J. Renaud; L. Rosselet; R. Schindler; I. Stumer; J. van der Lans; E. Vella; Ch.J. Wang
sqrt s = 63
Physics Letters B | 1982
T. P. A. Åkesson; M. Albrow; S. Almehed; Richard Batley; O. Benary; H. Bøggild; O. Botner; H. Brody; V. Burkert; A. Di Ciaccio; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; G. Damgaard; W.M. Evans; C. Fabjan; P. Frandsen; S. Frankel; W. Frati; H. A. Gordon; A. Hallgren; K.H. Hansen; B. Heck; H.J. Hilke; J.E. Hooper; G. Jarlskog; P. W. Jeffreys; T. Jensen; G. Kesseler
Physics Letters B | 1983
T. Åkesson; M. Albrow; S. Almehed; R. Batley; O. Benary; H. Bøggild; O. Botner; H. Breuker; H. Brody; V. Burkert; A. A. Carter; J. R. Carter; P. Cecil; S. U. Chung; W. Cleland; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; Piet Van Dam; G. Damgaard; S. Eidelman; W.M. Evans; C. Fabjan; P. Frandsen; S. Frankel; W. Frati; M.D. Gibson; U. Goerlach; H. A. Gordon
n GeV with more than 29 GeV total transverse energy emitted into 1.8 units of rapidity in the central region, we have extracted a sample of 4-jet events and compared it with models of the two sources of 4-jet production: double bremsstrahlung and double parton scattering. The data cannot be described by bremsstrahlung alone, and we extract the fraction of 4-jet events attributed to double parton scattering for various definitions of the 4-jet sample. We determine the double parton scattering/2-jet yield ratio, and this leads to a determination of the proton radius. We discuss the implications of our observations for the general understanding of high-ΣET events.
Physics Letters B | 1982
T. P. A. Åkesson; M. Albrow; S. Almehed; Richard Batley; O. Benary; H. Bøggild; O. Botner; H. Brody; V. Burkert; A. Di Ciaccio; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; G. Damgaard; W.M. Evans; C. Fabjan; P. Frandsen; S. Frankel; W. Frati; H. A. Gordon; A. Hallgren; K.H. Hansen; B. Heck; H.J. Hilke; J.E. Hooper; G. Jarlskog; P. W. Jeffreys; T. Jensen; G. Kesseler
We present results from a study of centrally produced mesons in 3 × 106 events with two small-angle protons at the CERN Intersecting Storage Rings. A high-statistics sample of exclusive pp → ppπ+π− events at √s = 63 GeV has been obtained, where the reaction mechanism is dominated by double pomeron exchange. Scalar or tensor glueballs may be produced by this process. The π+π− mass spectrum has a distinctive structure, and analysis shows that the data are dominantly S-wave up to 1600 MeV. The behaviour of the D-wave provides evidence for a 2++ resonance (M = 1480 ± 50 MeV, Γ = 150 ± 50 MeV) in addition to the f(1270). We also show data on exclusive K+K−, pp, and π+π−π+π− production, and on the analogous reaction αα → ααπ+π− at √s = 126 GeV. Flavour independence is suggested by the observation of approximately equal numbers of K+K− and π+π− pairs for mass above 1 GeV. The mass spectra are also apparently independent of √s (45, 63, 126 GeV) and incident particle type (p, α).
Physics Letters B | 1983
T. Åkesson; M. Albrow; S. Almehed; Richard Batley; O. Benary; O. Botner; H. Bøggild; H. Breuker; H. Brody; V. Burkert; R. Carosi; A. A. Carter; J. R. Carter; P. Cecil; W. Cleland; S. U. Chung; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; P. Dam; G. Damgaard; S. Eidelman; W.M. Evans; C.W. Fabjan; P. Frandsen; S. Frankel; W. Frati; M.D. Gibson; U. Goerlach
Abstract We present results obtained with a uranium/copper scintillator fine-sampling calorimeter with wavelength shifter readout. Test beam measurements made with e±, π± and protons in the momentum range 0.3–40 GeV/c are presented. The calorimeter achieves energy resolutions of σ(E) E = 0.36 √E and 0.16 √E for hadrons and electrons, respectively. The measured ratio of response for electrons to that for hadrons is 1.11, for energies of 2 GeV or more. The spatial resolution achieved for single particles at normal incidence is ∼1 cm for electromagnetic showers and ∼3 cm for hadronic showers. Operational experience over three years of running at the CERN ISR, including operation at very high luminosities (∼1.4×1032 cm−2 s−1) is described.
Nuclear Physics | 1982
T. P. A. Åkesson; M. Albrow; S. Almehed; O. Benary; H. Bøggild; O. Botner; H. Brody; V. Burkert; A. Di Ciaccio; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; P. Dam; G. Damgaard; W.M. Evans; C. Fabjan; T. Ferbel; P. Frandsen; S. Frankel; W. Frati; M.D. Gibson; H. A. Gordon; A. Hallgren; K.H. Hansen; B. Heck; S. Henning; J.W. Hiddleston; H.J. Hilke; R.W. Hogue
We present data obtained from a 1.7 sr hadron calorimeter, triggered on transverse energy, in pp collisions at s=63 GeV at the CERN-ISR. From the change in the distribution of energy in the calorimeter, we extract the cross section for two-constituent hard scattering for pT between 6 and 14 GeV at y = 0. The decrease of this jet cross section over this pT range is consistent with exp (−bpT), with b = (1.02 ± 0.09) GeV−1. The slope and normalization of the cross section agree well with a QCD motivated Monte Carlo model. The ratio between jet and single particle cross sections [dσJET/dpT)/(dσπ0/dpT)]| y = 0 changes from about 200 at 6 GeV to about 1500 at 14 GeV.
Nuclear Physics | 1984
T. Åkesson; M. Albrow; S. Almehed; E. Anassontzis; Richard Batley; O. Benary; H. Bøggild; O. Botner; H. Breuker; H. Brody; V. Burkert; B. Callen; R. Carosi; A. A. Carter; J. R. Carter; P. Cecil; W. Cleland; D. J. A. Cockerill; S. Dagan; E. Dahl-Jensen; I. Dahl-Jensen; P. Dam; G. Damgaard; W.M. Evans; C. Fabjan; T. Ferbel; P. Frandsen; S. Frankel; W. Frati; M.D. Gibson
Abstract Bose-Einstein correlations between pions produced in the central region of rapidity in αα, pp and p p interactions have been studied at the ISR. The parameters r and τ c -often interpreted as the radius and depth of the π-emitting region - are found to be independent of incident particle type but to depend on the mean charged multiplicity. In high multiplicity events, the pions appear to originate from a larger space-time region.
Physics Letters B | 1982
T. P. A. Åkesson; J.E. Hooper; C. L. Woody; S. Almehed; A. Nilsson; E. Rosso; U. Mjörnmark; O. Botner; W. Frati; I. Dahl-Jensen; G. Damgaard; G. Jarlskog; R.H. Schindler; B.S. Nielsen; W.M. Evans; R. Batley; R. Møller; H.J. Hilke; P. Frandsen; K.H. Hansen; M. Wood; A. Hallgren; B. Lörstad; Gibson; E. Dahl-Jensen; L.H. Olsen; B. Heck; W. Molzon; D. Lissauer; N. A. McCubbin
Abstract The detailed shape of events triggered by a 1.7 sr hadron calorimeter is studied using charged track information in the Axial Field Spectrometer at the CERN ISR. With increasing transverse energy (ET) a large fraction of the events are seen to have a limited transverse momentum relative to the trigger direction. A comparison of the circularity of the events with a prediction of a QCD-motivated Monte Carlo model shows that at high ET the events originate predominantly from two-constituent scattering.