S. Almehed
Lund University
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Featured researches published by S. Almehed.
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 at
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 and Methods in Physics Research | 1982
H. Gordon; Y. Oren; C. Woody; H. Hofmann; N. A. McCubbin; E. Rosso; U. Mjörnmark; O. Botner; B. Schistad; H.J. Hilke; I. Dahl-Jensen; G. Damgaard; G. Jarlskog; R.H. Schindler; B.S. Nielsen; W. E. M. Evans; G. Kesseler; Rasmus Moller; P. Frandsen; S. Almehed; G. Kantardjian; K.H. Hansen; A. Hallgren; J. Lindsay; B. Lörstad; S.Ø. Nielsen; Gibson; E. Dahl-Jensen; H. Bøggild; P. Dam
\sqrt s = 63
Physics Letters B | 1991
P. Abreu; W. Adam; F. Adami; T. Adye; T. P. A. Åkesson; P. Allen; S. Almehed; F. Alted; B. Åsman; Pierre Astier; A. Augustinus; F. Barao; G. Barbiellini; A. Baroncelli; O. Barring; W. Bartl; M. Baubillier; M. Begalli; I. Belokopytov; P. Beltran; D. Benedic; M. Berggren; D. Bertrand; S. Biagi; F. Bianchi; P. Billoir; D. Bloch; D. Bollini; T. Bolognese; M. Bonapart
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
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 | 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
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 | 1998
P. Abreu; W. Adam; T. Adye; P. Adzic; T Aldeweireld; G. D. Alekseev; R. Alemany; T. Allmendinger; P. P. Allport; S. Almehed; U. Amaldi; S. Amato; E. Anassontzis; A. Andreazza; S. Andringa; P. Antilogus; W.D. Apel; Y. Arnoud; B. Åsman; J.-E. Augustin; A. Augustinus; Ba
Abstract The axial field spectrometer is being exploited in a wide-ranging programme to study pp and p p -collisions which are characterized by a large transverse momentum. A specially shaped magnet together with an “imaging” drift chamber is used for efficient detection and momentum analysis of high multiplicity events at interaction rates of up to 5 × 106 s. Particle identification is accomplished over 1 sr; an uranium/scintillator hadron calorimeter will cover more than 8 sr in 1982 to provide an unbiased energy measurement.
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
Abstract In four-jet events from e+e− →Z0 →multihadrons one can separate the three principal contributions from the triple-gluon vertex, double gluon-bremsstrahlung and the secondary quark-antiquark production, using the shape of the two-dimensional angular distributions in the generalized Nachtmann-Reiter angle θ NR ∗ and the opening angle of the secondary jets. Thus one can identify directly the contribution from the triple-gluon vertex without comparison with a specific non-QCD model. Applying this new method to events taken with the DELPHI-detector we get for the ratio of the colour factor Nc to the fermionic Casimir operator C F : N c C F = 2.55 ± 0.55 ( stat. ) ± 0.4 ( fragm. + models ) ± 0.2 ( error in bias ) in agreement with the value 2.25 expected in QCD from Nc=3 and C F = 4 3 .
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
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 | 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
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.