NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.Flanders Found 36 matches. 2008AN15 Phys.Rev. C 78, 065803 (2008) N.Anantaraman, S.M.Austin, B.A.Brown, G.M.Crawley, A.Galonsky, R.G.T.Zegers, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, J.W.Watson, C.C.Foster Electron capture strength for 60, 62Ni and 58, 60, 62, 64Ni(p, n)58, 60, 62, 64Cu reactions at 134.3 MeV NUCLEAR REACTIONS 58,60,62,64Ni(p, n), E=134.3 MeV; measured neutron spectra, angular distributions, σ; calculated B(GT), reaction rates. 58,60,62,64Cu; deduced levels. Comparison with (n, p) reactions, shell model calculations.
doi: 10.1103/PhysRevC.78.065803
2001KH19 Phys.Rev. C64, 064606 (2001) M.G.Khayat, P.G.Roos, N.S.Chant, A.P.Dvoredsky, H.Breuer, J.J.Kelly, B.S.Flanders, T.M.Payerle, F.Adimi, T.Gu, J.Huffman, A.Klein, T.Dooling, T.Greco, G.S.Kyle, T.Chang, Z.Lin, M.Wang, R.Meier, S.Ritt, K.Koch, J.Konter, S.Kovalev, S.Mango, B.Van Den Brandt, J.Lawrie Analyzing Power Reduction in Quasifree Pion-Nucleon Knockout Reactions NUCLEAR REACTIONS 7Li(π+, π+'p), E=240 MeV; measured σ(E, θ), Ay(θ); deduced spin dependence in Δ-nucleus potential. Polarized target, DWIA calculations.
doi: 10.1103/PhysRevC.64.064606
1997MA68 Phys.Rev. C56, 3210 (1997) R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, W.Bertozzi, T.Chittrakarn, J.R.Comfort, J.M.Finn, C.C.Foster, C.Hyde-Wright, J.J.Kelly, C.Lebo, H.Orihara, W.Pairsuwan, J.W.Watson 0+ to 0- Transition in the 16O(p, n)16F Reaction at 79 MeV NUCLEAR REACTIONS 16O(p, n), E=79 MeV; measured σ(θ, En), σ(θ). Comparison with DWIA calculations.
doi: 10.1103/PhysRevC.56.3210
1996RA05 Phys.Rev. C53, 1005 (1996) B.A.Raue, T.A.Greco, M.G.Khayat, F.Adimi, B.van den Brandt, H.Breuer, T.Chang, N.S.Chant, H.Chen, T.A.Dooling, A.P.Dvoredsky, B.S.Flanders, T.Gu, J.P.Haas, P.Hautle, J.Huffman, J.J.Kelly, A.Klein, K.Koch, J.A.Konter, A.I.Kovalev, G.S.Kyle, J.J.Lawrie, Z.Lin, S.Mango, P.Markowitz, R.Meier, T.Payerle, S.Ritt, P.G.Roos, M.Wang Analyzing Powers for 1H(pol)(π+, π+p) at T(π) = 165 and 240 MeV NUCLEAR REACTIONS 1H(π+, π+p), E=165, 240 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevC.53.1005
1995PA37 Phys.Rev. C52, 2552 (1995) W.Pairsuwan, J.W.Watson, M.Ahmad, N.S.Chant, B.S.Flanders, R.Madey, P.J.Pella, P.G.Roos Analyzing Powers for the 2H(p(pol), pn)1H Reaction at 200 MeV NUCLEAR REACTIONS 2H(polarized p, np), E=200 MeV; measured σ(θp, θn, Ep), analyzing power vs θ.
doi: 10.1103/PhysRevC.52.2552
1994BR10 Phys.Rev. C49, R2276 (1994) H.Breuer, M.G.Khayat, F.Adimi, B.S.Flanders, M.A.Khandaker, P.G.Roos, D.Zhang, Th.S.Bauer, J.Konijn, C.T.A.M.de Laat, G.S.Kyle, S.Mukhopadhyay, M.Wang, R.Tacik Excitation Function for 4He(π+, pp)2H Two-Nucleon Absorption Across the Δ Resonance NUCLEAR REACTIONS 4He(π+, 2p), E=64-327 MeV; measured σ(θ), σ(E) for 2-nucleon production; deduced reaction mechanism. Quasideuteron model.
doi: 10.1103/PhysRevC.49.R2276
1994ED01 Phys.Rev. C50, R1749 (1994) T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, M.Farkhondeh, J.M.Finn, B.S.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, D.M.Manley, P.Markowitz, J.Mougey, B.Ni, T.Payerle, P.J.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney Electric Form Factor of the Neutron from the 2H(e(pol), e'n(pol))1H Reaction at Q2 = 0.255 (GeV/c)2 NUCLEAR REACTIONS 2H(polarized e, e'n), E=868 MeV; measured neutron polarization. 1n deduced electric form factor.
doi: 10.1103/PhysRevC.50.R1749
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
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
1993MA21 Phys.Rev. C48, R5 (1993) P.Markowitz, J.M.Finn, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, T.Eden, M.Farkhondeh, B.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, R.Madey, D.M.Manley, J.Mougey, B.Ni, T.Payerle, P.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney, W.M.Zhang Measurement of the Magnetic Form Factor of the Neutron NUCLEAR REACTIONS 2H(e, e'n), E not given; measured en-coin. 1n deduced magnetic form factor. Associated particle technique.
doi: 10.1103/PhysRevC.48.R5
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
1992AD03 Phys.Rev. C45, 2589 (1992) F.Adimi, H.Breuer, B.S.Flanders, M.A.Khandaker, M.G.Khayat, P.G.Roos, D.Zhang, Th.S.Bauer, J.Konijn, C.T.A.M.de Laat, G.S.Kyle, S.Mukhopadhyay, M.Wang, R.Tacik Two-Nucleon Absorption of π+ in 4He at T(π+) = 114 and 162 MeV NUCLEAR REACTIONS 4He(π+, 2p), E=114, 162 MeV; measured missing momentum distribution, pp(φ), σ(θp); deduced absorption on two-nucleon σ. Quasideuteron absorption model, Monte Carlo simulations.
doi: 10.1103/PhysRevC.45.2589
1991FL01 Phys.Rev. C43, 2103 (1991) B.S.Flanders, J.J.Kelly, H.Seifert, D.Lopiano, B.Aas, A.Azizi, G.Igo, G.Weston, C.Whitten, A.Wong, M.V.Hynes, J.McClelland, W.Bertozzi, J.M.Finn, C.E.Hyde-Wright, R.W.Lourie, B.E.Norum, P.Ulmer, B.L.Berman Empirical Density-Dependent Effective Interaction for Nucleon-Nucleus Scattering at 500 MeV NUCLEAR REACTIONS 16O(polarized p, p), E=498 MeV; measured σ(θ) analyzing power, spin rotation function, depolarization parameters. 40Ca(polarized p, p'), (polarized p, p), E=500 MeV; analyzed data; deduced density dependent empiricial effective interaction. Compared with nonrelativistic effective interactions, relativistic optical potentials.
doi: 10.1103/PhysRevC.43.2103
1991GO14 Phys.Rev.Lett. 66, 2193 (1991) J.J.Gorgen, J.R.Comfort, J.R.Tinsley, T.Averett, J.DeKorse, G.Franklin, B.G.Ritchie, G.Kyle, A.Klein, B.Berman, G.Burleson, K.Cranston, J.A.Faucett, J.J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.-F.Yen, S.Hoibraten, H.Breuer, B.S.Flanders, M.A.Khandaker, D.L.Naples, D.Zhang, M.L.Barlett, G.W.Hoffmann, M.Purcell Analyzing Powers for Pion Charge Exchange on Polarized 13C NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.2193
1991KE02 Phys.Rev. C43, 1272 (1991) J.J.Kelly, A.E.Feldman, B.S.Flanders, H.Seifert, D.Lopiano, B.Aas, A.Azizi, G.Igo, G.Weston, C.Whitten, A.Wong, M.V.Hynes, J.McClelland, W.Bertozzi, J.M.Finn, C.E.Hyde-Wright, R.W.Lourie, P.E.Ulmer, B.E.Norum, B.L.Berman Effective Interaction for 16O(p, p') at E(p) = 318 MeV NUCLEAR REACTIONS 16O(polarized p, p'), (polarized p, p), E=318 MeV; measured σ(θ), analyzing power vs θ; deduced empirical effective interaction. Folding model analysis, density dependence.
doi: 10.1103/PhysRevC.43.1272
1991KE09 Phys.Rev. C44, 1963 (1991) J.J.Kelly, M.A.Khandaker, P.Boberg, A.E.Feldman, B.S.Flanders, S.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Neutron and Proton Transition Densities from 32,34S(p, p') at E(p) = 318 MeV. I. Isoscalar Densities for 32S NUCLEAR REACTIONS 32,34S(polarized p, p'), E=318 MeV; measured σ(θ), analyzing powers. 32S levels deduced isoscalar transition densities. DWIA analysis. Shell model.
doi: 10.1103/PhysRevC.44.1963
1991KE13 Phys.Rev. C44, 2602 (1991) J.J.Kelly, P.Boberg, A.E.Feldman, B.S.Flanders, M.A.Khandaker, S.D.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Effective Interaction for 40Ca(p, p') at E(p) = 318 MeV NUCLEAR REACTIONS 40Ca(polarized p, p'), (polarized p, p), E=318 MeV; measured σ(θ), analyzing power vs θ; deduced nucleon-nucleon effective interaction. Dirac phenomenology, global optical potentials.
doi: 10.1103/PhysRevC.44.2602
1991KH06 Phys.Rev. C44, 1978 (1991) M.A.Khandaker, J.J.Kelly, P.Boberg, A.E.Feldman, B.S.Flanders, S.Hyman, H.Seifert, P.Karen, B.E.Norum, P.Welch, S.Nanda, A.Saha Neutron and Proton Transition Densities from 32,34S(p, p') at E(p) = 318 MeV. II. Neutron Densities for 34S NUCLEAR REACTIONS 32,34S(polarized p, p'), E=318 MeV; measured σ(θ), analyzing powers. 34S levels deduced isoscalar transition densities, neutron, proton transition matrix elements ratio. DWIA analysis. Shell model.
doi: 10.1103/PhysRevC.44.1978
1990GO36 J.Phys.(Paris), Colloq.C-6, 583 (1990) J.Gorgen, J.Comfort, T.Averett, J.DeKorse, G.Franklin, B.Ritchie, J.Tinsley, G.Kyle, B.Berman, G.R.Burleson, K.Cranston, A.Klein, J.A.Faucett, J.Jarmer, J.N.Knudson, S.Penttila, N.Tanaka, B.Brinkmoller, D.Dehnhard, Y.F.Yen, H.Breuer, M.A.Khandaker, D.L.Naples, B.S.Flanders, D.Zhang, M.Barlett, G.W.Hoffmann, M.Purcell, S.Hoibraten Analyzing Power Measurements for the (π+, π0) Reaction on a Polarized 13C Target at T(π+) = 163 MeV NUCLEAR REACTIONS 13C(π+, π0), E=163 MeV; measured σ(θ), analyzing power vs θ. Polarized target. DWIA analyses.
1989FL01 Phys.Rev. C40, 1985 (1989) B.S.Flanders, R.Madey, B.D.Anderson, A.R.Baldwin, J.W.Watson, C.C.Foster, H.V.Klapdor, K.Grotz Gamow-Teller Strength in the 208Pb(p, n)208Bi Reaction at 134.4 MeV NUCLEAR REACTIONS 208Pb(p, n), E=134.3 MeV; measured σ(En). 208Bi deduced Gamow-Teller transition strength distribution.
doi: 10.1103/PhysRevC.40.1985
1989MA35 Phys.Rev. C40, 540 (1989) R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, J.W.Watson, S.M.Austin, C.C.Foster, H.V.Klapdor, K.Grotz Low-Lying Structures in the Gamow-Teller Strength Functions for the Double-Beta-Decaying Nuclei 76Ge, 82Se, 128Te, and 130Te NUCLEAR REACTIONS 76Ge, 82Se, 128,130Te(p, n), E=134.4 MeV; measured neutron spectra at θ ≤ 8°. 76As, 82Br, 128,130I deduced Gamow-Teller transition strengths. Shell model comparison.
doi: 10.1103/PhysRevC.40.540
1989WA17 Phys.Rev. C40, 570 (1989) J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.D.Brown, C.C.Foster, D.L.Friesel, H.Nann, E.J.Stephenson, P.B.Foot, G.G.Shute, B.M.Spicer 48Ca(d, n)49Sc Reaction at 79 MeV NUCLEAR REACTIONS 48Ca(polarized d, n), E=79 MeV; measured σ(En), σ(θ), vector analyzing power; deduced model parameters. 49Sc levels deduced C2S. DWBA, Johnson-Soper adiabatic approximation analyses.
doi: 10.1103/PhysRevC.40.570
1988SC14 Phys.Rev. C38, 2205 (1988) R.A.Schumacher, P.A.Amaudruz, C.H.Q.Ingram, U.Sennhauser, H.Breuer, N.S.Chant, A.E.Feldman, B.S.Flanders, F.Khazaie, D.J.Mack, P.G.Roos, J.D.Silk, G.S.Kyle Exclusive Quasi-Deuteron Absorption of Pions in 16O and 18O at 116 MeV NUCLEAR REACTIONS 18,16O(π+, 2p), E=116 MeV; measured σ(E(2p)), σ(θ1, θ2), σ(θ1, θ2, E1); deduced reaction mechanism.
doi: 10.1103/PhysRevC.38.2205
1987FO22 Aust.J.Phys. 40, 611 (1987) P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, J.D.Brown, D.L.Friesel, H.Nann, J.W.Seubert, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, W.Pairsuwan, J.W.Watson D State Effects in the 11B(d(pol), n)12C Reaction at 79 MeV NUCLEAR REACTIONS 11B(polarized d, n), E=79 MeV; measured σ(θ), vector analyzing power vs θ; deduced 2H D-state effects role. DWBA analysis.
1987MA19 Phys.Rev. C35, 2011 (1987); Erratum Phys.Rev. C36, 1647 (1987) R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, C.Lebo, J.W.Watson, S.M.Austin, A.Galonsky, B.H.Wildenthal, C.C.Foster Gamow-Teller Strength in the 26Mg(p, n)26Al Reaction at 135 MeV and Its Fractionation into T=0, 1, and 2 Isospin Channels NUCLEAR REACTIONS, MECPD 26Mg(p, n), E=134.4 MeV; measured σ(En); deduced σ(θ). 26Al deduced levels, J, π, T, Gamow-Teller transition strength distribution. Tof. DWIA.
doi: 10.1103/PhysRevC.35.2011
1986WA28 Phys.Lett. 181B, 47 (1986) J.W.Watson, P.J.Pella, B.D.Anderson, A.R.Baldwin, T.Chittrakarn, B.S.Flanders, R.Madey, C.C.Foster, I.J.van Heerden Gamow-Teller and Spin-Dipole Strength in the 40,48Ca(p(pol), n(pol)) Reactions at 135 MeV NUCLEAR REACTIONS, MECPD 40,48Ca(polarized p, n), E=135 MeV; measured σ(En, θ), spin flip probabilities, neutron polarization vs θ, polarization transfer coefficient. 48Ca deduced 1+ strength in continuum near giant Gamow-Teller resonance. 40Ca deduced dipole resonance spin-flip, nonspin-flip component relative width.
doi: 10.1016/0370-2693(86)91252-9
1985FO05 Phys.Rev. C31, 1133 (1985) P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, H.Nann, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.W.Watson 11B(d, n)12C Reaction and the Adiabatic Approximation NUCLEAR REACTIONS 11B(d, n), E=79 MeV; measured σ(θ); deduced deuteron optical model parameters. 12C levels deduced L, S. Adiabatic model, DWBA analysis.
doi: 10.1103/PhysRevC.31.1133
1985WA24 Phys.Rev.Lett. 55, 1369 (1985) J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, R.J.McCarthy, B.A.Brown, B.H.Wildenthal, C.C.Foster Relationship between Gamow-Teller Transition Proabilities and (p, n) Cross Sections at Small Momentum Transfers NUCLEAR REACTIONS 14C, 15N, 17,18O, 26Mg, 39K(p, n), E=135 MeV; measured σ(θ), σ(θn, En). 13C, 19F(p, n), E=160 MeV; analyzed σ(θ). 14N, 15O, 17,18F, 26Al, 39Ca levels deduced Gamow-Teller transitions. DWBA analysis, β-decay input.
doi: 10.1103/PhysRevLett.55.1369
1984AH04 Nucl.Phys. A424, 92 (1984) M.Ahmad, J.W.Watson, D.W.Devins, B.S.Flanders, D.L.Friesel, N.S.Chant, P.G.Roos, J.Wastell Neutron-Knockout Reactions from 2H, 40Ca and 48Ca NUCLEAR REACTIONS 2H, 40,48Ca(p, np), E=149.5 MeV; measured pn-coin, σ(θp, Ep, θn). 40,48Ca deduced neutron hole state spectroscopic factors C2S, rms radii. PWIA, DWIA analysis.
doi: 10.1016/0375-9474(84)90130-1
1984WA21 J.Phys.(Paris), Colloq.C-4, 91 (1984) J.W.Watson, P.J.Pella, M.Ahmad, B.S.Flanders, N.S.Chant, P.G.Roos, D.W.Devins, D.L.Friesel Neutron Deep-Hole States from the (p, pn) Reaction NUCLEAR REACTIONS 2H, 9Be, 16O, 28Si, 58Ni, 90Zr(polarized p, np), E=148.8 MeV; measured separation energy spectra, σ(Ep, θp, θn), analyzing powers. 8Be, 15O, 27Si, 57Ni, 89Zr deduced tentative deep-hole neutron states. Si, Ge detectors, tof. DWIA calculations.
1983FR10 Nucl.Instrum.Methods 207, 403 (1983) D.L.Friesel, B.S.Flanders, R.H.Pehl A Variable Geometry High-Purity Germanium Detector Telescope System for use with Intermediate Energy Charged Particles NUCLEAR REACTIONS 62Ni(p, p'), (p, d), (p, t), E=60 MeV; 28Si(p, p'), E=115 MeV; 12C(3He, t), E=200 MeV; measured σ(Ep'), σ(Ed), σ(Et); 40Ca(p, 2p), E=150 MeV; measured pp-coin. Variable geometry telescope detector system.
doi: 10.1016/0167-5087(83)90651-8
1983GR16 Phys.Lett. 126B, 417 (1983) K.Grotz, H.V.Klapdor, J.Metzinger, R.Madey, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.Flanders, C.Lebo, J.W.Watson, C.C.Foster The Gamow-Teller Strength Distribution in 208Bi - A Probe of the Charge Distribution in 208Pb ( Question ) NUCLEAR STRUCTURE 208Bi; calculated Gamow-Teller transition strength distribution. Two-quasiparticle formalism, comparison with (p, n) data. NUCLEAR REACTIONS 208Pb(p, n), E=134.4 MeV; measured σ(θ). 208Pb deduced ground state correlation effects, single particle orbit occupation probabilities. Comparison with Gamow-Teller strength calculations.
doi: 10.1016/0370-2693(83)90353-2
1983WA29 Nucl.Instrum.Methods 215, 413 (1983) J.W.Watson, B.D.Anderson, A.R.Baldwin, C.Lebo, B.Flanders, W.Pairsuwan, R.Madey, C.C.Foster A Comparison of Methods for Determining Neutron Detector Efficiencies at Medium Energies NUCLEAR REACTIONS 7Li, 12C(p, n), E=135, 160 MeV; measured σ(θ). Lithium activation method, comparison to other techniques, neutron detector efficiency determination.
doi: 10.1016/0167-5087(83)90472-6
1982WA17 Phys.Rev. C26, 961 (1982) J.W.Watson, M.Ahmad, D.W.Devins, B.S.Flanders, D.L.Friesel, N.S.Chant, P.G.Roos, J.Wastell 40Ca(p, pn)39Ca and 48Ca(p, pn)47Ca Neutron Knockout Reactions at 149.5 MeV NUCLEAR REACTIONS 40,48Ca(p, np), E=149.5 MeV; measured σ(θp, θn, Ep), pn-coin. 39,47Ca levels deduced C2S. DWIA analysis.
doi: 10.1103/PhysRevC.26.961
1979BO18 Phys.Rev. C20, 641 (1979) P.Bonche, K.T.R.Davies, B.Flanders, H.Flocard, B.Grammaticos, S.E.Koonin, S.J.Krieger, M.S.Weiss Time-Dependent Hartee-Fock Calculations of Fusion Cross Sections for 16O + 40Ca and 28Si + 28Si NUCLEAR REACTIONS 16O(40Ca, X), E(cm)=30-250 MeV; 28Si(28Si, X), E(cm)=35-250 MeV; calculated fusion σ; deduced angular momentum fusion window. Time-dependent Hartree-Fock, Skyrme interaction.
doi: 10.1103/PhysRevC.20.641
1978KO22 Phys.Lett. 77B, 13 (1978) S.Koonin, B.Flanders, H.Flocard, M.Weiss A Separable Approximation to Time-Dependent Hartree-Fock Calculations NUCLEAR REACTIONS 16O(16O, 16O), 40Ca(40Ca, 40Ca); calculated reaction parameters.
doi: 10.1016/0370-2693(78)90188-0
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