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Featured researches published by A. Chen.


Nuclear Instruments and Methods in Physics Research | 1983

The CLEO detector

D. Andrews; P. Avery; K. Berkelman; R. Cabenda; D. G. Cassel; J. W. DeWire; R. Ehrlich; T. Ferguson; B.G. Gibbard; M. G. D. Gilchriese; B. Gittelman; D. L. Hartill; D. Herrup; M. Herzlinger; J. Kandaswamy; D. L. Kreinick; D. Larson; N. B. Mistry; F. Morrow; E. Nordberg; R. Perchonok; R. Plunkett; K. A. Shinsky; R. H. Siemann; A. Silverman; P. C. Stein; S. Stone; Richard Talman; D. Weber; R. Wilcke

Abstract The construction and performance of a large aperture magnetic detector designed for use at the Cornell Electon Storage Ring is descr bed.


Physics Letters B | 1987

A measurement of the tau lifetime

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

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 D | 1986

Study of the decay BX

M. S. Alam; N. Katayama; I. J. Kim; C. R. Sun; V. Tanikella; A. Bean; G. J. Bobbink; I. Brock; A. Engler; T. Ferguson; R.W. Kraemer; C. Rippich; R.B. Sutton; 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

We have measured the inclusive branching ratio for B..-->..psiX to be (1.09 +- 0.16 +- 0.21)%, and the exclusive branching ratios for B/sup -/..-->..psiK/sup -/ and B-bar /sup 0/..-->..psiK-bar /sup *//sup 0/ to be (0.09 +- 0.05)% and (0.41 +- 0.18)%, respectively. The mass difference between neutral and charged B mesons is 1.1 +- 2.1 MeV, while the difference between the mass of UPSILON(4S) and twice the mean B-meson mass is 18.5 +- 3.0 MeV. The psi momentum distribution implies a substantial two-body decay (in agreement with direct measurements), but also some combination of B..-->..psiX with M/sub X/>1.5 GeV, and B..-->..psiX.


Physical Review Letters | 1982

Measurement of the branching ratio of (3S)+-(1S)

J. Green; F. Sannes; P. Skubic; A. Snyder; R. Stone; A. Chen; M. Goldberg; N. Horwitz; H. Jawahery; M. Jibaly; P. Lipari; G. C. Moneti; H. W. van Hecke; M. S. Alam; S. E. Csorna; A. Fridman; R. G. Hicks; M. D. Mestayer; R. S. Panvini; D. Andrews; P. Avery; R. Cabenda; D. G. Cassel; J. W. DeWire; R. Ehrlich; T. Ferguson; R. S. Galik; M. Gilchriese; B. Gittelman; D. L. Hartill

The branching ratio of UPSILON(3S)..--> pi../sup +/..pi../sup -/UPSILON(1S) has been measured to be (4.9 +- 0.9 +- 0.5)%. The di-pion invariant-mass distribution for this decay is flatter than that for the decays UPSILON(2S)..--> pi../sup +/..pi../sup -/UPSILON(1S) and psi..--> pi../sup +/..pi../sup -/psi.


Physics Letters B | 1983

Ruling out exotic models of b quark decay

A. Chen; M. Goldberg; Nahmin Horwitz; A. Jawahery; M. Jibaly; H. Kooy; P. Lipari; G. C. Moneti; H. W. van Hecke; M. S. Alam; S. E. Csorna; A. Fridman; M. D. Mestayer; R. S. Panvini; D. Andrews; P. Avery; K. Berkelman; D. G. Cassel; J. W. DeWire; R. Ehrlich; T. Ferguson; R. S. Galik; M. G. D. Gilchriese; B. Gittelman; D. L. Hartill; D. Herrup; M. Herzlinger; S. Holzner; M. Ito; J. Kandaswamy

Abstract We consider three broad classes of nonstandard models for b quark decay: (1) b → llq with charged or neutral leptons of arbitrary flavor; (2) b → l q q ; and (3) b → qa − where a − is a Higgs boson or hyperpion. For these classes of models we have calculated the charged energy fraction and the inclusive yields of electrons, muons, protons, and lambdas. We demonstrate that these model predictions are inconsistent with CLEO measurements at the γ (4S).


Physics Letters B | 1987

Measurement of the D0, D+ and Ds+ meson lifetimes at √s = 10.58 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

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.


Physics Letters B | 1984

A search for the ρ(2.2) in the ϒ region

S. Behrends; K. Chadwick; J. Chauveau; T. Gentile; Jan M. Guida; Joan A. Guida; A. C. Melissinos; S. L. Olsen; G. Parkhurst; D. Peterson; R. Poling; C. Rosenfeld; E. H. Thorndike; P. Tipton; D. Besson; J. Green; R. G. Hicks; R. Namjoshi; F. Sannes; P. Skubic; A. Snyder; R. Stone; A. Chen; M. Goldberg; N. Horwitz; A. Jawahery; P. Lipari; G. C. Moneti; C. G. Trahern; H. W. van Hecke

Abstract We have searched in the decays of the ϒ(1S), ϒ(2S) and B mesons for the narrow state, γ, seen by the Mark II group in radiative ψ decay. We find the product branching fractions B[ϒ(1S) → γγ]·B[γ → K+K−], B[ϒ(2S) → γ γ]· B[γ → K+K−] and B[B → γX]·B[γ → K+K−] to be less than 2×10−4, 9×10−5 and 3×10−3, respectively at 90% confidence level. These limits constrain theoretical models if the γ is interpreted as a Higgs boson.


Physical Review Letters | 1986

Observation of the decay BFX

P. Haas; M. Hempstead; T. Jensen; H. Kagan; R. Kass; S. Behrends; T. Gentile; Jan M. Guida; Joan A. Guida; F. Morrow; R. Poling; C. Rosenfeld; E. H. Thorndike; P. Tipton; J. Green; R. Namjoshi; F. Sannes; R. Stone; M. S. Alam; N. Katayama; I. J. Kim; C. R. Sun; V. Tanikella; D. Bortoletto; A. Chen; L. Garren; M. Goldberg; N. Horwitz; A. Jawahery; P. Lubrano

We present evidence for inclusive F-italic-meson production in B-italic-meson decay. The product branching fraction B-italic(B-italic..-->..F-italicX-italic)B-italic(F-italic/sup +/..-->..phi..pi../sup +/) is measured to be 0.0038 +- 0.010. The F-italic momentum spectrum indicates the presence of a large component of two-body final states in the decay B-italic..-->..F-italicX-italic.


Physical Review Letters | 1980

Observation of a fourth upsilon state in e+e- annihilations

D. Andrews; K. Berkelman; R. Cabenda; D. G. Cassel; J. W. DeWire; R. Ehrlich; T. Ferguson; T. Gentile; M. Gilchriese; B. Gittelman; D. L. Hartill; D. Herrup; M. Herzlinger; D. L. Kreinick; N. B. Mistry; E. Nordberg; R. Perchonok; R. Plunkett; K. A. Shinsky; R. H. Siemann; A. Silverman; P. C. Stein; S. Stone; Richard Talman; H. G. Thonemann; D. Weber; C. Bebek; J. Haggerty; J. M. Izen; W. A. Loomis


Physical Review Letters | 1980

Observation of Three Upsilon States

D. Andrews; K. Berkelman; M. Billing; R. Cabenda; D. G. Cassel; J. W. DeWire; R. Ehrlich; T. Ferguson; T. Gentile; B. Gibbard; M. G. D. Gilchriese; B. Gittelman; D. L. Hartill; D. Herrup; M. Herzlinger; D. L. Kreinick; D. Larson; N. B. Mistry; E. Nordberg; S. Peggs; R. Perchonok; R. Plunkett; J. Seeman; K. A. Shinsky; R. H. Siemann; A. Silverman; P. C. Stein; S. Stone; Richard Talman; H. G. Thonemann

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