K. O. Bunnell
Stanford University
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Featured researches published by K. O. Bunnell.
Physical Review Letters | 1989
Joan Adler; D.H. Coward; D. E. Dorfan; W. Stockhausen; W. J. Wisniewski; G. Eigen; D. Pitman; R. E. Cassell; D. Wisinski; K. O. Bunnell; A. I. Mincer; Robert F. Mozley; J. D. Richman; K. Einsweiler; A. Li; C. A. Heusch; A. J. Weinstein; I. E. Stockdale; H. J. Willutzki; A. Odian; R. P. Hamilton; B. Tripsas; R. H. Schindler; U. Mallik; T. Browder; C. Simopoulos; C. Gatto; S. A. Plaetzer; J. Drinkard; D. M. Coffman
Measurements of the exclusive branching fractions B(D^0→π^-e^+ν_e) and B(D^0→K^-e^+ν_e), using data collected at the ψ(3770) with the Mark III detector at the SLAC e^+e^- storage ring SPEAR, are used to determine the ratio of the Kobayashi-Maskawa matrix elements │V_(cd)/V_(cs)│^2 =0.057_(-0.015)^(+0.038)±0.005.
Physics Letters B | 1991
D. Coffman; F. DeJongh; G. P. Dubois; G. Eigen; David Hitlin; C. G. Matthews; A. I. Mincer; J. D. Richman; William J. Wisniewski; Y. Zhu; Z. Bai; Mark J. Burchell; D. E. Dorfan; J. Drinkard; C. Gatto; Clemens A. Heusch; William Lockman; R. Partridge; H. F.-W. Sadrozinski; M. Scarlatella; T. Schalk; Abraham Seiden; A. J. Weinstein; S. Weseler; R. Xu; J. S. Brown; B. I. Eisenstein; T. Freese; G. E. Gladding; Jm Izen
Abstract We report a high statistics study of the inclusive decay properties of the charmed D0 and D+ mesons, and the first inclusive study of the charmed Ds+. The data are collected at s =3.77 GeV and s =4.14 GeV with the Mark III detector at the e+e− storage ring SPEAR. For each charmed meson species, the charged-particle multiplicity, the strangeness content of the final state, and the average π0 multiplicity are determined.
Physics Letters B | 1987
Joan Adler; J. J. Becker; G. Blaylock; T. A. Bolton; J. S. Brown; K. O. Bunnell; T. H. Burnett; R. E. Cassell; D. M. Coffman; V. Cook; D.H. Coward; D. E. Dorfan; G. P. Dubois; A. L. Duncan; G. Eigen; K. Einsweiler; B. I. Eisenstein; T. Freese; G. E. Gladding; C. Grab; F. Grancagnolo; R. P. Hamilton; J. Hauser; C. A. Heusch; D. G. Hitlin; J. M. Izen; L. Köpke; A. Li; W. S. Lockman; U. Mallik
Abstract Dalitz plot analyses of four Kππ decays of the D 0 and D + mesons are presented. The relative amounts of K ∗ π, Kϱ and non-resonant Kππ in each decay mode are determined, and isospin amplitudes and phases are derived. These results are compared with predictions from QCD. The K − π + π + mode has a non-uniform, non-resonant contribution; attempts to fit this distribution are described.
Physics Letters B | 1988
Joan Adler; J. J. Becker; G. Blaylock; T. A. Bolton; J. C. Brient; J. S. Brown; K. O. Bunnell; Mark J. Burchell; T. H. Burnett; R. E. Cassell; D. M. Coffman; V. Cook; D.H. Coward; D. E. Dorfan; J. Drinkard; G. P. Dubois; A. L. Duncan; G. Eigen; K. Einsweiler; B. I. Eisenstein; T. Freese; C. Gatto; G. E. Gladding; C. Grab; R. P. Hamilton; J. Hauser; C. A. Heusch; D. G. Hitlin; J. M. Izen; P. C. Kim
We report a new measurement of the D∗ branching ratios, using data obtained with the Mark III detector at the e^+e^− storage ring SPEAR at s=4.14GeV. A fit to the recoil mass squared spectrum of D mesons reconstructed through the decay modes K^−π^+π^+ and K^−π^+ is used to extract the D^(∗+) → γD^+, π^0D^+, π^+D^0 and D^(∗0) → γD^0, π^0D^0 branching ratios.
Physical Review Letters | 1990
Z. Bai; G. Blaylock; T. A. Bolton; T. E. Browder; J. S. Brown; K. O. Bunnell; T. H. Burnett; R. E. Cassell; D. M. Coffman; Cook; F. DeJongh; D. E. Dorfan; J. Drinkard; G. P. Dubois; G. Eigen; K. Einsweiler; B. I. Eisenstein; T. Freese; C. Gatto; G. E. Gladding; J. Hauser; C. A. Heusch; D. G. Hitlin; J. M. Izen; P. Kim; J. Labs; A. Li; W. S. Lockman; U. Mallik; C. G. Matthews
We present a study of the radiative decay J/ψ→γOO in the γK + K − K + K − and γK + K − K S 0 K L 0 final states. A pseudoscalar state is observed in the OO invariant-mass spectrum at 2.22 GeV/c 2 with a width of 150 MeV/c 2 . The product branching ratios are B(J/ψ→γX)B(X→OO)=(3.3±0.8±0.5)×10 −4 for the MeV/c γK + K − K + K − mode and B(J/ψ→γX)B(X→OO)=(2.7±0.6±0.6)×10 −4 for the γK + K − K S 0 K L 0 mode. No evidence for 2 ++ states below 2.4 GeV/c 2 is found in this decay
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1984
D. Bernstein; J. Bernstein; K. O. Bunnell; G. Burgueno; R. E. Cassell; B. Collins; D.H. Coward; K. F. Einsweiler; R.L. Eisele; B. Haber; D. Hutchinson; G. Mazaheri; E. McNerney; L. Moss; R. F. Mozley; A. Odian; J. Roehrig; K. Skarpaas; B. Sukiennicki; W. Toki; Y. Unno; F. Villa; W. Wadley; N. Wermes; D. Wisinski; R. M. Baltrusaitis; G. Belyansky; D. Coffman; R. Cooper; W. Freidler
Abstract This paper describes the design, construction and performance of the Mark III, a new general purpose large solid angle spectrometer at SPEAR, the SLAC 2–8 GeV e+e− storage ring. The detector has been designed for the study of exclusive final states in e+e− annihilation, which requires large solid angle coverage combined with charged particle momentum resolution, particle identification, and photon detection efficiency at low energies.
Physical Review D | 1992
D. M. Coffman; F. DeJongh; G. P. Dubois; G. Eigen; D. G. Hitlin; C. G. Matthews; A. Mincer; J. D. Richman; A. J. Weinstein; William J. Wisniewski; Y. Zhu; T. Bolton; K. O. Bunnell; R. E. Cassell; D.H. Coward; P. C. Kim; J.F. Labs; A. Odian; D. Pitman; R. H. Schindler; W. Toki; S. Wasserbaech; J. J. Drinkard; C. Gatto; C. A. Heusch; W. S. Lockman; M. Scarlatella; H. Sadrozinski; T. Schalk; A. Seiden
We determine the resonant substructure of D -> [...] decays using a five-dimensional maximum likelihood technique to extract the relative fractions and phases of the amplitudes contributing to the [...], [...], and [...] final states. We find that two-body decay modes account for about 75% of these decays. We obtain branching ratios for [...], [...], [...], [...], and [...] decay modes, as well as several three and four-body decay modes. In the case of [...] and [...], we obtain the branching ratios for all three possible isospin combinations, enabling us to extract the isospin 1/2 and 3/2 amplitudes. This allows us to eliminate the ambiguity due to phase shifts between the isospin amplitudes when comparing our results with theoretical models. We find that the isospin 3/2 amplitudes are suppressed relative to the isospin 1/2 amplitudes, confirming that an understanding of the lifetime difference of the D0 and D+ depends on an understanding of two-body hadronic decays. For the [...] decay modes, we obtain detailed information on the polarization of the [...] and [...]. This enables us to obtain information on form-factors for [...] and [...] transitions, within the context of the factorization hypothesis. Comparison of our results on [...] decays with recent results on semileptonic decays allows us to test the factorization hypothesis.
Physics Letters B | 1987
J. J. Becker; G. Blaylock; T. A. Bolton; J. S. Brown; K. O. Bunnell; T. H. Burnett; R. E. Cassell; D. M. Coffman; V. Cook; D.H. Coward; D. E. Dorfan; G. P. Dubois; A. L. Duncan; G. Eigen; K. Einsweiler; B. I. Eisenstein; T. Freese; G. E. Gladding; C. Grab; F. Grancagnolo; R. P. Hamilton; J. Hauser; C. A. Heusch; D. G. Hitlin; J. M. Izen; L. Köpke; A. Li; W. S. Lockman; U. Mallik; C. G. Matthews
Abstract A search for the lepton family number violating decay D 0 → μ e is reported. No signal is observed in a data sample of 9.3 pb −1 collected at the ζ (3770) resonance with the MARK III detector, where 0.18±0.06±0.05 background events are expected. A 90% confidence level upper limit on the branching fraction B (D 0 → μ e) of 1.5 × 10 −4 is obtained.
Physics Letters B | 1978
D.G. Hill; M. Sakitt; G.R. Snape; A.J. Stevens; K. O. Bunnell; Robert F. Mozley; A. Odian; J. Park; D.N. Slone; William P. Swanson; F. Villa; L.C. Wang
Abstract We report results from a Dalitz plot analysis of 17750 K e3 0 candidates obtained in an experiment designed to have high efficiency across the Dalitz plot. Assuming a vector interaction form factor ƒ + (q 2 ) = ƒ + (0) (1 + λ + q 2 /m π 2 ) we obtain λ + = 0.0348 ± 0.0044. Our upper limits for the scalar (ƒ s ) and tensor (ƒ t ) form factors at the 95% confidence level are ƒ s ƒ + (0) and ƒ t ƒ + (0) .
Physics Letters B | 1992
T. Bolton; J. S. Brown; K. O. Bunnell; M. Burchell; T. H. Burnett; R. E. Cassell; D. Coffman; D.H. Coward; F. DeJongh; J. Drinkard; G. P. Dubois; G. Eigen; B.I. Eisentein; T. Freese; C. Gatto; G. E. Gladding; C.A. Heusch; D. G. Hitlin; Jm Izen; P.C. Kim; J.F. Labs; A. Li; William Lockman; U. Mallik; C. G. Matthews; R. Mir; P. Mockett; A. Odian; L. Parrish; D. Pitman
Abstract We present an analysis of J ψ →γf 1 (1285) , f 1 (1285)→ π + π − π + π − , using the Mark III detector at SPEAR, based on 5.8 × 10 6 produced J ψ events. We measure B( J ψ →γf 1 (1285) , f 1 (1285)→ π + π − π + π − )=(4.8±1.3±0.9) × 10 −5 . We obtain a new measurement of the absolute branching ratio of J ψ →γf 1 (1285) . The mixing angle of the f 1 (1285) and the f 1 (1420) in the 1 ++ nonet is determined.