B.K. Park
New Mexico State University
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Featured researches published by B.K. Park.
Nuclear Physics | 1994
D. L. Prout; S. Delucia; E. Sugarbaker; B. Luther; D. Cooper; T.N. Taddeucci; L. Rybarcyk; J. B. McClelland; C.D. Goodman; B.K. Park; J. Rapaport; T. Sams; G. Edwards; C. Glasshauser
Abstract We present ( p , n ) spin observable measurements in the delta region of excitation taken on the targets 2H and 12C at 0° and 795 MeV proton energy. These observables have been used to form the spin-longitudinal and spin-transverse cross sections. Good agreement is found between experiment and theory in the spin-longitudinal channel.
Physical Review C | 1997
M. A. Espy; J. M. O’Donnell; B. Davis; D. Dehnhard; J. L. Langenbrunner; B. Larson; M. Palarczyk; C.M. Riedel; K. Wick; S. Blanchard; G. R. Burleson; W. R. Gibbs; Brian A. Lail; B. Nelson; B.K. Park; Q. Zhao; William Cummings; P. P. J. Delheij; B.K. Jennings; O. Häusser; R. Henderson; D. Thiessen; E. Brash; M. K. Jones; B. Brinkmöller; K. Maeda; F. Merrill; C. L. Morris; S. Penttilä; D. Swenson
Asymmetries A{sub y} for {pi}{sup +} and {pi}{sup {minus}} elastic scattering from polarized {sup 3}He were measured at incident energies passing through the {pi} nucleon P{sub 33}, or {Delta}(1232), resonance. The data were taken at the Clinton P. Anderson Meson Physics Facility using the high-energy pion channel P{sup 3} and a large acceptance spectrometer to detect the scattered pions. The polarized {sup 3}He target, originally developed at TRIUMF, was modified for these experiments by the addition of diode lasers. Completely unexpected negative asymmetries were observed at and below the resonance in {pi}{sup +} scattering near 50{degree}{endash}60{degree}, which cannot be reproduced by multiple scattering theory and Faddeev wave functions. A hybrid model, which adds a {Delta}-neutron spin-spin interaction term to the conventional calculations, provides a good description of the {pi}{sup +} data. For {pi}{sup {minus}} scattering this term predicts a negligible effect on A{sub y} and the data do not show the anomalous A{sub y} seen with {pi}{sup +}. {copyright} {ital 1997} {ital The American Physical Society}
Nuclear Physics | 1994
R. Gilman; E. Brash; G. Edwards; C. Glashausser; M.K. Jones; F.T. Baker; S. Bastea; D.P. Beatty; L. Bimbot; J. Brusoe; J. Chiba; D. Cooper; G. Kumbartzki; C. Mauger; T. Nagae; B.K. Park; D. Prout; R.D. Ransome; M. Rawool-Sullivan; Paul Martin Rutt; B. Storm; E. Sugarbaker; T.N. Taddeucci; J. Zumbro
Abstract Studies of the production of the Δ resonance in hadronic charge exchange reactions show a shift in the Δ peak position. Measurements looking also at the Δ decay products give some evidence for coherent pion production. We have recently completed a new measurement of the 12 C ( p , n ) reaction leading to the Δ resonance, including a higher resolution coincidence measurement of decay πs in the forward direction. We describe the experiment and some aspects of the preliminary analysis.
Physical Review C | 1997
Espy; S. Penttilä; B.K. Park; C. Bennhold; B. Larson; D. Swenson; C. L. Morris; B.K. Jennings; S. Blanchard; W. R. Gibbs; J. L. Langenbrunner; J.M. O'Donnell; M. Palarczyk; Brian A. Lail; P. P. J. Delheij; M. K. Jones; B. Nelson; D. Tupa; K. Wick; S. S. Kamalov; F. Merrill; E. Brash; D. Dehnhard; D. Thiessen; K. Maeda; O. Häusser; G. R. Burleson; William Cummings; R. Henderson; B. Brinkmöller
Asymmetries A{sub y} for {pi}{sup +} and {pi}{sup {minus}} elastic scattering from polarized {sup 3}He were measured at incident energies passing through the {pi} nucleon P{sub 33}, or {Delta}(1232), resonance. The data were taken at the Clinton P. Anderson Meson Physics Facility using the high-energy pion channel P{sup 3} and a large acceptance spectrometer to detect the scattered pions. The polarized {sup 3}He target, originally developed at TRIUMF, was modified for these experiments by the addition of diode lasers. Completely unexpected negative asymmetries were observed at and below the resonance in {pi}{sup +} scattering near 50{degree}{endash}60{degree}, which cannot be reproduced by multiple scattering theory and Faddeev wave functions. A hybrid model, which adds a {Delta}-neutron spin-spin interaction term to the conventional calculations, provides a good description of the {pi}{sup +} data. For {pi}{sup {minus}} scattering this term predicts a negligible effect on A{sub y} and the data do not show the anomalous A{sub y} seen with {pi}{sup +}. {copyright} {ital 1997} {ital The American Physical Society}
Physical Review C | 1997
Espy; J.M. O'Donnell; B. Davis; D. Dehnhard; J. L. Langenbrunner; B. Larson; M. Palarczyk; C.M. Riedel; K. Wick; S. Blanchard; G. R. Burleson; W. R. Gibbs; Brian A. Lail; B. Nelson; B.K. Park; Q. Zhao; William Cummings; P. P. J. Delheij; B.K. Jennings; O. Haeusser; R. Henderson; D. Thiessen; E. Brash; M. K. Jones; B. Brinkmoeller; K. Maeda; F. Merrill; C. L. Morris; S. I. Penttilae; D. Swenson
Asymmetries A{sub y} for {pi}{sup +} and {pi}{sup {minus}} elastic scattering from polarized {sup 3}He were measured at incident energies passing through the {pi} nucleon P{sub 33}, or {Delta}(1232), resonance. The data were taken at the Clinton P. Anderson Meson Physics Facility using the high-energy pion channel P{sup 3} and a large acceptance spectrometer to detect the scattered pions. The polarized {sup 3}He target, originally developed at TRIUMF, was modified for these experiments by the addition of diode lasers. Completely unexpected negative asymmetries were observed at and below the resonance in {pi}{sup +} scattering near 50{degree}{endash}60{degree}, which cannot be reproduced by multiple scattering theory and Faddeev wave functions. A hybrid model, which adds a {Delta}-neutron spin-spin interaction term to the conventional calculations, provides a good description of the {pi}{sup +} data. For {pi}{sup {minus}} scattering this term predicts a negligible effect on A{sub y} and the data do not show the anomalous A{sub y} seen with {pi}{sup +}. {copyright} {ital 1997} {ital The American Physical Society}
The 5th conference on the intersections of particle and nuclear physics | 1995
D. Prout; E. Sugarbaker; S. Delucia; D. Cooper; B. Luther; C.D. Goodman; B.K. Park; J. Rapaport; J. B. McClelland; Lawrence J. Rybarcyk; T.N. Taddeucci; Thomas Sams; G. Edwards; G. Glasshauser
We present (p↘,n↘) spin observable measurements in the quasielastic and quasifree delta region of excitation taken on the targets 2H and 12C at 0° and 795 MeV proton energy. These observables have been used to form the spin–longitudinal (σ⋅q) and spin–transverse (σ×q) cross sections. Good agreement is found between experiment and theory in the spin–longitudinal channel.
Physical Review Letters | 1994
T.N. Taddeucci; B. Luther; L. Rybarcyk; R.C. Byrd; J. B. McClelland; D. L. Prout; S. DeLucia; D. Cooper; D. Marchlenski; E. Sugarbaker; B.K. Park; Thomas Sams; C.D. Goodman; J. Rapaport; M. Ichimura; K. Kawahigashi
Physical Review Letters | 1994
T.N. Taddeucci; B. Luther; L. Rybarcyk; R.C. Byrd; J. B. McClelland; D. L. Prout; S. DeLucia; D. Cooper; D. Marchlenski; E. Sugarbaker; B.K. Park; Thomas Sams; C.D. Goodman; J. Rapaport; M. Ichimura; K. Kawahigashi
Physical Review C | 1995
D. L. Prout; C.D. Zafiratos; T.N. Taddeucci; J. L. Ullmann; R.C. Byrd; T. A. Carey; P. W. Lisowski; J. B. McClelland; L. Rybarcyk; Sailor Wc; Amian W; Braunstein M; David A. Lind; Mercer Dj; Cooper D; S. DeLucia; B. Luther; D. Marchlenski; E. Sugarbaker; J. Rapaport; B.K. Park; Gülmez E; C.A. Whitten; C.D. Goodman; Huang W; D. Ciskowski; William P. Alford
Physical Review C | 1994
L. Wang; X. Yang; J. Rapaport; C.D. Goodman; C.C. Foster; Y. Wang; J. Piekarewicz; E. Sugarbaker; D. Marchlenski; S. de Lucia; B. Luther; L. Rybarcyk; T.N. Taddeucci; B.K. Park