NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = N.S.King Found 73 matches. 2007SO06 Phys.Rev. C 75, 034611 (2007) D.S.Sorenson, J.L.Ullmann, A.Ling, B.K.Park, R.C.Haight, N.S.P.King, R.A.Lindgren, H.Baghaei, E.J.Stephenson, F.P.Brady, J.L.Romero, J.Rapaport, B.L.Clausen, C.Wuest, F.Sammarruca Limitations of the distorted-wave impulse approximation in describing the energy dependence of the 10B(n, p)10Be(g.s.) reaction NUCLEAR REACTIONS 10B(n, p), E=70240 MeV; measured σ(E, θ). Comparison with zero- and finite-range DWIA predictions.
doi: 10.1103/PhysRevC.75.034611
2004OS02 Phys.Rev. C 70, 054613 (2004) J.H.Osborne, F.P.Brady, J.L.Romero, J.L.Ullmann, D.S.Sorenson, A.Ling, N.S.P.King, R.C.Haight, J.Rapaport, R.W.Finlay, E.Bauge, J.P.Delaroche, A.J.Koning Measurement of neutron elastic scattering cross sections for 12C, 40Ca, and 208Pb at energies from 65 to 225 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(n, n), E=65-225 MeV; measured σ(θ). Comparison with model predictions, previous results.
doi: 10.1103/PhysRevC.70.054613
2003MO26 Nucl.Instrum.Methods Phys.Res. B211, 297 (2003) G.L.Morgan, K.R.Alrick, A.Saunders, F.C.Cverna, N.S.P.King, F.E.Merrill, L.S.Waters, A.L.Hanson, G.A.Greene, R.P.Liljestrand, R.T.Thompson, E.A.Henry Total cross sections for the production of 22Na and 24Na in proton-induced reactions on 27Al from 0.40 to 22.4 GeV NUCLEAR REACTIONS 27Al(p, X)22Na/24Na, E=0.4-22.4 GeV; measured production σ. Activation technique, comparison with previous results.
doi: 10.1016/S0168-583X(03)01364-8
1998LO12 Phys.Rev. C57, 3191 (1998) S.A.Long, B.M.Spicer, K.J.Raywood, R.Abegg, W.P.Alford, A.Celler, D.Frekers, P.E.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, N.S.P.King, C.A.Miller, M.A.Moinester, V.C.Officer, G.G.Shute, A.Trudel, M.C.Vetterli, A.I.Yavin, S.Yen Spin-Isovector Giant Resonances Induced by (n, p) Reactions on Heavy Nuclei NUCLEAR REACTIONS 120Sn, 181Ta(n, p), E=298 MeV; 238U(n, p), E=318 MeV; measured σ(Ep, θ). 90Zr, 208Pb(n, p), E=198 MeV; analyzed σ(Ep, θ). 90Y, 120In, 181Hf, 208Tl, 238Pa deduced L=0, 1, 2, 3 giant resonances energy distributions, quasi-free contributions, comparison with sum rules for L=1, 3. Multipole decomposition procedure.
doi: 10.1103/PhysRevC.57.3191
1996FE05 Yad.Fiz. 59, No 9, 1551 (1996); Phys.Atomic Nuclei 59, 1492 (1996) X.Feng, M.H.Holzscheiter, M.Charlton, F.Cverna, T.Ichioka, N.S.P.King, R.A.Lewis, G.L.Morgan, J.Rochet, Y.Yamazaki Ultralow-Energy Antiprotons for Antihydrogen Spectroscopy and Antimatter Gravity
1993PO05 Phys.Rev. C47, 2751 (1993) R.Pourang, J.W.Watson, R.Abegg, M.Ahmad, W.P.Alford, B.D.Anderson, A.R.Baldwin, A.Celler, D.Frekers, O.Hausser, R.Helmer, R.Henderson, K.Hicks, R.Jeppesen, K.P.Jackson, N.S.P.King, R.Madey, C.A.Miller, M.Moinester, M.C.Vetterli, S.Yen High-Spin Stretched States Excited in (n, p) Reactions at 300 MeV NUCLEAR REACTIONS 12C, 28Si, 120Sn(n, p), E=300 MeV; measured spectra, σ(θ). 12B, 28Al, 120In deduced stretched states normalizations. DWIA analysis.
doi: 10.1103/PhysRevC.47.2751
1992SO02 Phys.Rev. C45, R500 (1992) D.S.Sorenson, X.Aslanoglou, F.P.Brady, J.R.Drummond, R.C.Haight, C.R.Howell, N.S.P.King, A.Ling, P.W.Lisowski, B.K.Park, J.Rapaport, J.L.Romero, W.Tornow, J.L.Ullmann Energy Dependence of the Gamow-Teller Strength in p-Shell Nuclei Observed in the (n, p) Reaction NUCLEAR REACTIONS 6Li, 13,12C(n, p), E=60-260 MeV; measured σ(θ, E); deduced unit σ, effective interaction volume integrals.
doi: 10.1103/PhysRevC.45.R500
1991BR10 Phys.Rev. C43, 2284 (1991) F.P.Brady, T.D.Ford, G.A.Needham, J.L.Romero, D.S.Sorenson, C.M.Castaneda, J.L.Drummond, E.L.Hjort, B.McEachern, N.S.P.King, D.J.Millener 12C(n, p)12B Reaction at 56, 60, and 65 MeV NUCLEAR REACTIONS 12C(n, p), E=56, 60, 65 MeV; measured σ(E, θ). 12C(p, p), E=65 MeV; 12C(n, p), E=62, 65 MeV; calculated σ(θ). Microscopic DWBA, shell model analyses. NUCLEAR STRUCTURE 12C, 12B; calculated levels, wave functions, one-body density-matrix elements. Shell model.
doi: 10.1103/PhysRevC.43.2284
1991LI36 Phys.Rev. C44, 2794 (1991) A.Ling, X.Aslanoglou, F.P.Brady, R.W.Finlay, R.C.Haight, C.R.Howell, N.S.P.King, P.W.Lisowski, B.K.Park, J.Rapaport, J.L.Romero, D.S.Sorenson, W.Tornow, J.L.Ullmann Ground-State Gamow-Teller Strength in 64Ni(n, p)64Co Cross Sections at 90-240 MeV NUCLEAR REACTIONS 64Ni(n, p), E=90-240 MeV; measured σ(E, θ); deduced unit σ. DWIA analysis.
doi: 10.1103/PhysRevC.44.2794
1991SA17 Nucl.Phys. A530, 370 (1991) A.L.Sagle, B.E.Bonner, F.P.Brady, N.S.P.King, J.L.Romero 4He(p(pol), d)3He Analyzing Powers and Differential Cross Sections at 32, 40, 50 and 52.5 MeV NUCLEAR REACTIONS 4He(polarized p, d), E=32-52.5 MeV; measured σ(θ), analyzing power vs θ. Legendre polynomial fits.
doi: 10.1016/0375-9474(91)90808-J
1991SA18 Nucl.Phys. A530, 387 (1991) A.L.Sagle, B.E.Bonner, F.P.Brady, N.S.P.King, M.W.McNaughton, J.L.Romero, J.L.Ullmann 3H + d → n(pol) + 4He n(pol) + 4He → 3H + d Measurements and Absolute Neutron-Polarization Determination at 50 MeV NUCLEAR REACTIONS 3H(d, n), E=20-50 MeV; measured absolute neutron polarization. Inverse reaction as analyzer. 4He(polarized n, d), E=50 MeV; measured σ(θ), analyzing power.
doi: 10.1016/0375-9474(91)90809-K
1990RA13 Phys.Rev. C41, 2836 (1990) K.J.Raywood, B.M.Spicer, S.Yen, S.A.Long, M.A.Moinester, R.Abegg, W.P.Alford, A.Celler, T.E.Drake, D.Frekers, P.E.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, J.D.King, N.S.P.King, C.A.Miller, V.C.Officer, R.Schubank, G.G.Shute, M.Vetterli, J.Watson, A.I.Yavin Spin-Flip Isovector Giant Resonances from the 90Zr(n, p)90Y Reaction at 198 MeV NUCLEAR REACTIONS 90Zr(n, p), E=198 MeV; measured σ(Ep, θ); deduced σ(θ). 90Y deduced spin isovector dipole transition strengths.
doi: 10.1103/PhysRevC.41.2836
1989BR17 Phys.Rev. C40, R475 (1989) F.P.Brady, T.D.Ford, J.L.Romero, C.M.Castaneda, J.R.Drummond, E.L.Hjort, N.S.P.King, B.McEachern, D.S.Sorenson, Z.Aung, A.Klein, W.G.Love, J.K.Wambach Gamow-Teller and Spin-Dipole Strength in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(θp, Ep). 90Y deduced Gamow-Teller, spin dipole transition strength.
doi: 10.1103/PhysRevC.40.R475
1989MO19 Phys.Lett. 230B, 41 (1989) M.A.Moinester, A.Trudel, K.Raywood, S.Yen, B.M.Spicer, R.Abegg, W.P.Alford, N.Auerbach, A.Celler, D.Frekers, O.Hausser, R.L.Helmer, R.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, N.S.P.King, S.Long, C.A.Miller, M.Vetterli, J.Watson, A.I.Yavin A Study of Spin Isovector Giant Resonances with the 208Pb(n, p)208Tl Reaction NUCLEAR REACTIONS 208Pb(n, p), E=198, 458 MeV; measured σ(θp, Ep). 208Tl deduced spin isovector giant resonances.
doi: 10.1016/0370-2693(89)91650-X
1989RA09 Phys.Rev. C39, 1929 (1989) J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).
doi: 10.1103/PhysRevC.39.1929
1988HI12 Phys.Rev.Lett. 61, 1174 (1988) K.H.Hicks, R.Abegg, A.Celler, O.Hausser, R.S.Henderson, N.W.Hill, K.P.Jackson, R.G.Jeppesen, N.S.P.King, M.A.Kovash, R.Liljestrand, C.A.Miller, G.L.Morgan, J.R.Shepard, A.Trudel, M.Vetterli, S.Yen Spin-Dependent Observables for the 12C(p, p'γ) Reaction at 400 MeV NUCLEAR REACTIONS 12C(polarized p, p'γ), E=400 MeV; measured σ(θp', θγ), spin dependent observables. 12C level deduced spin-flip probability. Relativistic, nonrelativistic treatments, impulse approximation.
doi: 10.1103/PhysRevLett.61.1174
1988YE01 Phys.Lett. 206B, 597 (1988) S.Yen, B.M.Spicer, M.A.Moinester, K.Raywood, R.Abegg, W.P.Alford, A.Celler, T.E.Drake, D.Frekers, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.Jeppesen, J.D.King, N.S.P.King, K.Lin, S.Long, C.A.Miller, V.C.Officer, R.Schubank, G.G.Shute, M.C.Vetterli, A.I.Yavin Gamow-Teller Strength and Giant Resonances in 90Zr(n, p) at 198 MeV NUCLEAR REACTIONS 90Zr(n, p), E=198 MeV; measured σ(θp, Ep). 90Y deduced giant resonances, Gamow-Teller Strength.
doi: 10.1016/0370-2693(88)90703-4
1987CO17 Phys.Rev. C36, 230 (1987) W.B.Cottingame, K.G.Boyer, W.J.Braithwaite, S.J.Greene, C.J.Harvey, R.J.Joseph, D.B.Holtkamp, C.F.Moore, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, J.R.Shepard, G.R.Smith, R.L.Boudrie, N.S.P.King, C.L.Morris, J.Piffaretti, H.A.Thiessen Inelastic Pion Scattering from 12C NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=100-291 MeV; measured σ(θ); deduced σ. 12C levels deduced isospin mixing effects. DWIA analysis.
doi: 10.1103/PhysRevC.36.230
1987FO10 Phys.Lett. 195B, 311 (1987) T.D.Ford, J.L.Romero, F.P.Brady, C.M.Castaneda, J.R.Drummond, B.McEachern, D.S.Sorenson, Zin Aung, N.S.P.King, A.Klein, W.G.Love Excitation of Isovector Monopole and Quadrupole Giant Resonances in 90Zr(n, p) at 65 MeV NUCLEAR REACTIONS 90Zr(n, p), E=65 MeV; measured σ(E(p), θ(p)), σ(θ(p)). 90Y deduced isovector monopole, quadrupole giant resonances. RPA-DWA analyses.
doi: 10.1016/0370-2693(87)90023-2
1987UL01 Phys.Rev. C35, 1099 (1987) J.L.Ullmann, P.W.F.Alons, B.L.Clausen, J.J.Kraushaar, J.H.Mitchell, R.J.Peterson, R.A.Ristinen, R.L.Boudrie, N.S.P.King, C.L.Morris, J.N.Knudson, E.F.Gibson Pion Scattering to Collective Excitations in 90Zr and 118Sn NUCLEAR REACTIONS 118Sn, 90Zr(π+, π+'), (π-, π-'), E=163 MeV; measured σ(θ). 118Sn, 90Zr levels deduced deformation lengths, GQR, giant monopole sum rule strengths, σ ratios.
doi: 10.1103/PhysRevC.35.1099
1986FI11 Phys.Rev. C34, 619 (1986) D.H.Fitzgerald, H.W.Baer, J.D.Bowman, M.D.Cooper, F.Irom, N.S.P.King, M.J.Leitch, E.Piasetzky, W.J.Briscoe, M.E.Sadler, K.J.Smith, J.N.Knudson Forward-Angle Cross Sections for Pion-Nucleon Charge Exchange between 100 and 150 MeV/c NUCLEAR REACTIONS 1H(π-, π0), E at 100-150 MeV/c; measured σ(θ) vs momentum; deduced σ(θ=0°), s-, p-wave interference minimum parameters, isospin-odd, s-wave scattering length. Partial wave analyses.
doi: 10.1103/PhysRevC.34.619
1986KI12 Phys.Lett. 175B, 279 (1986) N.S.P.King, P.W.Lisowski, G.L.Morgan, P.N.Craig, R.G.Jeppesen, D.A.Lind, J.R.Shepard, J.L.Ullmann, C.D.Zafiratos, C.D.Goodman, C.A.Goulding Observation of Fermi and Gamow-Teller Strength in the 800 MeV (p, n) Reaction NUCLEAR REACTIONS 6Li, 12,13C, 15N(p, n), E=800 MeV; measured σ(θ), σ(θ) vs neutron momentum. 12,13N, 15O, 6Be deduced Gamow-Teller, Fermi transition strengths.
doi: 10.1016/0370-2693(86)90856-7
1985UL01 Phys.Rev. C31, 177 (1985) J.L.Ullmann, J.J.Kraushaar, T.G.Masterson, R.J.Peterson, R.S.Raymond, R.A.Ristinen, N.S.P.King, R.L.Boudrie, C.L.Morris, R.E.Anderson, E.R.Siciliano Pion Inelastic Scattering to Giant Resonances and Low-Lying Collective States in 118Sn and 40Ca NUCLEAR REACTIONS 40Ca, 118Sn(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=135 MeV; measured σ(E(π)), σ(θ). 40Ca, 118Sn deduced giant quadrupole, monopole, low-energy octupole resonance strengths, deformation lengths, sum rule fraction. Isoscalar models.
doi: 10.1103/PhysRevC.31.177
1984BO27 J.Phys.(Paris), Colloq.C4, 351 (1984); See 1984Bo51 J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance
1984BO51 J.Phys.(Paris), Colloq.C-4, 351 (1984) J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π-, π0), E=165 MeV; measured σ(E(π0), θ(π0)), σ(θ(π0)). 40Ca, 60Ni, 90Zr(π+, π0), E not given; measured not abstracted. 40Ca, 60Ni, 90Zr deduced GDR, isovector monopole resonance. RPA, DWIA analyses.
1984BR03 J.Phys.(London) G10, 363 (1984) F.P.Brady, G.A.Needham, J.L.Ullmann, C.M.Castaneda, T.D.Ford, N.S.P.King, J.L.Romero, M.L.Webb, V.R.Brown, C.H.Poppe Excitation of Analogue Isovector Resonances via the (n, p) Reaction at 60 MeV NUCLEAR REACTIONS 6,7Li, 12C, 16O, 28Si, 58,60,62,64Ni, 209Bi(n, p), E=60 MeV; measured σ(θ); deduced effective nucleon-nucleon interaction isovector spin-dependent component, analog isovector resonance excitation mechanism. 28Al deduced Gamow-Teller type transition. 7He deduced L=1 dipole strength contribution. 6He, 12B deduced L=1 strength spin character, Gamow-Teller type transition. 16N deduced L=1 strength spin character.
doi: 10.1088/0305-4616/10/3/011
1984CO04 Phys.Rev.Lett. 52, 1100 (1984) M.D.Cooper, H.W.Baer, R.Bolton, J.D.Bowman, F.Cverna, N.S.P.King, M.Leitch, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano Angular Distribution for 15N(π+, π0)15O(g.s.) at T(π) = 48 MeV NUCLEAR REACTIONS 15N(π+, π0), E=48 MeV; measured σ(θ), σ(E(π0)); deduced optical potential second-order term role. 15O deduced IAS excitation.
doi: 10.1103/PhysRevLett.52.1100
1984UL01 Nucl.Phys. A427, 493 (1984) J.L.Ullmann, F.P.Brady, C.M.Castaneda, D.H.Fitzgerald, G.A.Needham, J.L.Romero, N.S.P.King Analog Giant Dipole Ni(n, p) at 59.6 MeV NUCLEAR REACTIONS 58,60,62,64Ni(n, p), E=59.6 MeV; measured σ(θ). 58,60,62,64Co deduced GDR analog, sum rule, blocking. Enriched targets.
doi: 10.1016/0375-9474(84)90227-6
1983BA13 Nucl.Phys. A396, 437c (1983) H.W.Baer, R.Bolton, J.D.Bowman, M.D.Cooper, F.Cverna, N.S.P.King, M.Leitch, H.S.Matis, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano Study of Isovector Resonances with Pion Charge Exchange NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 120Sn(π+, π0), (π-, π0), E=164 MeV; measured σ(θ), σ(θ, E(π0)). 90Y, 90Nb, 120Sb, 120In deduced isovector monopole, dipole resonances.
doi: 10.1016/0375-9474(83)90037-4
1983BO07 Phys.Rev.Lett. 50, 1195 (1983) J.D.Bowman, H.W.Baer, R.Bolton, M.D.Cooper, F.H.Cverna, N.S.P.King, M.Leitch, H.S.Matis, A.Erell, J.Alster, A.Doron, M.A.Moinester, E.Blackmore, E.R.Siciliano Observation of the Nuclear Isovector Monopole Resonance NUCLEAR REACTIONS 90Zr, 120Sn(π-, π0), (π+, π0), E=165 MeV; measured σ(θ, E(π)). 90Zr deduced GDR, isovector monopole resonance, Γ. 120Sn deduced IAS, GDR, isovector monopole resonance, Γ.
doi: 10.1103/PhysRevLett.50.1195
1983CA19 Phys.Rev. C28, 1493 (1983) C.M.Castaneda, J.L.Ullmann, F.P.Brady, J.L.Romero, N.S.P.King, M.Blann Precompound Analyses of 58-64Ni(n, px) Reactions NUCLEAR REACTIONS 58,60,62,64Ni(n, pX), E=60 MeV; measured σ(θp), σ vs nucleon kinetic energy; deduced neutron number dependence, best fit model. Hybrid, geometry dependent hybrid models, neutron skin effect.
doi: 10.1103/PhysRevC.28.1493
1983UL01 Phys.Rev.Lett. 51, 1038 (1983) J.L.Ullmann, J.J.Kraushaar, T.G.Masterson, R.J.Peterson, R.S.Raymond, R.A.Ristinen, N.S.P.King, R.L.Boudrie, C.L.Morris, W.W.True, R.E.Anderson, E.R.Siciliano Excitation of the Isoscalar Giant Quadrupole Resonance in 118Sn(π±, π±') NUCLEAR REACTIONS 118Sn(π+, π+'), (π-, π-'), E=130 MeV; measured σ(E(π')), σ(θ); deduced σ(π-)/σ(π+). 118Sn deduced GQR excitation neutron, proton asymmetry. DWIA calculations.
doi: 10.1103/PhysRevLett.51.1038
1982BA50 Phys.Rev.Lett. 49, 1376 (1982) H.W.Baer, R.Bolton, J.D.Bowman, M.D.Cooper, F.Cverna, N.S.P.King, M.Leitch, H.S.Matis, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano Observation of Analogs of the Giant-Dipole Resonance in Pion Single Charge Exchange on 40Ca NUCLEAR REACTIONS 40Ca(π+, π0), (π-, π0), E=164 MeV; measured σ(θ, E(π0)); deduced σ(π+)/σ(π-). 40Sc deduced IAS. DWIA, Goldhaber-Teller transition density.
doi: 10.1103/PhysRevLett.49.1376
1982BR04 Phys.Rev.Lett. 48, 860 (1982) F.P.Brady, C.M.Castaneda, G.A.Needham, J.L.Ullmann, J.L.Romero, T.Ford, M.L.Johnson, N.S.P.King, C.M.Morris, F.Petrovich, R.H.Howell Isovector and Gamow-Teller Strength from Small-Angle (n, p) Reactions at 60 MeV NUCLEAR REACTIONS 6Li, 12C, 28Si(n, p), E=60 MeV; measured σ(Ep), σ(θ); deduced effective isovector spin-flip nucleon-nucleon interaction. 6He, 12B, 28Al level deduced Gamow-Teller transition strength.
doi: 10.1103/PhysRevLett.48.860
1982CO01 Phys.Rev. C25, 438 (1982) M.D.Cooper, H.W.Baer, J.D.Bowman, F.H.Cverna, R.H.Heffner, C.M.Hoffman, N.S.P.King, J.Piffaretti, J.Alster, A.Doron, S.Gilad, M.A.Moinester, P.R.Bevington, E.Winkelmann 3He(π-, π0) Reaction at T(π) = 200 MeV NUCLEAR REACTIONS 3He(π-, π0), E=200 MeV; measured σ(θ), σ(θ, E(π0)); deduced σ(total) for IAR excitation, effective nucleon number, Pauli blocking. Glauber model.
doi: 10.1103/PhysRevC.25.438
1982DO02 Phys.Rev.Lett. 48, 989 (1982) A.Doron, J.Alster, A.Erell, S.Gilad, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, P.R.Bevington, E.Winkelmann, C.D.Goodman Energy Dependence of the Small-Angle Differential Cross Sections to Isobaric Analog States in 7Li(π+, π0)7Be and 13C(π+, π0)13N NUCLEAR REACTIONS 7Li, 13C(π+, π0), E=70, 100, 150, 165, 180 MeV; measured σ(θ), σ(E(π0)). 13N, 7Be deduced IAS excitation dependence on pion energy.
doi: 10.1103/PhysRevLett.48.989
1982DO10 Phys.Rev. C26, 189 (1982) A.Doron, J.Alster, A.Erell, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, C.D.Goodman Angular Distributions of Single Pion Charge Exchange Reactions to Isobaric Analog States in Light Nuclei NUCLEAR REACTIONS 13C, 15N(π+, π0), E=164 MeV; measured σ(θ). 13N, 15O deduced IAS excitation. Enriched targets. Semiphenomenological isobar doorway, second-order coupled-channels calculations.
doi: 10.1103/PhysRevC.26.189
1982GI01 Nucl.Phys. A377, 389 (1982) E.F.Gibson, J.J.Kraushaar, T.G.Masterson, R.J.Peterson, R.S.Raymond, R.A.Ristinen, R.L.Boudrie, N.S.P.King Elastic and Inelastic π+ and π- Scattering from 7Li at 143 MeV NUCLEAR REACTIONS 7Li(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=143 MeV; measured σ(θ), σ(Eπ). 7Li deduced neutron, proton radii, deformations. Enriched target.
doi: 10.1016/0375-9474(82)90048-3
1982LI23 Phys.Rev.Lett. 49, 255 (1982) P.W.Lisowski, R.E.Shamu, G.F.Auchampaugh, N.S.P.King, M.S.Moore, G.L.Morgan, T.S.Singleton Search For Resonance Structure In The np Total Cross Section Below 800 Mev NUCLEAR REACTIONS 1H(n, x), E=39-793 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12761.
doi: 10.1103/PhysRevLett.49.255
1982MC05 Phys.Rev. C25, 2107 (1982) M.W.McNaughton, E.P.Chamberlin, J.J.Jarmer, N.S.P.King, H.B.Willard, E.Winkelmann Spin Correlation A(nn) and Analyzing Power A in pp → pp at 643 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=643 MeV; measured analyzing power, spin correlation parameter vs θ. Polarized target.
doi: 10.1103/PhysRevC.25.2107
1982NE04 Nucl.Phys. A385, 349 (1982) G.A.Needham, F.P.Brady, D.H.Fitzgerald, J.L.Romero, J.L.Ullmann, J.W.Watson, C.Zanelli, N.S.P.King, G.R.Satchler Excitation of Analog Isovector Giant Resonances via the (n, p) Reaction on 14N and 16O at 60 MeV NUCLEAR REACTIONS 14N, 16O(n, p), E=60 MeV; measured σ(θ). 14C, 16N deduced GDR analog excitation. Natural targets. DWBA analysis.
doi: 10.1016/0375-9474(82)90092-6
1982RO03 Phys.Rev. C25, 2214 (1982) J.L.Romero, J.L.Ullmann, F.P.Brady, J.D.Carlson, D.H.Fitzgerald, A.L.Sagle, T.S.Subramanian, C.I.Zanelli, N.S.P.King, M.W.McNaughton, B.E.Bonner Neutron-Deuteron Analyzing Power Measurements at 50 MeV. I. Backward Angles NUCLEAR REACTIONS 2H(polarized n, n), E=50 MeV; measured A(θ).
doi: 10.1103/PhysRevC.25.2214
1982SA05 Phys.Rev. C25, 1685 (1982) A.L.Sagle, F.P.Brady, J.L.Romero, B.E.Bonner, N.S.P.King, M.W.McNaughton, H.E.Conzett Time Reversal and Charge Symmetry Studies in Single Nucleon Transfer Reactions in the A = 5 System NUCLEAR REACTIONS 4He(polarized p, d), E=32, 50 MeV; 4He(polarized n, d), E=50 MeV; measured analyzing power vs θ. 3H(d, n), E=37.1 MeV; deduced P(n); deduced time reversal invariance, charge symmetry validity.
doi: 10.1103/PhysRevC.25.1685
1982UL01 Nucl.Phys. A386, 179 (1982) J.L.Ullmann, F.P.Brady, D.H.Fitzgerald, G.A.Needham, J.L.Romero, C.M.Castaneda, N.S.P.King Analog Giant Dipole Excitation in Si(n, p) at 59.6 MeV NUCLEAR REACTIONS 28Si(n, p), E=59.6 MeV; measured σ(θ). 28Al deduced parent analog giant dipole resonance strength. Natural target.
doi: 10.1016/0375-9474(82)90407-9
1981CV01 Phys.Rev. C23, 1698 (1981) F.H.Cverna, P.R.Bevington, M.W.McNaughton, H.B.Willard, N.S.P.King, D.R.Giebink Single and Double Pion Production from 800 MeV Proton-Proton Collisions NUCLEAR REACTIONS 1H(p, π+), (p, π-π+), E=800 MeV; measured σ(θ, pion momentum). Peripheral model analysis, double pion production.
doi: 10.1103/PhysRevC.23.1698
1981MC01 Phys.Rev. C23, 838 (1981) M.W.McNaughton, H.W.Baer, P.R.Bevington, F.H.Cverna, H.B.Willard, E.Winkelmann, E.P.Chamberlin, J.J.Jarmer, N.S.P.King, J.E.Simmons, M.A.Schardt, H.Willmes Spin Correlation Parameter A(nn) in pp Elastic Scattering at 796 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=796 MeV; measured spin correlation parameter vs θ. Polarized target.
doi: 10.1103/PhysRevC.23.838
1981MC04 Phys.Rev. C23, 1128 (1981) M.W.McNaughton, P.R.Bevington, H.B.Willard, E.Winkelmann, E.P.Chamberlin, F.H.Cverna, N.S.P.King, H.Willmes Polarization Analyzing Power A(θ) in pp Elastic Scattering at 796 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=428, 796 MeV; measured analyzing power A(θ). High precision.
doi: 10.1103/PhysRevC.23.1128
1980BA27 Phys.Rev.Lett. 45, 982 (1980) H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, M.B.Johnson, N.S.P.King, J.Piffaretti, E.R.Siciliano, J.Alster, A.Doron, S.Gilad, M.Moinester, P.R.Bevington, E.Winkelmann Observation of Isobaric Analog States in Pion Single-Charge-Exchange Reactions NUCLEAR REACTIONS 7Li, 13C, 27Al, 58Ni, 90Zr, 120Sn, 208Pb(π+, π0), E=98 MeV; measured σ(θ). 7Be, 13N, 27Si, 58Cu, 90Nb, 120Sb, 208Bi deduced IAS. Optical model.
doi: 10.1103/PhysRevLett.45.982
1980KI04 Phys.Rev. C21, 1185 (1980) N.S.P.King, J.D.Reber, J.L.Romero, D.H.Fitzgerald, J.L.Ullmann, T.S.Subramanian, F.P.Brady Neutron-Proton Scattering. I. Differential Cross Section at 63.1 MeV NUCLEAR REACTIONS 1H(n, p), E=63.1 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.21.1185
1980PE01 Phys.Rev. C21, 1030 (1980) R.J.Peterson, R.L.Boudrie, J.J.Kraushaar, R.A.Ristinen, J.R.Shepard, G.R.Smith, C.F.Moore, W.J.Braithwaite, N.S.P.King, C.L.Morris, H.A.Thiessen, J.Piffaretti Spin and Isospin Transfer in the 12C(π+, π+') Reaction NUCLEAR REACTIONS 12C(π+, π+'), E=100-291 MeV; measured σ(θ); deduced spin, isospin transfer effects. Two-step reaction mechanism.
doi: 10.1103/PhysRevC.21.1030
1980WI07 Phys.Rev. C21, 2535 (1980) E.Winkelmann, P.R.Bevington, M.W.McNaughton, H.B.Willard, P.H.Cverna, E.P.Chamberlin, N.S.P.King Proton-Deuteron Elastic Scattering at 800 MeV NUCLEAR REACTIONS 2H(p, p), E=800 MeV; measured σ(θ), A(θ).
doi: 10.1103/PhysRevC.21.2535
1979AN03 Phys.Rev. C19, 905 (1979) B.D.Anderson, P.R.Bevington, F.H.Cverna, M.W.McNaughton, H.B.Willard, R.J.Barrett, N.S.P.King, D.J.Ernst Proton Total Reaction Cross Section Measurements for 40,44,48Ca at 700 MeV NUCLEAR REACTIONS 40,44,48Ca(p, X), E=700 MeV; measured total reaction σ; deduced matter radii differences.
doi: 10.1103/PhysRevC.19.905
1979SH09 Nucl.Phys. A322, 92 (1979) J.R.Shepard, R.E.Anderson, J.J.Kraushaar, R.A.Ristinen, J.R.Comfort, N.S.P.King, A.Bacher, W.W.Jacobs The (p, t) Reaction on 12C, 54Fe and 208Pb at 80 MeV NUCLEAR REACTIONS 12C, 54Fe, 208Pb(p, t), E=80 MeV; measured σ(E1, θ). 10C, 52Fe, 206Pb levels deduced enhancement factors. Self-supporting enriched 54Fe, 208Pb targets. Zero-range DWBA calculations, determined overall normalizations.
doi: 10.1016/0375-9474(79)90334-8
1978BE36 Phys.Rev.Lett. 41, 384 (1978) P.R.Bevington, M.W.McNaughton, H.B.Willard, H.W.Baer, E.Winkelmann, F.Cverna, E.P.Chamberlin, N.S.P.King, R.R.Stevens, H.Willmes, M.A.Schardt Polarization Analyzing Power A(y)(θ) in pp Elastic Scattering at 643, 787, and 796 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=643, 787, 796 MeV; measured A(θ).
doi: 10.1103/PhysRevLett.41.384
1978CH04 Nucl.Phys. A297, 105 (1978) H.H.Chang, B.W.Ridley, T.H.Braid, T.W.Conlon, E.F.Gibson, N.S.P.King Energy Dependence of the Optical Model Parameters for 3He Ions Scattered from 40Ca and 58Ni NUCLEAR REACTIONS 40Ca, 58Ni(3He, 3He), E=27.7, 51.4, 73.2, 83.5 MeV; measured σ(θ). Enriched targets for 58Ni.
doi: 10.1016/0375-9474(78)90201-4
1978RO04 Phys.Rev. C17, 468 (1978) J.L.Romero, M.W.McNaughton, F.P.Brady, N.S.P.King, T.S.Subramanian, J.L.Ullmann Neutron-Proton Polarization at 50 MeV NUCLEAR REACTIONS 1H(polarized n, p), E=50.0 MeV; measured polarization P(θ).
doi: 10.1103/PhysRevC.17.468
1977BR17 Phys.Rev. C16, 31 (1977) F.P.Brady, N.S.P.King, B.E.Bonner, M.W.McNaughton, J.C.Wang, W.W.True 6Li(n, d)5He and 7Li(n, d)6He with 56.3 MeV Neutrons NUCLEAR REACTIONS 6,7Li(n, d), E=56.3 MeV; measured σ(Ed, θ), θ(cm)=7-60°. 5,6He levels deduced S.
doi: 10.1103/PhysRevC.16.31
1977BR31 Nucl.Phys. A288, 269 (1977) F.P.Brady, J.R.Shepard, N.S.P.King, M.W.McNaughton, J.C.Wang Proton Pickup from 27Al via the (n, d) Reaction at 56.3 MeV NUCLEAR REACTIONS 27Al(n, d), E=56.3 MeV; measured σ(Ed, θ). 26Mg levels deduced S.
doi: 10.1016/0375-9474(77)90134-8
1977DR08 Phys.Rev. C16, 1594 (1977) J.E.Draper, R.J.McDonald, N.S.P.King In-Beam Study of 206Pb Level Scheme Including Conversion Electrons ≥ 40 keV NUCLEAR REACTIONS 204Hg(α, 2nγ), E=30 MeV; measured I(ce), Eγ, Iγ, γγ-coin, γ(t). 206Pb deduced levels, J, π, ICC. Ge(Li), Si(Li) detectors.
doi: 10.1103/PhysRevC.16.1594
1977JO08 Phys.Rev.Lett. 38, 1123 (1977) S.W.Johnson, F.P.Brady, N.S.P.King, M.W.McNaughton Measurement of the n-p Spin-Correlation Parameter A(yy) at 50 MeV NUCLEAR REACTIONS 1H(polarized n, n), E=50 MeV; measured recoil protons; deduced pn spin-correlation parameter.
doi: 10.1103/PhysRevLett.38.1123
1977KI09 Phys.Lett. 69B, 151 (1977) N.S.P.King, J.L.Romero, J.Ullmann, H.E.Conzett, R.M.Larimer, R.Roy Polarization in Proton-Deuteron Scattering at 50 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=50 MeV; measured A(θ).
doi: 10.1016/0370-2693(77)90631-1
1976BR01 Phys.Rev.Lett. 36, 15 (1976) F.P.Brady, N.S.P.King, M.W.McNaughton, G.R.Satchler Excitation of Analogs of Giant Dipole States via the Reaction 27Al(n, p)27Mg NUCLEAR REACTIONS 27Al(n, p), E=56.1 MeV; measured σ(Ep, θ). 27Mg deduced IAS, L.
doi: 10.1103/PhysRevLett.36.15
1976CE02 Phys.Lett. 64B, 411 (1976) F.E.Cecil, J.R.Shepard, R.R.Sercely, R.J.Peterson, N.S.P.King A Study of the 12N 2.43 MeV Level NUCLEAR REACTIONS 12C(3He, 3He'), (3He, t), E=44 MeV; 14N(p, t), E=52 MeV; measured σ(θ). 12N level deduced J, π, T.
doi: 10.1016/0370-2693(76)90108-8
1976CH19 Nucl.Phys. A270, 413 (1976) H.H.Chang, B.W.Ridley, T.H.Braid, T.W.Conlon, E.F.Gibson, N.S.P.King Energy Dependence of the Optical Model Parameters for α-Particles Scattered from 40Ca and 58Ni NUCLEAR REACTIONS 40Ca, 58Ni(α, α), E=24.4-85.6 MeV; measured σ(θ); deduced optical potential parameters. Enriched targets for 58Ni.
doi: 10.1016/0375-9474(76)90454-1
1975MC18 Nucl.Instrum.Methods 130, 555 (1975) M.W.McNaughton, N.S.P.King, F.P.Brady, J.L.Romero, T.S.Subramanian Measurements of 7Li(p, n) and 9Be(p, n) Cross Sections at 15, 20 and 30 MeV NUCLEAR REACTIONS 7Li, 9Be(p, n), E=15, 20, 30 MeV; measured σ.
doi: 10.1016/0029-554X(75)90057-9
1975MC19 Nucl.Instrum.Methods 129, 241 (1975) M.W.McNaughton, N.S.P.King, F.P.Brady, J.L.Ullmann Improved Predictions of Neutron Detection Efficiency Resulting from New Measurements of 12C(n, p) and 12C(n, d) Reactions at 56 MeV NUCLEAR REACTIONS 12C(n, p), (n, d), E=56 MeV; measured σ(θ).
doi: 10.1016/0029-554X(75)90135-4
1974DR02 Phys.Rev. C9, 948 (1974) J.E.Draper, N.S.P.King, W.G.Wyckoff In-Beam Measurement of E0 Matrix Elements in 72Se and 72Ge NUCLEAR REACTIONS 70Ge(α, 2nγ), 72Ge(α, α'γ), (α, npγ), E=27.5 MeV; measured E(ce), I(ce), ce(t), deduced ICC ratios. 72Se, 72Ge deduced levels, T1/2.
doi: 10.1103/PhysRevC.9.948
1974EP01 Phys.Rev. C9, 581 (1974) M.B.Epstein, D.J.Margaziotis, N.S.P.King, T.A.Cahill 20Ne(α, 2α)16O Reaction at 78.6 MeV NUCLEAR REACTIONS 20Ne(α, 2α), E=78.6 MeV; measured σ(Eα, θ). PWIA analysis.
doi: 10.1103/PhysRevC.9.581
1974WA13 Phys.Lett. 51B, 42 (1974) J.C.Wang, F.P.Brady, N.S.P.King, M.W.McNaughton Neutron-Deuteron Differential Cross Section at 26.5 MeV NUCLEAR REACTIONS 2H(n, n), E=26.5 MeV; measured σ(θ).
doi: 10.1016/0370-2693(74)90146-4
1973BA13 Ann.Phys.(New York) 76, 437 (1973) H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green, P.D.Kunz, E.Rost Study of the (p, t) Reaction on the Even-A Titanium Isotopes NUCLEAR REACTIONS 46,48,50Ti(p, t), E=19, 23, 27 MeV; measured σ(Et, θ). Deduced L. 44,46,48Ti deduced levels, J, π.
doi: 10.1016/0003-4916(73)90043-2
1972MO02 Nucl.Phys. A179, 89 (1972) C.E.Moss, N.S.P.King, A.B.Comiter, R.A.Ristinen The (p, nγ) Reaction on 27Al and 28Si NUCLEAR REACTIONS 27Al, 28Si(p, nγ), E=16, 23 MeV; measured Eγ, Iγ, nγ-coin. 27Al, 28Si(p, n), E=16, 23 MeV; measured En. 27Si, 28P deduced levels, γ-branching ratios. Ge(Li) detector.
doi: 10.1016/0375-9474(72)90107-8
1971KI17 Nucl.Phys. A177, 625 (1971) N.S.P.King, C.E.Moss, H.W.Baer, R.A.Ristinen A Study of Excited States in 58Cu, 54Co, 50Mn and 46V NUCLEAR REACTIONS 46Ti, 50Cr, 54Fe, 58Ni(p, nγ), E=7-16 MeV; measured σ(E;En, Eγ). 46Ti, 50Cr, 54Fe, 58Ni(p, n), E=14.5 MeV; measured En. 46Ti(3He, t), E=30 MeV; measured σ(Et). 46V, 50Mn, 54Co, 58Cu deduced levels, J. Enriched targets, Ge(Li) detector.
doi: 10.1016/0375-9474(71)90311-3
1970BA40 Phys.Rev.Lett. 25, 1035 (1970) H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green Inadequacies in a Conventional Distorted-Wave Born-Approximation Analysis of (p, t) Transitions in Titanium Isotopes at E = 27 MeV NUCLEAR REACTIONS 46,48,50Ti(p, t), E=27 MeV; measured σ(Et, θ). 44,46,48Ti transitions deduced L. DWBA.
doi: 10.1103/PhysRevLett.25.1035
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