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Featured researches published by K. Read.


Physics Letters B | 1987

Limits on rare exclusive decays of B mesons

P. Avery; D. Besson; T. J. V. Bowcock; R. T. Giles; J. F. Hassard; K. Kinoshita; F. M. Pipkin; Richard Wilson; J. Wolinski; Di Xiao; Thomas R. Gentile; P. Haas; M. Hempstead; T. Jensen; H. Kagan; R. Kass; S. Behrends; Jan M. Guida; Joan A. Guida; F. Morrow; R. Poling; E. H. Thorndike; P. Tipton; M. S. Alam; N. Katayama; I. J. Kim; C. R. Sun; V. Tanikella; D. Bortoletto; A. Chen

Abstract We have set upper limits for rare exclusive decays of B mesons arising from higher order processes in the standard model of electroweak interactions. Such decays may occur via “penguin diagrams” in B decay. We also set an upper limit on a lepton-number-violating decay mode of the neutral B meson.


Physical Review D | 2009

Inclusive cross section and double helicity asymmetry for pi^0 production in

A. Adare; Terry Awes; V. Cianciolo; A. Enokizono; K. Read; D. Silvermyr; Soren Pontoppidan Sorensen; P. W. Stankus; Glenn R Young

The PHENIX experiment presents results from the RHIC 2006 run with polarized p + p collisions at root s = 62.4 GeV, for inclusive pi(0) production at midrapidity. Unpolarized cross section results are measured for transverse momenta p(T) = 0.5 to 7 GeV/c. Next-to-leading order perturbative quantum chromodynamics calculations are compared with the data, and while the calculations are consistent with the measurements, next-to-leading logarithmic corrections improve the agreement. Double helicity asymmetries A(LL) are presented for p(T) = 1 to 4 GeV/c and probe the higher range of Bjorken x of the gluon (x(g)) with better statistical precision than our previous measurements at root s = 200 GeV. These measurements are sensitive to the gluon polarization in the proton for 0.06 < x(g) < 0.4.


Physical Review D | 2011

p^+ p

A. Adare; Terry Awes; V. Cianciolo; Y. V. Efremenko; A. Enokizono; K. Read; D. Silvermyr; Soren Pontoppidan Sorensen; P. W. Stankus

Measurements of double-helicity asymmetries in inclusive hadron production in polarized p+p collisions are sensitive to helicity-dependent parton distribution functions, in particular to the gluon helicity distribution, {Delta}g. This study focuses on the extraction of hte double-helicity asymmetry in {eta} production (p+p{yields}{eta}+X), the {eta} cross section, and the {eta}/{pi}{sup 0} cross section ratio. The cross section and ratio measurements provide essential input for the extraction of fragmentation functions that are needed to acess the helicity-dependent parton distribution functions.


Physical Review C | 2002

collisions at

I. Chemakin; E. P. Hartouni; M. Justice; J. H. Thomas; H. Hiejima; Y. Zhang; Y. H. Shin; Yagmur Torun; B. A. Cole; M. Rosati; A. D. Frawley; K. Read; M. Gilkes; D.R.O. Morrison; N. Maeda; J. H. Kang; S. Gushue; G. Rai; R. A. Soltz; Richard C. Fernow; W. A. Zajc; M.N. Namboodiri; D. Winter; M. Moulson; V. Cianciolo; X. Yang; Harold G. Kirk; S. Mioduszewski; R. L. McGrath; L.P. Remsberg

Differential cross-sections are presented for the inclusive production of charged pions in the momentum range 0.1 to 1.2 GeV/c in interactions of 12.3 and 17.5 GeV/c protons with Be, Cu, and Au targets. The measurements were made by Experiment 910 at the Alternating Gradient Synchrotron in Brookhaven National Laboratory. The cross-sections are presented as a function of pion total momentum and production polar angle


Physics Letters B | 1987

\sqrt{s}=62.4

C. Bebek; K. Berkelman; E. Blucher; D. G. Cassel; T. Copie; R. DeSalvo; J. W. DeWire; R. Ehrlich; R. S. Galik; M. Gilchriese; B. Gittelman; S. W. Gray; A. M. Halling; D. L. Hartill; B. K. Heltsley; S. Holzner; J. Kandaswamy; R. Kowalewski; D. L. Kreinick; Y. Kubota; N. B. Mistry; J. Mueller; R. Namjoshi; E. Nordberg; D. Perticone; D. Peterson; M. Pisharody; K. Read; D. Riley; A. Silverman

\theta


Physical Review C | 2009

GeV

A. Adare; Terry Awes; V. Cianciolo; A. Enokizono; K. Read; D. Silvermyr; Soren Pontoppidan Sorensen; P. W. Stankus; Glenn R Young

with respect to the beam.


Physics Letters B | 1987

Cross section and double helicity asymmetry for eta mesons and their comparison to neutral pion production in p+p collisions at sqrt(s)=200 GeV

S. E. Csorna; M. D. Mestayer; R. S. Panvini; G. B. Word; A. Bean; G.J. Bobbink; I. Brock; A. Engler; T. Ferguson; R.W. Kraemer; C. Rippich; H. Vogel; C. Bebek; K. Berkelman; E. Blucher; D. G. Cassel; T. Copie; R. DeSalvo; J. W. DeWire; R. Ehrlich; R. S. Galik; M. Gilchriese; B. Gittelman; S. W. Gray; A. M. Halling; D. L. Hartill; B. K. Heltsley; S. Holzner; M. Ito; J. Kandaswamy

The tau lepton lifetime is measured using four different methods with the DELPHI detector. Three measurements using one prong decays are combined, accounting for correlations, resulting in ττ=298 ±7 (stat.)±4 (syst.) fs while the decay length distribution of three prong decays gives ππ=298±13 (stat)±(syst.) fs. The combined result is ττ=298±7 fs. The ratio of the Fermi coupling constant from tau decay relative to that from muon decay is found to be 0.985±0.013, compatible with lepton universality.


Physical Review C | 2014

Inclusive soft pion production from 12.3-Gev/c and 17.5-GeV/c protons on Be, Cu and Au

Cheuk-Yin Wong; A. Sen; J. Gerhard; Giorgio Torrieri; K. Read

Measurements of the azimuthal anisotropy of high-p(T) neutral pion (pi(0)) production in Au+Au collisions at s(NN)=200 GeV by the PHENIX experiment are presented. The data included in this article were collected during the 2004 Relativistic Heavy Ion Collider running period and represent approximately an order of magnitude increase in the number of analyzed events relative to previously published results. Azimuthal angle distributions of pi(0) mesons detected in the PHENIX electromagnetic calorimeters are measured relative to the reaction plane determined event-by-event using the forward and backward beam-beam counters. Amplitudes of the second Fourier component (v(2)) of the angular distributions are presented as a function of pi(0) transverse momentum (p(T)) for different bins in collision centrality. Measured reaction plane dependent pi(0) yields are used to determine the azimuthal dependence of the pi(0) suppression as a function of p(T), R-AA(Delta phi,p(T)). A jet-quenching motivated geometric analysis is presented that attempts to simultaneously describe the centrality dependence and reaction plane angle dependence of the pi(0) suppression in terms of the path lengths of hypothetical parent partons in the medium. This set of results allows for a detailed examination of the influence of geometry in the collision region and of the interplay between collective flow and jet-quenching effects along the azimuthal axis.


Physical Review C | 2012

A measurement of the tau lifetime

A. Adare; Terry Awes; V. Cianciolo; Y. V. Efremenko; A. Enokizono; K. Read; D. Silvermyr; S. P. Sorensen; P. W. Stankus

Abstract We have measured the lifetimes of the D0, D+ and Ds+ mesons with data from the CLEO detector. We find τD0 = (5.0 ± 0.7 ± 0.4) × 10−13s, τD+ = (11.4 ± 1.6 ± 0.7) × 10−13s and τDs+ = (4.7 ± 2.2 ± 0.5) × 10−13s, giving lifetime ratios τD+/τD0 = 2.3 ± 0.5 and τDs+/τD0 = 0.9 ± 0.5.


Journal of Instrumentation | 2017

High-pT pi^zero Production with Respect to the Reaction Plane in Au+Au Collisions at s_NN) = 200 GeV

Jonatan Adolfsson; A. Ayala Pabon; M. Bregant; C.L. Britton; G. Brulin; Dionísio de Carvalho; V. Chambert; D. D. Chinellato; B. Espagnon; H.D. Hernandez Herrera; T. Ljubicic; Sohail Musa Mahmood; Ulf Mjörnmark; D. Moraes; M. G. Munhoz; G. Noël; A. Oskarsson; L. Österman; A. Pilyar; K. Read; A. Ruette; P. Russo; B.C.S. Sanches; Lucas Compassi Severo; D. Silvermyr; C. Suire; Ganesh Jagannath Tambave; K.M.M. Tun-Lanoë; W.A.M. Van Noije; A. Velure

To help guide our intuition, summarize important features, and point out essential elements, we review the analytical solutions of Landau (1+1)-dimensional hydrodynamics and exhibit the full evolution of the dynamics from the very beginning to subsequent times. Special emphasis is placed on the matching and the interplay between the Khalatnikov solution and the Riemann simple wave solution at the earliest times and in the edge regions at later times.

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