O. I. Dahl
University of California, Berkeley
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Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1991
G.R. Lynch; O. I. Dahl
The width of the angular distribution of the multiple Coulomb scattering of relativistic heavy particles can be described by simple formulas. The familiar one, which uses the number of radiation lengths, is accurate to 34% for all Z and can be accurate to 11% if a logarithmic path length correction is included. A fairly simple representation that does not use the radiation length agrees with the predictions of Moliere scattering to 2%.
Physical Review Letters | 1961
O. I. Dahl; Nahmin Horwitz; Donald H. Miller; Joseph J. Murray; Paul G. White
Author(s): Dahl, Orin I.; Horwitz, Nahmin; Miller, Donald H.; Murray, Joseph J.; White, Paul G.
European Physical Journal C | 1985
H. Aihara; M. Alston-Garnjost; J. A. Bakken; A. Barbaro-Galtieri; A. V. Barnes; B. A. Barnett; H. U. Bengtsson; B. J. Blumenfeld; A. Bross; C. D. Buchanan; O. Chamberlain; C. Y. Chien; A. R. Clark; A. Cordier; O. I. Dahl; C. T. Day; K. A. Derby; Philippe H. Eberhard; D. L. Fancher; H. Fujii; B. Gabioud; J. W. Gary; W. Gorn; N. J. Hadley; J. M. Hauptman; W. Hofmann; J. E. Huth; J. Hylen; T. Kamae; H. S. Kaye
Three currently used fragmentation models are tested by studying the distribution of particles between jet axes in the 3-jet events ofe+e− annihilation, using data collected by the Time Projection Chamber at PEP. These three models — the Lund String model, the Webber Cluster model and an Independent Fragmentation model (IF) — each implement different Lorentz-frame structures for the fragmentation process of quarks and gluons into hadrons. The Lund model provides a good description of the data, while the IF model does not. The Webber model, which is untuned, does not describe the absolute particle densities between jets, but correctly predicts the ratios of those densities, which are less sensitive to the tuning.
European Physical Journal C | 1985
H. Aihara; M. Alston-Garnjost; D. H. Badtke; J. A. Bakken; A. Barbaro-Galtieri; A. V. Barnes; B. A. Barnett; B. J. Blumenfeld; A. Bross; C. D. Buchanan; O. Chamberlain; J. Chiba; C. Y. Chien; A. R. Clark; A. Cordier; O. I. Dahl; C. T. Day; K. A. Derby; Philippe H. Eberhard; D. L. Fancher; H. Fujii; T. Fujii; B. Gabioud; J. W. Gary; W. Gorn; N. J. Hadley; J. M. Hauptman; H. Hilke; W. Hofmann; J. E. Huth
We have measured the inclusive prompt electron cross section over a wide momentum range (P>0.5 GeV/c) with the PEP-4 TPC detector. The semielectronic branching fractions of thec andb quarks are (9.1±0.9 (stat.)±1.3 (syst.))% and (11.0±1.8±1.0)%, respectively. Theb quark fragmentation function peaks at highz with 〈zb〉=0.74±0.05±0.03. The axial couplings to the neutral current areac=2.3±1.4±1.0 for thec quark andab=−2.0±1.9±0.5 for theb quark.
IEEE Transactions on Nuclear Science | 1983
H. Aihara; M. Alston-Garnjost; D. H. Badtke; J. A. Bakken; A. Barbaro-Galtieri; A. V. Barnes; B. A. Barnett; Barry Blumenfeld; A. Bross; C. Buchanan; W. C. Carithers; O. Chamberlain; J. Chiba; C.Y. Chien; Alan R. Clark; O. I. Dahl; C. T. Day; P. Delpierre; K. A. Derby; Philippe H. Eberhard; D. L. Fancher; H. Fujii; Tatsuya Fujii; B. Gabioud; J. W. Gary; W. Gorn; N. J. Hadley; J. M. Hauptman; B. Heck; H. Hilke
The spatial resolution and response of the segmented cathode pads of the PEP-4 TPC have been measured with data taken at 8.5 atmospheres of 80% Argon-20% Methane gas with a 4kG magnetic field. The dependence of the spatial resolution and pad response on drift distance and track-anode crossing angle is presented.
Physics Letters | 1963
Donald H. Miller; Gideon Alexander; O. I. Dahl; Laurence Jacobs; Goerge R. Kalbfleisch; Gerald A. Smith
Author(s): Miller, Donald H.; Alexander, Gideon; Dahl, Orin I.; Jacobs, Laurence; Kalbfleisch, Goerge R.; Smith, Gerald A.
IEEE Transactions on Nuclear Science | 1983
B. Gabioud; H. Aihara; M. Alston-Garnjost; D. H. Badtke; J. A. Bakken; A. Barbaro-Galtieri; A. V. Barnes; B. A. Barnett; Barry Blumenfeld; A. Bross; C. Buchanan; W. C. Carithers; O. Chamberlain; J. Chiba; C.Y. Chien; Alan R. Clark; O. I. Dahl; C. T. Day; P. Delpierre; K. A. Derby; Philippe H. Eberhard; D. L. Fancher; H. Fujii; Tatsuya Fujii; J. W. Gary; W. Gorn; N. J. Hadley; J. M. Hauptman; B. Heck; H. Hilke
We present here some results obtained with the LBL Time Projection Chamber (TPC) regarding the particle identification by the measurement of the ionization losses in the relativistic rise region. This includes the method of calibration using 55Fe sources, the measurement of the resolution using cosmic rays, which shows an equivalent K-¿ separation of 4.8 standard deviations at 3.5 GeV/c, and the preliminary results obtained with multihadronic events from e+e- annihilations.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
H. Aihara; A.A. Arthur; O. I. Dahl; Philippe H. Eberhard; W.R. Edwards; R.L. Fulton; J.M. Haughian; R. J. Madaras; N. A. Roe; D.B. Shuman; A.L. Spadafora; M. L. Stevenson; J.D. Taylor; W. A. Wenzel; Jinghong Chen; C. Cretsinger; G. E. Forden; A. Milder; J. P. Rutherfoord; M. A. Shupe; J. Featherly; B. Gibbard; H. A. Gordon; J. M. Guida; W. Guryn; S. Kahn; S. Protopopescu; D. Cutts; D. Nešić; J. S. Hoftun
Author(s): Aihara, H.; Arthur, A.A.; Dahl, O.I.; Eberhard, P.H.; Edwards, W.R.; Fulton, R.L.; Haughian, J.M.; Madaras, R.J.; Roe, N.A.; Shuman, D.B.; Spadafora, A.L.; Stevenson, M.L.; Taylor, J.D.; Wenzel, W.A.
European Physical Journal C | 1985
H. Aihara; M. Alston-Garnjost; J. A. Bakken; A. Barbaro-Galtieri; A. V. Barnes; B. A. Barnett; H. U. Bengtsson; B. Blumenfeld; A. Bross; C. Buchanan; O. Chamberlain; J. Chiba; C.Y. Chien; A. R. Clark; A. Cordier; O. I. Dahl; C. T. Day; K. A. Derby; Philippe H. Eberhard; D. L. Fancher; H. Fujii; T. Fujii; B. Gabioud; J. W. Gary; W. Gorn; N. J. Hadley; J. M. Hauptman; W. Hofmann; J. E. Huth; J. Hylen
Inclusive production cross sections for photons and π0s ine+e− annihilation at a center of mass energy of 29 GeV have been measured. The π0 production spectrum agrees with a corresponding measurement for π±. The ratio of the π0 inclusive rate to the average for π± is 0.92±0.14. The fractions of the total energy carried by photons and π0s are 0.244±0.016 and 0.217±0.033, respectively. The fraction of total energy carried by all stable hadrons, prompt leptons and photons is determined to be 0.938±0.045, leaving 0.062±0.045 for neutrinos.
Physics Letters B | 1998
B. Abbott; M. Abolins; B. S. Acharya; I. Adam; D. L. Adams; M. Adams; S. Ahn; H. Aihara; G. A. Alves; N. Amos; E. W. Anderson; R. Astur; M. M. Baarmand; A. Baden; V. Balamurali; J. Balderston; B. Baldin; S. Banerjee; J. Bantly; E. Barberis; J. F. Bartlett; K. Bazizi; A. Belyaev; S. B. Beri; I. Bertram; V. A. Bezzubov; P. C. Bhat; V. Bhatnagar; M. Bhattacharjee; N. Biswas
Abstract We have searched for the flavor-changing neutral current decay b → X s μ + μ − in p p collisions at s = 1.8 TeV with the DO detector at Fermilab. We determine the 90% confidence level limit for the branching fraction to be B ( b → X s μ + μ − ) −4 . We argue that this limit is more stringent than the best published limit on this decay rate.We have searched for the flavor-changing neutral current decay b ->s mu+ mu- in p pbar collisions at sqrt(s) = 1.8 TeV with the DO detector at Fermilab. We determine the 90% confidence level limit for the branching fraction to be B(b ->X_s mu+ mu-)<3.2 x 10^{-4}. We argue that this limit is more stringent than the best published limit on this decay rate.