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Dive into the research topics where D. Koltick is active.

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Featured researches published by D. Koltick.


Physics Letters B | 1986

Rapidity Dependence of the Charged Particle Multiplicity Distributions in e+ e- Annihilation at 29-GeV

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

Performance of multiclad scintillating and clear waveguide fibers read out with visible light photon counters

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

Measurement of the inclusive cross section of jets in γγ interactions at TRISTAN

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

Production cross section and electroweak asymmetry of D* and D mesons produced in e+e- annihilations at 29 GeV

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

Comparison of charged particle multiplicities in quark and gluon jets produced in e+e- annihilation at 29 GeV

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

Measurement of inclusive particle spectra and test of MLLA prediction in e+e− annihilation at s=58Gev

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

Tracking with scintillating fibers and visible light photon counters

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

Search for SUSY Particles in e+ e- Annihilation at Tristan

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

Measurement of the D ± Cross Section using a Soft-Pion Analysis in Two-Photon Processes

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

Evidence for the decay τ+→π+ηντ

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.

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D. Blockus

Indiana University Bloomington

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C. Akerlof

University of Michigan

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B. Brabson

Indiana University Bloomington

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C. Jung

Indiana University Bloomington

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M. Derrick

Argonne National Laboratory

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B. Musgrave

Argonne National Laboratory

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L. E. Price

Argonne National Laboratory

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J. Chapman

University of Michigan

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