NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = A.Scott Found 74 matches. 2003EL01 Phys.Rev. C 67, 024609 (2003) J.B.Elliott, L.G.Moretto, L.Phair, G.J.Wozniak, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.C.Kintner, V.Lindenstruth, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, W.F.J.Muller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, H.H.Wieman, T.Wienold, K.Wolf Constructing the phase diagram of finite neutral nuclear matter NUCLEAR REACTIONS C(197Au, X), (La, X), (Kr, X), E=1.0 GeV/nucleon; analyzed fragment charge and mass yields; deduced parameters. Fisher's droplet model, characteristics of neutral nuclear matter discussed.
doi: 10.1103/PhysRevC.67.024609
2001BA99 Phys.Rev. C64, 064305 (2001) Energy of the 9.17 MeV Excited State of 14N NUCLEAR REACTIONS 13C(p, γ), E ≈ 1.75 MeV; measured Eγ, Iγ. 14N levels deduced energies.
doi: 10.1103/PhysRevC.64.064305
2001GR02 Phys.Rev. C63, 014005 (2001) D.L.Groep, M.F.van Batenburg, Th.S.Bauer, H.P.Blok, D.J.Boersma, E.Cisbani, R.De Leo, S.Frullani, F.Garibaldi, W.Glockle, J.Golak, P.Heimberg, W.H.A.Hesselink, M.Iodice, D.G.Ireland, E.Jans, H.Kamada, L.Lapikas, G.J.Lolos, C.J.G.Onderwater, R.Perrino, A.Scott, R.Starink, M.F.M.Steenbakkers, G.M.Urciuoli, H.de Vries, L.B.Weinstein, H.Witala Investigation of the Exclusive 3He(e, e'pp)n Reaction NUCLEAR REACTIONS 3He(e, e'2p), E=564 MeV; measured σ(Eθ), ep-, pp-coin; deduced reaction mechanism features. Continuum-Fadeev calculations.
doi: 10.1103/PhysRevC.63.014005
2000EL09 Phys.Rev.Lett. 85, 1194 (2000) J.B.Elliott, L.G.Moretto, L.Phair, G.J.Wozniak, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.C.Kintner, V.Lindenstruth, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, W.F.J.Muller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.G.Warren, H.H.Wieman, T.Wienold, K.Wolf Nuclear Multifragmentation, Percolation, and the Fisher Droplet Model: Common features of reducibility and thermal scaling NUCLEAR REACTIONS C(197Au, X), E=high; analyzed Au fragmentation data; deduced parameters of droplet and percolation models of nuclear multifragmentation.
doi: 10.1103/PhysRevLett.85.1194
1999GR29 Phys.Rev.Lett. 83, 5443 (1999) D.L.Groep, M.F.van Batenburg, Th.S.Bauer, H.P.Blok, D.J.Boersma, E.Cisbani, R.De Leo, S.Frullani, F.Garibaldi, W.Glockle, J.Golak, P.Heimberg, W.H.A.Hesselink, M.Iodice, D.G.Ireland, E.Jans, H.Kamada, L.Lapikas, G.J.Lolos, R.Perrino, A.Scott, R.Starink, M.F.M.Steenbakkers, G.M.Urciuoli, H.de Vries, L.B.Weinstein, H.Witala Investigation of the Exclusive 3He(e, e'pp)n Reaction NUCLEAR REACTIONS 3He(e, e'2p), E=564 MeV; measured σ(E, θ); deduced reaction mechanism. Continuum Fadeev calculations.
doi: 10.1103/PhysRevLett.83.5443
1999GR37 Nucl.Phys. (Supplement) A654, 509c (1999) D.L.Groep, M.F.van Batenburg, Th.S.Bauer, H.P.Blok, D.J.Boersma, E.Cisbani, R.De Leo, S.Frullani, F.Garibaldi, W.Glockle, J.Golak, P.Heimberg, W.H.A.Hesselink, M.Iodice, D.G.Ireland, E.Jans, H.Kamada, L.Lapikas, G.Lolos, R.Perrino, A.Scott, R.Starink, M.F.M.Steenbakkers, G.M.Urciuoli, H.de Vries, L.B.Weinstein, H.Witala Electron-Induced Two-Proton Knockout from 3He NUCLEAR REACTIONS 3He(e, e'2p), E=564 MeV; measured σ(E, θ). Comparison with continuum Fadeev calculations.
doi: 10.1016/S0375-9474(00)88489-4
1999HT01 Phys.Rev. C59, 336 (1999) M.M.Htun, R.Madey, W.M.Zhang, M.Elaasar, D.Keane, B.D.Anderson, A.R.Baldwin, J.Jiang, A.Scott, Y.Shao, J.W.Watson, K.Frankel, L.Heilbronn, G.Krebs, M.A.McMahan, W.Rathbun, J.Schambach, G.D.Westfall, S.Yennello, C.Gale, J.Zhang Neutrons from Multiplicity-Selected La-La and Nb-Nb Collisions at 400A MeV and La-La Collisions at 250A MeV NUCLEAR REACTIONS La(La, nX), E=250, 400 MeV/nucleon; Nb(Nb, nX), E=250 MeV/nucleon; measured neutron emission σ(θ, φ) vs rapidity; deduced maximum azimuthal anisotropy ratio vs θ, neutron flow features. Comparison with BUU calculations.
doi: 10.1103/PhysRevC.59.336
1999SR03 Phys.Rev. C60, 064606 (1999) B.K.Srivastava, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, P.Danielewicz, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.C.Kintner, V.Lindenstruth, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, W.F.J.Muller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.P.Scharenberg, A.Scott, Y.Shao, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, H.H.Wieman, T.Wienold, K.Wolf, and the EOS Collaboration Comparison of the 1A GeV 197Au + C Interaction with First-Stage Transport Codes NUCLEAR REACTIONS C(197Au, X), E=1 GeV/nucleon; measured light, intermediate fragments mass, energy distributions. Comparisons with intranuclear cascade and BUU transport calculations.
doi: 10.1103/PhysRevC.60.064606
1998HE33 Phys.Rev. C58, 3451 (1998) L.Heilbronn, R.Madey, M.Elaasar, M.Htun, K.Frankel, W.G.Gong, B.D.Anderson, A.R.Baldwin, J.Jiang, D.Keane, M.A.McMahan, W.H.Rathbun, A.Scott, Y.Shao, J.W.Watson, G.D.Westfall, S.Yennello, W.-M.Zhang Neutron Yields from 435 MeV/nucleon Nb Stopping in Nb and 272 MeV/nucleon Nb Stopping in Nb and Al NUCLEAR REACTIONS 93Nb(93Nb, nX), E=272, 435 MeV/nucleon; 27Al(93Nb, nX), E=272 MeV/nucleon; measured neutron stopping-target yields, multiplicity, σ(En, θ). Comparison to model calculations.
doi: 10.1103/PhysRevC.58.3451
1997HA38 Nucl.Phys. A621, 285c (1997) V.Y.Hansper, S.G.Tims, A.J.Morton, A.F.Scott, C.I.W.Tingwell, D.G.Sargood Cross Sections and Reaction Rates Relevant to Silicon Burning NUCLEAR REACTIONS 52Cr(α, n), E=4-10 MeV; 52Cr(α, p), E=6-10 MeV; 55Mn(p, n), E=0.7-2.1 MeV; 55Mn(p, γ), E=0.7-2.1 MeV; analyzed data; deduced model parameters, thermonuclear reaction rates. Statistical model.
doi: 10.1016/S0375-9474(97)00256-X
1997HJ01 Phys.Rev.Lett. 79, 4345 (1997) E.L.Hjort, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, A.Insolia, M.Justice, D.Keane, J.C.Kintner, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.G.Warren, H.H.Wieman, T.Wienold, K.Wolf Δ Resonance Production in 58Ni + Cu Collisions at E = 1.97A GeV NUCLEAR REACTIONS Cu(58Ni, X), E=1.97 GeV/nucleon; measured invariant mass spectra associated with π±, π--absorption on proton; deduced Δ resonance mass shift.
doi: 10.1103/PhysRevLett.79.4345
1997KI07 Phys.Rev.Lett. 78, 4165 (1997) J.C.Kintner, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.Scharenberg, A.Scott, Y.Shao, B.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, H.H.Wieman, T.Wienold, K.Wolf Pion Flow and Antiflow in 1.15A GeV Au + Au NUCLEAR REACTIONS 197Au(197Au, X), E=1.15 GeV/nucleon; measured pion transverse flow vs impact parameter; deduced antiflow behavior for π+, π-.
doi: 10.1103/PhysRevLett.78.4165
1996HA19 Phys.Rev.Lett. 77, 235 (1996) J.A.Hauger, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.C.Kintner, V.Lindenstruth, M.A.Lisa, U.Lynen, H.S.Matis, M.McMahan, C.McParland, W.F.J.Muller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, H.H.Wieman, T.Wienold, K.Wolf, and the EOS Collaboration Dynamics of the Multifragmentation of 1A GeV Gold on Carbon NUCLEAR REACTIONS Cu(197Au, X), E=1 GeV/nucleon; analyzed multi-fragmentation dynamics; deduced prompt, equilibrated remnant decay stages.
doi: 10.1103/PhysRevLett.77.235
1996WA17 Phys.Rev.Lett. 76, 3911 (1996) S.Wang, M.A.Lisa, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.Kintner, V.Lindenstruth, H.Liu, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.L.Tincknell, C.Tuve, P.G.Warren, D.Weerasundara, H.H.Wieman, K.L.Wolf, and the EOS Collaboration In-Plane Retardation of Collective Expansion in Au + Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=600 MeV/nucleon; measured light fragments transverse mass spectra, other features; deduced collective expansion in-plane retardation related features.
doi: 10.1103/PhysRevLett.76.3911
1995LI41 Phys.Rev.Lett. 75, 2662 (1995) M.A.Lisa, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.Kintner, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, G.D.Westfall, H.H.Wieman, K.Wolf, and the EOS Collaboration Radial Flow in Au + Au Collisions at E = (0.25-1.15)A GeV NUCLEAR REACTIONS 197Au(197Au, X), E=0.25-1.15 GeV/nucleon; measured light fragment energy spectra at midrapidity; deduced temperature, radial flow parameters. Quantum molecular dynamics, BUU models analysis.
doi: 10.1103/PhysRevLett.75.2662
1995PA39 Phys.Rev.Lett. 75, 2100 (1995) M.D.Partlan, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.Cebra, A.D.Chacon, J.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.Kintner, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, G.Peilert, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.L.Tincknell, C.Tuve, S.Wang, P.G.Warren, H.H.Wieman, K.Wolf, and the EOS Collaboration Fragment Flow in Au + Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=0.25-1.15 GeV/nucleon; measured light fragment associated averaged collective flow; deduced 'soft' or 'hard' equation of state inadequacy.
doi: 10.1103/PhysRevLett.75.2100
1995RI02 Nucl.Phys. A583, 491c (1995) H.G.Ritter, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.Kintner, V.Lindenstruth, M.A.Lisa, U.Lynen, H.S.Matis, M.McMahan, C.McParland, W.F.J.Mueller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.L.Tincknell, C.Tuve, S.Wang, P.G.Warren, H.H.Wieman, K.L.Wolf, and the EOS Collaboration Flow and Multifragmentation in Nuclear Collisions at Intermediate Energies NUCLEAR REACTIONS 197Au(197Au, X), E=0.25-1.15 GeV/nucleon; measured light fragment σ(θ, E); deduced radially expanding thermal source properties.
doi: 10.1016/0375-9474(94)00710-5
1995WA11 Phys.Rev.Lett. 74, 2646 (1995) S.Wang, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, M.L.Gilkes, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.Kintner, M.A.Lisa, H.S.Matis, M.McMahan, C.McParland, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, R.P.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.L.Tincknell, C.Tuve, P.G.Warren, D.Weerasundara, H.H.Wieman, K.L.Wolf, and the EOS Collaboration Light Fragment Production and Power Law Behavior in Au + Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=1.15 GeV/nucleon; measured momentum space light charged particle densities vs rapidity, multiplicity, beam energy; deduced momentum-space coalescence evidence.
doi: 10.1103/PhysRevLett.74.2646
1994FE05 Phys.Rev. C49, 2068 (1994) A.E.Feldman, J.J.Kelly, B.S.Flanders, M.A.Khandaker, H.Seifert, P.Boberg, S.D.Hyman, P.H.Karen, B.E.Norum, P.Welch, Q.Chen, A.D.Bacher, G.P.A.Berg, E.J.Stephenson, S.Nanda, A.Saha, A.Scott Neutron Transition Densities for 48Ca from Proton Scattering at 200 and 318 MeV NUCLEAR REACTIONS 48Ca(polarized p, p'), (polarized p, p), E=200, 318 MeV; measured σ(θ), analyzing power vs θ. 48Ca levels deduced nucleon transition densities, multipole moments. Extended random phase approximation.
doi: 10.1103/PhysRevC.49.2068
1994GI10 Phys.Rev.Lett. 73, 1590 (1994) M.L.Gilkes, S.Albergo, F.Bieser, F.P.Brady, Z.Caccia, D.A.Cebra, A.D.Chacon, J.L.Chance, Y.Choi, S.Costa, J.B.Elliott, J.A.Hauger, A.S.Hirsch, E.L.Hjort, A.Insolia, M.Justice, D.Keane, J.C.Kintner, V.Lindenstruth, M.A.Lisa, U.Lynen, H.S.Matis, M.McMahan, C.McParland, W.F.J.Muller, D.L.Olson, M.D.Partlan, N.T.Porile, R.Potenza, G.Rai, J.Rasmussen, H.G.Ritter, J.Romanski, J.L.Romero, G.V.Russo, H.Sann, R.Scharenberg, A.Scott, Y.Shao, B.K.Srivastava, T.J.M.Symons, M.Tincknell, C.Tuve, S.Wang, P.Warren, H.H.Wieman, K.Wolf, and the EOS Collaboration Determination of Critical Exponents from the Multifragmentation of Gold Nuclei NUCLEAR REACTIONS C(197Au, X), E=1 GeV/nucleon; measured charged fragment distribution; deduced critical exponents value.
doi: 10.1103/PhysRevLett.73.1590
1994MO11 Nucl.Phys. A573, 276 (1994) A.J.Morton, A.F.Scott, S.G.Tims, V.Y.Hansper, D.G.Sargood The 50Cr(α, n)53Fe and 50Cr(α, p)53Mn Cross Sections NUCLEAR REACTIONS, ICPND 50Cr(α, n), E=5.409-10.009 MeV; 50Cr(α, p), E=4.868-10.009 MeV; measured neutron, proton, activation yields; deduced σ(E), thermonuclear reaction rates. Statistical model analysis. Enriched target.
doi: 10.1016/0375-9474(94)90171-6
1993DE31 Nuovo Cim. 106A, 1119 (1993) R.De Swiniarski, F.T.Baker, A.Scott, C.Glashausser, K.W.Jones Elastic and Inelastic Scattering of 0.8 GeV Polarized Protons from 18O NUCLEAR REACTIONS 18O(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 18O level deduced L. Dirac equation based coupled-channels calculation.
doi: 10.1007/BF02773499
1993HA01 Nucl.Phys. A551, 158 (1993) V.Y.Hansper, A.J.Morton, S.G.Tims, C.I.W.Tingwell, A.F.Scott, D.G.Sargood Cross Sections and Thermonuclear Reaction Rates for 51V(α, n)54Mn and 51V(α, p)54Cr NUCLEAR REACTIONS, ICPND 51V(α, n), E=2-9.49 MeV; 51V(α, p), E=5.755-9.59 MeV; measured neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Natural targets, activation technique.
doi: 10.1016/0375-9474(93)90309-L
1993KE03 Phys.Rev. C47, 2146 (1993) J.J.Kelly, B.S.Flanders, F.W.Hersman, J.H.Heisenberg, J.Calarco, J.P.Connelly, T.E.Milliman, A.Scott, F.T.Baker, V.Penumetcha, W.P.Jones, G.T.Emery, A.D.Bacher, C.Olmer, M.A.Grimm, M.L.Whiten Neutron Transition Densities from 88Sr(p, p') at E(p) = 200 MeV NUCLEAR REACTIONS 88Sr(polarized p, p'), (polarized p, p), E=200 MeV; measured σ(θ), analyzing power vs θ. 88Sr levels deduced neutron transition densities. Shell model comparison.
doi: 10.1103/PhysRevC.47.2146
1993SC05 Nucl.Phys. A552, 363 (1993) A.F.Scott, A.J.Morton, S.G.Tims, V.Y.Hansper, D.G.Sargood The 34S(α, γ)38Ar, 34S(α, n)37Ar and 34S(α, p)37Cl Cross Sections NUCLEAR REACTIONS, ICPND 34S(α, γ), E=2.79-5.87 MeV; 34S(α, n), E=5.26-9.88 MeV; 34S(α, p), E=5.7-9.33 MeV; measured γ-spectra, neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched target.
doi: 10.1016/0375-9474(93)90499-N
1993SE02 Phys.Rev. C47, 1615 (1993) H.Seifert, J.J.Kelly, A.E.Feldman, B.S.Flanders, M.A.Khandaker, Q.Chen, A.D.Bacher, G.P.A.Berg, E.J.Stephenson, P.Karen, B.E.Norum, P.Welch, A.Scott Effective Interaction for 16O(p, p') and 40Ca(p, p') at E(p) = 200 MeV NUCLEAR REACTIONS 16O, 40Ca(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced effective interaction. Relativistic impulse approximation model, other data input.
doi: 10.1103/PhysRevC.47.1615
1993TI06 Nucl.Phys. A563, 473 (1993) S.G.Tims, A.F.Scott, A.J.Morton, V.Y.Hansper, D.G.Sargood Cross Sections of the Reactions 58Fe(p, γ)59Co, 58Fe(p, n)58Co, 55Mn(α, n)58Co, 55Mn(α, p)58Fe and 57Fe(p, n)57Co NUCLEAR REACTIONS, ICPND 58Fe(p, γ), E=0.785-4.65 MeV; 58Fe(p, n), E=3.155-4.925 MeV; 55Mn(α, n), E=2.7-9.995 MeV; 55Mn(α, p), E=5.145-10.045 MeV; 57Fe(p, n), E=1.645-3.155 MeV; measured gamma, neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched, natural targets, activation technique.
doi: 10.1016/0375-9474(93)90124-G
1992MO04 Nucl.Phys. A537, 167 (1992) A.J.Morton, S.G.Tims, A.F.Scott, V.Y.Hansper, C.I.W.Tingwell, D.G.Sargood The 48Ti(α, n)51Cr and 48Ti(α, p)51V Cross Sections NUCLEAR REACTIONS, ICPND 48Ti(α, n), E=4.98-9.52 MeV; 48Ti(α, p), E=5.52-8.98 MeV; measured neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets, activation technique.
doi: 10.1016/0375-9474(92)90163-E
1991SC07 Nucl.Phys. A523, 373 (1991) A.F.Scott, A.J.Morton, C.I.W.Tingwell, S.G.Tims, V.Y.Hansper, D.G.Sargood Cross Sections and Thermonuclear Reaction Rates for 41K(α, n)44Sc and 41K(α, p)44Ca NUCLEAR REACTIONS, ICPND 41K(α, n), E=3-8 MeV; 41K(α, p), E=4.5-9 MeV; measured neutron, proton yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets, activation technique.
doi: 10.1016/0375-9474(91)90009-U
1991TI01 Nucl.Phys. A524, 479 (1991) S.G.Tims, A.J.Morton, C.I.W.Tingwell, A.F.Scott, V.Y.Hansper, D.G.Sargood The 54Fe(α, n)57Ni and 54Fe(α, p)57Co Cross Sections NUCLEAR REACTIONS, ICPND 54Fe(α, n), E=6.35-9.5 MeV; 54Fe(α, p), E=5.31-9.59 MeV; measured neutron, proton, activation yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(91)90281-A
1989HA38 Nucl.Phys. A504, 605 (1989) V.Y.Hansper, C.I.W.Tingwell, S.G.Tims, A.F.Scott, D.G.Sargood The 45Sc(α, p)48Ti and 45Sc(α, n)48V Cross Sections NUCLEAR REACTIONS, ICPND 45Sc(α, p), E=4.45-9.15 MeV; 45Sc(α, n), E=3.76-9.98 MeV; measured proton, neutron, activation yields; deduced σ(E), thermonuclear reaction rates. Statistical model analysis. Natural targets.
doi: 10.1016/0375-9474(89)90560-5
1989TI01 Nucl.Phys. A496, 127 (1989) C.I.W.Tingwell, V.Y.Hansper, S.G.Tims, A.F.Scott, A.J.Morton, D.G.Sargood The 60Ni(p, γ)61Cu and 62Ni(p, γ)63Cu Cross Sections NUCLEAR REACTIONS, ICPND 60Ni(p, γ), (p, p'γ), E=1-4 MeV; 61Ni(p, γ), (p, p'γ), E=1.02-4.42 MeV; measured γ-ray yields; deduced σ(E), thermonuclear reaction rates. 61Cu deduced resonances, strengths. Statistical model analysis. Enriched targets.
doi: 10.1016/0375-9474(89)90219-4
1988TI03 Nucl.Phys. A480, 162 (1988) C.I.W.Tingwell, V.Y.Hansper, S.G.Tims, A.F.Scott, D.G.Sargood Cross Sections of Proton Induced Reactions on 61Ni NUCLEAR REACTIONS, ICPND 61Ni(p, γ), (p, p'γ), E=1.05-3.98 MeV; 61Ni(p, n), E=3.08-4.66 MeV; measured γ-ray, neutron, activation yields; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched target.
doi: 10.1016/0375-9474(88)90390-9
1988TI05 Nucl.Phys. A483, 354 (1988); Erratum Nucl.Phys. A518, 801 (1990) S.G.Tims, C.I.W.Tingwell, V.Y.Hansper, A.F.Scott, D.G.Sargood The 59Co(α, p)62Ni and 59Co(α, n)62Cu Cross Sections NUCLEAR REACTIONS, ICPND 59Co(α, p), E=5.18-9.4 MeV; 59Co(α, n), E=5.07-9.8 MeV; measured proton, neutron, activation yields; deduced σ(E), thermonuclear reaction rates. Natural targets.
doi: 10.1016/0375-9474(88)90541-6
1987SC27 Nucl.Phys. A475, 548 (1987) A.F.Scott, C.I.W.Tingwell, V.Y.Hansper, S.G.Tims, D.G.Sargood The 39K(α, p)42Ca Cross Section and Thermonuclear Reaction Rate NUCLEAR REACTIONS, ICPND 39K(α, p), E=4.5-9 MeV; measured proton yield; deduced σ(E), thermonuclear reaction rates. Statistical-model analysis. Enriched targets.
doi: 10.1016/0375-9474(87)90077-7
1986MI06 Phys.Lett. 169B, 166 (1986) C.A.Miller, A.Scott, R.Abegg, R.Helmer, K.P.Jackson, M.Whiten, S.Yen, L.Lee, T.E.Drake, D.Frekers, S.S.M.Wong, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Dymarz, H.V.von Geramb, C.J.Horowitz Large Angle Elastic Scattering of 200 MeV Protons from 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced exchange medium effects role. Microscopic Schrodinger, relativistic impulse approximation analyses.
doi: 10.1016/0370-2693(86)90643-X
1984GR02 Phys.Rev. C29, 459 (1984) E.E.Gross, T.P.Cleary, J.L.C.Ford, Jr., D.C.Hensley, K.S.Toth, F.T.Baker, A.Scott, C.R.Bingham, J.A.Vrba Nuclear Moments of the First Excited State of 22Ne from 22Ne(132 MeV) + 208Pb Scattering NUCLEAR REACTIONS 208Pb(22Ne, 22Ne), (22Ne, 22Ne'), E=132 MeV; measured σ(θ); deduced optical potential parameters. 22Ne levels deduced quadrupole, hexadecapole deformation parameters, transition matrix elements. Enriched target, coupled-channels analysis.
doi: 10.1103/PhysRevC.29.459
1983BA06 Nucl.Phys. A393, 283 (1983) F.T.Baker, A.Scott, M.A.Grimm, W.G.Love, V.Penumetcha, C.Glashausser, G.S.Adams, G.Igo, G.W.Hoffmann, J.M.Moss, W.Swenson, B.E.Wood The 90,92Zr(p(pol), p') Reactions at E(p) = 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(Ep', θ), σ(θ), Aθ, A(Ep', θ). Distorted wave analyses, collective, semimicroscopic-models, free nucleon-nucleon t-matrix. Enriched targets.
doi: 10.1016/0375-9474(83)90143-4
1982BA38 Nucl.Phys. A386, 45 (1982) F.T.Baker, A.Scott, W.G.Love, J.A.Mowrey, W.P.Jones, J.D.Wiggins A Comparison of t-Matrix and G-Matrix Analyses for the 207Pb(p, p') Reaction at E(p) = 95 MeV NUCLEAR REACTIONS 207Pb(p, p'), E=95 MeV; measured σ(Ep', θ). 207Pb deduced levels, β(L). Semi-microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(82)90400-6
1982GL08 Phys.Lett. 116B, 215 (1982) C.Glashausser, R.De Swiniarski, K.Jones, S.Nanda, F.T.Baker, M.Grimm, V.Penumetcha, A.Scott, G.Adams, G.Igo, G.W.Hoffmann, J.Moss, W.Swenson, B.E.Wood Coupled-Channels Analysis of 800 MeV Polarized Proton Inelastic Scattering from 18O NUCLEAR REACTIONS 18O(polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 18O deduced β2, β4, β6. Coupled-channels analysis.
doi: 10.1016/0370-2693(82)90328-8
1981BA01 Nucl.Phys. A351, 63 (1981) F.T.Baker, A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek 182,184,186W(α, α') Reactions at Eα = 24 MeV NUCLEAR REACTIONS 182,184,186W(α, α'), E=24 MeV; measured σ(Eα', θ); deduced optical model parameters. 182,184,186W deduced β2, β4 charge, density quadrupole, hexadecapole moments. 184W deduced β3. Enriched targets. Rotational-vibrational model.
doi: 10.1016/0375-9474(81)90545-5
1981BA49 Nucl.Phys. A371, 68 (1981) F.T.Baker, M.A.Grimm, Jr., A.Scott, R.C.Styles, T.H.Kruse, K.Jones, R.Suchannek 192Os(α, α') Reaction at Eα = 24 MeV and the IBA Model NUCLEAR REACTIONS 192Os(α, α), (α, α'), E=24 MeV; measured σ(θ), σ(Eα', θ). 192Os deduced B(E4), deformation parameter β4. Enriched target. Interacting boson model, coupled-channels analysis.
doi: 10.1016/0375-9474(81)90745-4
1981BA54 Phys.Rev.Lett. 47, 1823 (1981) F.T.Baker, C.Glashausser, A.Scott, M.A.Grimm, G.S.Adams, G.Hoffmann, G.Igo, W.G.Love, J.M.Moss, S.Nanda, V.Penumetcha, W.Swenson, B.E.Wood Test of Data-to-Data Relations for the Reactions 90,92Zr(p(pol), p') at 800 MeV NUCLEAR REACTIONS 90,92Zr(polarized p, p), (polarized p, p'), E=800 MeV; measured σ(θ), analyzing power vs θ; deduced data-to-data relation inadequacies.
doi: 10.1103/PhysRevLett.47.1823
1981SC04 Nucl.Phys. A357, 9 (1981) A.Scott, F.T.Baker, W.G.Love, J.D.Wiggins, Jr., M.L.Whiten Comparison of the 92Mo(p, p') and 90Zr(p, p') Reactions at 61.2 MeV NUCLEAR REACTIONS 92Mo(p, p'), E=61.2 MeV; measured σ(Ep', θ). 90Zr(p, p'), E=61.2 MeV; analyzed σ(θ). 92Mo deduced levels, deformation parameter β(L). Isotopically enriched target.
doi: 10.1016/0375-9474(81)90623-0
1981SC11 Nucl.Phys. A366, 91 (1981) A.Scott, F.T.Baker, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. 207Pb(p, p') Measurements at 135 and 61 MeV, the Effective Interaction and Core Polarization NUCLEAR REACTIONS 207Pb(p, p'), E=134.8 MeV; measured σ(Ep', θ). 207Pb deduced levels, deformation β(L). Enriched target. Microscopic DWBA, DWIA calculations.
doi: 10.1016/0375-9474(81)90489-9
1980MO06 Phys.Rev.Lett. 44, 1189 (1980) J.M.Moss, C.Glashausser, F.T.Baker, R.Boudrie, W.D.Cornelius, N.Hintz, G.Hoffmann, G.Kyle, W.G.Love, A.Scott, H.A.Thiessen Excitation of Unnatural-Parity States in 12C by 800-MeV Polarized Protons NUCLEAR REACTIONS 12C(polarized p, p'), E=800 MeV; measured σ(θ), A(θ). 12C levels deduced T, J, π. DWIA analysis.
doi: 10.1103/PhysRevLett.44.1189
1980SC21 Phys.Rev.Lett. 45, 1315 (1980) A.Scott, F.T.Baker, M.A.Grimm, Jr., J.H.Johnson, V.Penumetcha, R.C.Styles, W.G.Love, W.P.Jones, J.D.Wiggins, Jr. Shapes of Measured (p(pol), p') Analyzing Powers at 160 MeV for Proton States in 90Zr and Neutron States in 92Zr NUCLEAR REACTIONS 90,92Zr(polarized p, p'), E=160 MeV; measured analyzing power vs θ; deduced spin-orbit potential parameters. 90,92Zr levels deduced configurations, β. DWIA, free nucleon-nucleon t-matrix.
doi: 10.1103/PhysRevLett.45.1315
1979BA19 Nucl.Phys. A321, 222 (1979) F.T.Baker, A.Scott, T.P.Cleary, J.L.C.Ford, E.E.Gross, D.C.Hensley 194Pt(12C, 12C') Reaction and the Triaxial-Rotor Model NUCLEAR REACTIONS 194Pt(12C, 12C'), E=78 MeV, θ(cm)=25°-80°; measured σ(E(12C), θcm). 194Pt deduced optical-model parameters, asymmetric-rotor model parameters β2, β4, γ. Enriched target.
doi: 10.1016/0375-9474(79)90695-X
1979BA32 Nucl.Phys. A325, 525 (1979) F.T.Baker, A.Scott, E.E.Gross, D.C.Hensley, D.L.Hillis 30Si(12C, 12C') Reaction at 41.3 MeV NUCLEAR REACTIONS 30Si(12C, 12C'), E=41.3 MeV; measured σ(E(12C'), θ); deduced optical-model parameters. 30Si level deduced sign, magnitude of nuclear β. Enriched target.
doi: 10.1016/0375-9474(79)90030-7
1978BA20 Phys.Rev. C17, 1559 (1978) F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin 192Pt(α, α') Reaction at E = 24 MeV NUCLEAR REACTIONS 192Pt(α, α'), E=24 MeV; measured σ(Eα', θ). 192Pt levels deduced β, relative signs of matrix elements. Coupled channels analysis. Enriched target.
doi: 10.1103/PhysRevC.17.1559
1978LO01 Phys.Lett. 73B, 277 (1978) W.G.Love, A.Scott, F.T.Baker, W.P.Jones, J.D.Wiggins, Jr. A Test of the DWIA at 135 MeV Using the 207Pb(p, p') Reaction NUCLEAR REACTIONS 207Pb(p, p'), E=135 MeV; calculted σ(θ).
doi: 10.1016/0370-2693(78)90513-0
1978RO02 Phys.Rev.Lett. 40, 364 (1978) R.M.Ronningen, F.T.Baker, A.Scott, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton Evidence for a Nonrotational Interpretation of [0+ m(E4) 4+] in 180Hf NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf levels deduced β2, β4.
doi: 10.1103/PhysRevLett.40.364
1978SA06 Nucl.Phys. A298, 313 (1978) G.R.Satchler, M.L.Halbert, N.M.Clarke, E.E.Gross, C.B.Fulmer, A.Scott, D.Martin, M.D.Cohler, D.C.Hensley, C.A.Ludemann, J.G.Cramer, M.S.Zisman, R.M.DeVries Heavy-Ion Elastic Scattering (II). 142 MeV 16O on 28Si, 59Co and 60Ni NUCLEAR REACTIONS 28Si, 59Co, 60Ni(16O, 16O); 28Si, 60Ni(16O, 16O'), E=141.9 MeV; measured σ(θ); deduced optical potentials.
doi: 10.1016/0375-9474(78)90259-2
1977BA31 Nucl.Phys. A284, 135 (1977) F.T.Baker, A.Scott, E.E.Gross, D.C.Hensley, D.L.Hillis Nuclear Reorientation Effects for the 26Mg, 28Si(12C, 12C') Reactions at E = 41 MeV NUCLEAR REACTIONS 26Mg(12C, 12C'), E=41.3 MeV, θ(cm)=19°-66°; 28Si(12C, 12C'), E=41.4 MeV, θ(cm)=18°-70°; measured σ(E(12C'), θ(cm)). 26Mg, 28Si deduced optical-model parameters, nuclear β2 deformations, signs of 2+ quadrupole moments. Enriched targets.
doi: 10.1016/0375-9474(77)90690-X
1977BA58 Phys.Lett. 70B, 167 (1977) F.T.Baker, A.Scott, R.M.Ronningen, T.H.Kruse, R.Suchannek, W.Savin, J.H.Hamilton Sensitivity of (α, α') Cross Sections to Excited-State Quadrupole Moments NUCLEAR REACTIONS 180Hf(α, α'), E=21, 24 MeV; measured σ(Eα', θ). 180Hf level deduced β.
doi: 10.1016/0370-2693(77)90512-3
1977HI07 Phys.Rev. C16, 1467 (1977) D.L.Hillis, E.E.Gross, D.C.Hensley, C.R.Bingham, F.T.Baker, A.Scott Multistep Effects in the Elastic and Inelastic Scattering of 70.4-MeV 12C Ions from the Even Neodymium Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(12C, 12C), (12C, 12C'), E=70.4 MeV; measured σ(θ); deduced optical model parameters. 142,144,146,148,150Nd deduced β. Coupled-channel analysis. Enriched targets.
doi: 10.1103/PhysRevC.16.1467
1977SC17 Nucl.Phys. A285, 222 (1977) A.Scott, N.P.Mathur, F.Petrovich Low-Lying Normal Parity Excitations in the 208Pb(p, p')208Pb Reaction at E = 61.2 MeV NUCLEAR REACTIONS 208Pb(p, p'), E=61.2 MeV; measured σ(Ep', θ). 208Pb deduced levels, β(L). Isotopically enriched target, 99.3%.
doi: 10.1016/0375-9474(77)90249-4
1977SC26 Nucl.Phys. A289, 123 (1977) Excitation of Neutron-Hole States in 207Pb by Inelastic Scattering of 61 MeV Protons NUCLEAR REACTIONS 207Pb(p, p'), E=61.2 MeV; measured σ(Ep', θ). 207Pb deduced levels, β(L). Isotopically enriched target, 92.4%.
doi: 10.1016/0375-9474(77)90525-5
1976BA23 Phys.Rev.Lett. 37, 193 (1976) F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin Experimental Determination of the Signs of E2 Interference Terms for 192Os and 194Pt NUCLEAR REACTIONS 192Os, 194Pt(α, α'), E=12-24 MeV; analyzed data. 192Os, 194Pt deduced sign of interference term.
doi: 10.1103/PhysRevLett.37.193
1976BA35 Nucl.Phys. A266, 337 (1976) F.T.Baker, A.Scott, T.H.Kruse, W.Hartwig, E.Ventura, W.Savin Nuclear Shapes of the Transitional Nuclei 194,196,198Pt NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-24 MeV, θlab=127.5°; measured σ(E, e'). 194,196,198Pt deduced β2, β4 charge, mass deformations. 194Pt deduced sign of interference term.
doi: 10.1016/0375-9474(76)90362-6
1976HI01 Phys.Rev.Lett. 36, 304 (1976) D.L.Hillis, E.E.Gross, D.C.Hensley, L.D.Rickertsen, C.R.Bingham, A.Scott, F.T.Baker Multistep Processes in the Inelastic Scattering of 70.4-MeV 12C from 144Nd NUCLEAR REACTIONS 144Nd(12C, 12C'), E=70.4 MeV; measured σ(E(12C'), θ). 144Nd levels deduced J, π, coupling.
doi: 10.1103/PhysRevLett.36.304
1974SC20 Nucl.Phys. A226, 109 (1974) Core Polarization in Inelastic Proton Scattering from 209Bi at 61 MeV NUCLEAR REACTIONS 209Bi(p, p'), E=61.2 MeV; measured σ(Ep', θ). 209Bi deduced levels, β(L).
doi: 10.1016/0375-9474(74)90603-4
1973HO10 Nucl.Phys. A203, 339 (1973) C.G.Hoot, D.K.Olsen, R.E.Brown, J.R.Maxwell, A.Scott Study of Some Two-Nucleon Pick-up Reactions in the 1p Shell with 39.8 MeV Protons NUCLEAR REACTIONS 12C, 14N, 16O(p, 3He), 14C(p, t), Ep=39.8 MeV; measured σ(E(3He), θ), σ(Et, θ). DWBA analysis.
doi: 10.1016/0375-9474(73)90139-5
1972WH03 Nucl.Phys. A181, 417 (1972) M.L.Whiten, A.Scott, G.R.Satchler Inelastic Scattering of 61 MeV Protons from 90Zr and 89Y NUCLEAR REACTIONS 90Zr(p, p'), Ep=61.2 MeV; measured σ(Ep', θ). 90Zr deduced levels, some β(L). Enriched target, 98.6 %.
doi: 10.1016/0375-9474(72)90493-9
1972WO03 Nucl.Phys. A179, 657 (1972) P.B.Woollam, R.J.Griffiths, F.G.Kingston, C.B.Fulmer, J.C.Hafele, A.Scott Analysis of 50.8 MeV Proton Scattering from the Samarium Isotopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, p), (p, p')E=50.8 MeV; measured σ(θ) for ground state, lowest 2+ level, also lowest 4+ level for 154Sm; deduced optical-model parameters. 144,148,150,152,154Sm deduced β2 values. Collective-model DWBA, SCA analysis. Enriched targets, magnetic spectrograph, photographic plates.
doi: 10.1016/0375-9474(72)90610-0
1970FU05 Phys.Lett. 32B, 454 (1970) C.B.Fulmer, F.G.Kingston, A.Scott, J.C.Hafele Elastic Scattering of 50.8 MeV Protons from the Even Samarium Isotopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, p), E=50.8 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1016/0370-2693(70)90381-3
1969FU07 Phys.Rev. 181, 1565 (1969) C.B.Fulmer, J.B.Ball, A.Scott, M.L.Whiten Elastic Scattering of 61.4-MeV Protons NUCLEAR REACTIONS 12C, 27Al, 40Ca, 58Ni, 68Zn, 90Zr, 116Sn, 208Pb(p, p), E = 61.4 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRev.181.1565
1969SC25 Nucl.Phys. A137, 445 (1969) Inelastic Scattering of 61 MeV Protons from 89Y and the Associated Reaction Mechanisms NUCLEAR REACTIONS 89Y(p, p'), E = 61.2 MeV; measured σ(Ep', θ). 89Y deduced levels, β(L).
doi: 10.1016/0375-9474(69)90119-5
1967SC24 Phys.Lett. 25B, 463 (1967) Excitation of the 0.908 MeV Level in 89Y by Inelastic Scattering of 61.2 MeV Protons NUCLEAR STRUCTURE 89Y; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90108-6
1966SC07 Phys.Letters 20, 654 (1966) Inelastic Scattering of 40 MeV Protons by 208Pb NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91161-9
1964BL04 Phys. Rev. 134, B481 (1964) S.D.Bloom, L.G.Mann, R.Polichar, J.R.Richardson, A.Scott Circular Polarization Measurement of Gamma Rays Following Beta Decay of Al24 and Na24 to Determine the Meson Exchange Effect NUCLEAR STRUCTURE 24Al, 24Na; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B481
1963MA35 Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p.11 (1963) L.G.Mann, S.D.Bloom, A.Scott, R.Polichar, J.R.Richardson Circular Polarization Measurements in Na24 and Al24 to Determine the Mesonic Exchange Effect in β Decay NUCLEAR STRUCTURE 24Na, 24Al; measured not abstracted; deduced nuclear properties.
1963PO11 Bull.Am.Phys.Soc. 8, No.8, 595, D5 (1963) Ground-State Spin of Al28 NUCLEAR STRUCTURE 28Al; measured not abstracted; deduced nuclear properties.
1963SC02 Bull.Am.Phys.Soc. 8, No.1, 85, YB5 (1963) Positron Spectra of Al24 NUCLEAR STRUCTURE 24Al; measured not abstracted; deduced nuclear properties.
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