D. Koltick
Purdue University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by D. Koltick.
Physics Letters B | 1986
M. Derrick; K. K. Gan; P. Kooijman; J. S. Loos; B. Musgrave; L. E. Price; James Schlereth; K. Sugano; J.M. Weiss; D.E. Wood; D. Blockus; B. Brabson; S.W. Gray; C. Jung; H. A. Neal; H. Ogren; D. R. Rust; M. Valdata-Nappi; C. Akerlof; G. Bonvicini; J. Chapman; D. Errede; N. Harnew; P. Kesten; D.I. Meyer; D. Nitz; A.A. Seidl; R. P. Thun; T. Trinko; M. Willutzky
Abstract The charged particle multiplicity distribution for e+e− annihilations at s = 29 GeV has been measured using the High Resolution Spectrometer at PEP. The multiplicity distribution, expressed as a function of the mean, shows KNO scaling when compared to e+e− data at other energies. Multiplicity distributions for particles selected in different central rapidity spans are presented. All of these are well presented by the Negative binomial distribution. As the rapidity span is narrowed, the distributions become broader and approach a constant value of the parameter k.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994
B. Baumbaugh; J. Erdman; D. Gaskell; Q. Lu; J. Marchant; R. Ruchti; M. Wayne; C. Cooper; J. Hinson; D. Koltick; C.J. Schmitz; E. I. Shibata; M. Chung; S. Margulies; J. Solomon; M. Atac; A. Baumbaugh; A. Bross; J. E. Elias; M. Mishina; R. Chaney; H. Hammack; D.L. Adams; F. Bird; R. Lewis
Abstract Measurements have been made of the performance of scintillating fibers read out with visible light photon counters (VLPCs). The light yields of single-clad and multiclad scintillating fibers have been compared. The experiment consisted of 3 m long scintillating fibers of 830 μm diameter optically coupled to 8 m long waveguide fibers of 965 μm diameter read out with HISTE-IV VLPCs. For the case of multiclad scintillating fiber and waveguide, an average of 6.2 photoelectrons was detected from the far end of the scintillating fiber if the fiber end was unmirrored, and 10.2 photoelectrons if the fiber end was mirrored. With this substantial photoelectron yield, minimum-ionizing tracks can be easily detected in fiber arrays, and excellent performance characteristics are expected for the fiber trackers designed for the D0 experiment at the Fermilab Tevatron Collider and the SDC experiment at the SSC Laboratory.
Physics Letters B | 1993
H. Hayashii; A. Miyamoto; M. Iwasaki; S. Noguchi; N. Fujiwara; T. Abe; K. Abe; I. Adachi; M. Aoki; S. Awa; R. Belusevic; K. Emi; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; B. Howell; N. Iida; H. Ikeda; R. Itoh; H. Iwasaki; R. Kajikawa; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick; I. Levine
Abstract We have investigated the properties of jet production in almost real γγ collisions at √s=58 GeV with the TOPAZ detector at the TRISTAN e+e− collider. The data were analyzed with a jet-clustering method based on a cone algorithm. The jet rate shows evidence for a hard scattering effect of the hadronic constituents of a photon (resolved photon processes). We have also observed a substantial energy flow in the small-angle region, which is additional evidence for resolved photon processes. We present the transverse momentum dependence of the inclusive jet and two-jet cross sections and compare them with different model predictions.
Physics Letters B | 1988
P. Baringer; B.G. Bylsma; R. De Bonte; D. Koltick; E. H. Low; R. L. McIlwain; D. H. Miller; C. R. Ng; E. I. Shibata; S. Abachi; M. Derrick; P. Kooijman; B. Musgrave; L. E. Price; J. Repond; K. Sugano; D. Blockus; B. Brabson; J. M. Brom; C. Jung; H. Ogren; D. R. Rust; A. Snyder; C. Akerlof; J. Chapman; D. Errede; M. T. Ken; D. I. Meyer; H. A. Neal; D. Nitz
Abstract The production of D * and D mesons has been studied in e + e − annihilations at √s = 29GeV. The data, corresponding to an integrated luminosity of 300 pb −1 , were obtained using the HRS detector at PEP. The cross section is measured to be R (D 0 + D + ) = 2.40±0.35 and we determine the electroweak asymmetry to be −9.9 ± 2.7%, which corresponds to an axial vector coupling constant product g e g c = 0.26 ± 0.07.
Physics Letters B | 1985
M. Derrick; K. K. Gan; P. Kooijman; J. S. Loos; B. Musgrave; Lawrence Price; James Schlereth; K. Sugano; J.M. Weiss; D.E. Wood; D. Blockus; B. Brabson; S.W. Gray; C. Jung; H. A. Neal; H. Ogren; D. R. Rust; M. Valdata-Nappi; C. Akerlof; G. Bonvicini; J. Chapman; D. Errede; N. Harnew; P. Kesten; D.I. Meyer; D. Nitz; A.A. Seidl; R. P. Thun; T. Trinko; M. Willutzky
The charged particle multiplicities of the quark and gluon jets in the three-fold symmetric e+e− → qqg events at √s = 29 GeV have been studied using the high resolution spectrometer at PEP. A value of 〈n〉g = 6.7−2.1+1.1±1.0 for gluon jet s with an energy of 9.7−2.0+1.5 GeV is measured. The ratio, 〈n〉g/〈n〉q, is 1.29−0.41+0.21±0.20, which i s significantly lower than the value of 94 naively expected from the ration of the gluon-to-quark color charges.
Physics Letters B | 1995
R. Itoh; M. Yamauchi; A. Yamaguchi; K. Abe; Tomohiro Abe; I. Adachi; K. Adachi; Masato Aoki; S. Awa; K. Emi; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; N. Fujiwara; H. Hayashii; B. Howell; N. Iida; Y. Inoue; H. Iwasaki; M. Iwasaki; K. Kaneyuki; R. Kajikawa; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick
Abstract Inclusive momentum spectra are measured for all charged particles and for each of π ± , K ± , K 0 K 0 , and p p in hadronic events produced via e + e − annihilation at s =58 Gev . The measured spectra are compared with QCD predictions based on the modified leading log approximation (MLLA). The MLLA model reproduces the measured spectra well. The energy dependence of the peak positions of the spectra is studied by comparing the measurements with those at other energies. The energy dependence is also well described by the MLLA model.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992
M. Atac; J. Park; D. Cline; D. Chrisman; M.D. Petroff; F. Bird; H. Fenker; K. Morgan; J. Thomas; B. Baumbaugh; M. Kelly; J. Warchol; R. Ruchti; B. Abbott; R. Davies; D. Koltick
Abstract A fiber tracking system was constructed at UCLA, consisting of four layers of scintillating fiber ribbons coupled to visible light photon counters (VLPCs), and was tested by measuring cosmic ray track. The total legth of the fiber array is 7 m: 4 m of scintillating fiber and 3 m of clear optical fiber, 0.83 mm diameter. An average number of 6 photoelectrons were detected by the VLPCs, 7 m from the cosmic ray interaction point at the end of the fibers. The details of the experimental arragement and the test results are presented.
Physics Letters B | 1989
I. Adachi; H. Aihara; H.B. Dijkstra; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujiwara; N. Fujiwara; H. Hayashii; S. Higashi; B. Howell; N. Iida; A. Imanishi; H. Ikeda; T. Ishii; R. Itoh; H. Iwasaki; S. Iwata; R. Kajikawa; T. Kamae; S. Kato; S. Kawabata; Y. Kayahara; H. Kichimi; T. Kishida; M. Kobayashi; D. Koltick; Shigeru Kuroda
Abstract The TOPAZ detector has accumulated about 11 pb−1 of data in the energy range s =52−57 GeV . Charged supersymmetric particles have been searched for. Assuming the photino to be massless, we place limits on the chargino of m χ GeV , on the scalar muon, tau, and quark of m μ GeV , m τ GeV , and m q GeV . The scalar electron can be excluded up to a mass of ∼ 28 GeV. Other cases are examined.
Physics Letters B | 1994
R. Enomoto; K. Abe; Tomohiro Abe; I. Adachi; Masato Aoki; S. Awa; R. Belusevic; K. Emi; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; N. Fujiwara; H. Hayashii; B. Howell; N. Iida; H. Ikeda; R. Itoh; H. Iwasaki; M. Iwasaki; R. Kajikawa; K. Kaneyuki; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick; I. Levine; S. Minami
Abstract The differential cross section of dσ(e + e − → e + e − D ∗± X) dP T was measured using a soft-pion analysis D ∗± → π s ± D 0 (D 0 ) at TRISTAN. The average s was 58.7 GeV and the integrated luminosity used in this analysis was 198 pb − , respectively.
Physics Letters B | 1987
M. Derrick; P. Kooijman; J. S. Loos; B. Musgrave; L. E. Price; J. Repond; K. Sugano; D. Blockus; B. Brabson; J. M. Brom; C. Jung; H. A. Neal; H. Ogren; D. R. Rust; C. Akerlof; J. Chapman; D. Errede; M. T. Ken; D. Nitz; R. P. Thun; R. Tschirhart; S. Abachi; P. Baringer; B.G. Bylsma; R. DeBonte; D. Koltick; F. J. Loeffler; E. H. Low; R. L. McIlwain; D. H. Miller
Abstract The inclusive production of η mesons in tau lepton decay has been studied using the High Resolution Spectrometer at the PEP e + e - facility. The data sample corresponds to an integrated luminosity of 300 pb −1 and the storage ring was operated at GeV. The η production appeaars to be only compatible with the decay τ + →π + η ν , which violates isospin and G -parity conservation. The branching ratio of 5.1±1.5% explains much of the current discrepancy between the one-prong topological branching ratio and the sum of the individual one-prong modes.