NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Parker Found 19 matches. 1997WI23 Phys.Rev. C56, 3152 (1997) C.F.Williamson, T.C.Yates, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley Quasielastic Electron Scattering from 40Ca NUCLEAR REACTIONS 40Ca(e, e'), E=130-841 MeV; measured σ(θ, E); deduced transverse, longitudinal response functions, agreement with Fermi gas predictions.
doi: 10.1103/PhysRevC.56.3152
1993YA09 Phys.Lett. 312B, 382 (1993) T.C.Yates, C.F.Williamson, W.M.Schmitt, M.Osborn, M.Deady, P.D.Zimmerman, C.C.Blatchley, K.K.Seth, M.Sarmiento, B.Parker, Y.Jin, L.E.Wright, D.S.Onley Longitudinal Response Functions for 40Ca from Quasi-Elastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'X), E=130-480 MeV; measured σ(θ) vs energy transfer; deduced longitudinal response functions.
doi: 10.1016/0370-2693(93)90971-J
1991SE06 Phys.Rev.Lett. 66, 2448 (1991) Evidence for Dineutrons in Extremely Neutron-Rich Nuclei NUCLEAR REACTIONS 6Li(π-, π+), E=220 MeV; 6Li, 9Be(π-, p), E=125 MeV; analyzed data; deduced dineutron evidence.
doi: 10.1103/PhysRevLett.66.2448
1990PA25 Phys.Lett. 251B, 483 (1990) B.Parker, K.K.Seth, R.Soundranayagam Search for Superheavy Hydrogen-6 NUCLEAR REACTIONS 6Li(π-, π+X), E=220 MeV; measured missing mass spectra; deduced no evidence for 6H.
doi: 10.1016/0370-2693(90)90783-3
1989PA20 Phys.Rev.Lett. 63, 1570 (1989) B.Parker, K.K.Seth, C.M.Ginsburg, B.O'Reilly, M.Sarmiento, R.Soundranayagam, S.Trokenheim Search for a T = 2 Dibaryon NUCLEAR REACTIONS 2H(π-, π+), E=291.2 MeV; measured missing mass spectra following breakup; deduced no T=2 dibaryon resonance.
doi: 10.1103/PhysRevLett.63.1570
1989PL05 Phys.Rev. C40, 1861 (1989) M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer 180° Electron Scattering from 14C NUCLEAR REACTIONS 14C(e, e'), E=82-269 MeV; measured σ(E(e'), θ); deduced 14C, 14B Coulomb energy difference. 14C levels deduced structure coefficients, form factors, IAS.
doi: 10.1103/PhysRevC.40.1861
1988HO11 Phys.Rev. C38, 1547 (1988) A.Hotta, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, P.J.Ryan, R.P.Singhal, D.Halderson Electroexcitation of 4He in the Near Continuum NUCLEAR REACTIONS 4He(e, e'), E=130, 200 MeV; measured σ(E(e'), θ(e')). Shell model in continuum interpretation.
doi: 10.1103/PhysRevC.38.1547
1987SE05 Phys.Rev.Lett. 58, 1930 (1987) K.K.Seth, M.Artuso, D.Barlow, S.Iversen, M.Kaletka, H.Nann, B.Parker, R.Soundranayagam Exotic Nucleus Helium-9 and Its Excited States NUCLEAR REACTIONS 9Be(π-, π+), E at 180 MeV/c; measured missing-mass spectrum. 9He deduced mass excess, neutron binding energy, levels. Magnetic spectrometer, tof.
doi: 10.1103/PhysRevLett.58.1930
1986PA20 Phys.Rev. C34, 2354 (1986) B.Parker, R.S.Hicks, A.Hotta, R.L.Huffman, G.A.Peterson, M.A.Plum, P.J.Ryan, R.P.Singhal Transverse Quasielastic Electron Scattering from the Deuteron NUCLEAR REACTIONS 2H(e, e'), E=220, 270, 320 MeV; measured σ(E(e'), θ); deduced isobar configuration role.
doi: 10.1103/PhysRevC.34.2354
1984HO13 Phys.Rev. C30, 87 (1984) A.Hotta, P.J.Ryan, H.Ogino, B.Parker, G.A.Peterson, R.P.Singhal Quasielastic Electron Scattering from 56Fe at 180° NUCLEAR REACTIONS 56Fe(e, e'), E=155-555 MeV; measured σ(θ) vs energy loss, transverse response function; deduced effective mass ratio. Relativistic Fermi gas model.
doi: 10.1103/PhysRevC.30.87
1984HU07 Phys.Lett. 139B, 249 (1984) R.L.Huffman, R.S.Hicks, J.Dubach, B.Parker, M.A.Plum, G.Lahm, R.Neuhausen, J.C.Bergstrom Comparison of Isoscalar and Isovector (e, e') M1 Form Factors at High Momentum Transfer NUCLEAR REACTIONS 14N(e, e), (e, e'), E not given; measured M1 form factors. 14N deduced isoscalar, isovector transition differences. Shell model comparison.
doi: 10.1016/0370-2693(84)91073-6
1984PL02 Phys.Lett. 137B, 15 (1984) M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer Isoscalar and Isovector M4 Spin Transitions in 14C NUCLEAR REACTIONS 14C(e, e'), E=100-300 MeV; measured σ(E(e')), transverse form factor. 14C levels deduced M4 spin transition density isoscalar, isovector amplitudes, σ(π+)/σ(π-). Pion data input.
doi: 10.1016/0370-2693(84)91096-7
1984RY01 Phys.Rev. C29, 655 (1984) P.J.Ryan, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson Transverse Quasielastic Electron Scattering from 12C at 180° NUCLEAR REACTIONS 12C(e, e'), E=150.6 MeV; measured σ(θ, E(e')), transverse quasielastic scattering. 12C deduced resonances. RPA theory comparison.
doi: 10.1103/PhysRevC.29.655
1983SI11 Phys.Rev. C28, 513 (1983) R.P.Singhal, J.Dubach, R.S.Hicks, R.A.Lindgren, B.Parker, G.A.Peterson Electron Scattering at 180° from the ' Single-Hole ' States in 15N NUCLEAR REACTIONS 15N(e, e), (e, e'), E=70-327 MeV; measured σ(E, θ). 15N levels deduced form factors. Shell, core polarization models comparison.
doi: 10.1103/PhysRevC.28.513
1982HI07 Phys.Rev. C26, 339 (1982) R.S.Hicks, J.Dubach, R.A.Lindgren, B.Parker, G.A.Peterson Elastic Magnetic Scattering of Electrons from 13C NUCLEAR REACTIONS 13C(e, e), E=80-338 MeV; measured σ(E, θ). 13C deduced M1 form factor. Shell model.
doi: 10.1103/PhysRevC.26.339
1982HI10 Phys.Rev. C26, 920 (1982) R.S.Hicks, R.L.Huffman, R.A.Lindgren, B.Parker, G.A.Peterson, S.Raman, C.P.Sargent Inelastic Electron Scattering from 208Pb at 180° NUCLEAR REACTIONS 208Pb(e, e'), E=40.5, 50.4, 60.3, 75.2 MeV; measured σ(θ=180°). 208Pb deduced levels, transverse form factors. Enriched target, magnetic spectrometer.
doi: 10.1103/PhysRevC.26.920
1981LI05 Phys.Rev.Lett. 46, 706 (1981) R.A.Lindgren, J.B.Flanz, R.S.Hicks, B.Parker, G.A.Peterson, R.D.Lawson, W.Teeters, C.F.Williamson, S.Kowalski, X.K.Maruyama Comparison of Inelastic Electron Scattering with [g9/2 x (f1/2-3)(J)] (8)- Shell-Model Calculations for the T=1 and T=2, 8-States in 54Fe NUCLEAR REACTIONS 54Fe(e, e'), E=205.1 MeV; measured σ(E(e')), form factors. 54Fe levels deduced J, π, T, γ-multipolarity, B(M8) strength distribution. Shell model calculations.
doi: 10.1103/PhysRevLett.46.706
1981LI19 Phys.Rev.Lett. 47, 1266 (1981) R.A.Lindgren, M.A.Plum, W.J.Gerace, R.S.Hicks, B.Parker, G.A.Peterson, R.Singhal, C.F.Williamson, X.K.Maruyama, F.Petrovich Isospin Splitting of Isovector High-Spin ' Stretched ' Particle-Hole Excitations in Non-Self-Conjugate Nuclei NUCLEAR REACTIONS 60Ni(e, e'), E=205 MeV; measured σ(θ(e), E(e)). 60Ni deduced levels, J, π, T, B(M8), isospin splitting. Lane model parametrization, stretched particle-hole excitations. NUCLEAR STRUCTURE 13C, 15N, 54,56Fe, 58,60Ni; calculated isospin splitting. Lane model parametrization, stretched particle-hole excitation.
doi: 10.1103/PhysRevLett.47.1266
1978FL09 Phys.Rev.Lett. 41, 1642 (1978) J.B.Flanz, R.S.Hicks, R.A.Lindgren, G.A.Peterson, A.Hotta, B.Parker, R.C.York Convection Currents and Spin Magnetization in E2 Transitions of 12C NUCLEAR REACTIONS 12C(e, e'); measured square of electromagnetic form factors; 12C 4.439-MeV level deduced contribution of nuclear convection currents. 12C 16.107-MeV level deduced spin magnetization contributions.
doi: 10.1103/PhysRevLett.41.1642
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