NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.S.Mackintosh Found 115 matches. Showing 1 to 100. [Next]2024MA11 Phys.Rev. C 109, 034605 (2024) Stripping and pickup contributions to the optical potentials for 3H and 3He on 40Ca
doi: 10.1103/PhysRevC.109.034605
2023KE03 Phys.Rev. C 107, 034602 (2023) Reaction channel contributions to the triton + 208Pb optical potential NUCLEAR REACTIONS 208Pb(t, α), (t, t), E=33 MeV; calculated σ(θ); deduced optical potential parameters, dynamical polarization potentials (DPP). Identified the influence of dynamically nonlocality due to various channel couplings. Comparison with 208Pb(3He, α), (3He, 3He') reactions. Coupled reaction channel (CRC) calculations.
doi: 10.1103/PhysRevC.107.034602
2022MA55 Phys.Rev. C 106, 054611 (2022) Reaction channel contributions to the proton + 208Pb optical potential at 40 MeV NUCLEAR REACTIONS 208Pb(p, d), (p, p'), E=40 MeV; calculated σ(θ), analyzing power; deduced optical potential parameters, dynamical polarization potentials (DPP). Identified the influence of dynamically generated nonlocality due to various channel couplings. Coupled reaction channel (CRC) calculations.
doi: 10.1103/PhysRevC.106.054611
2021MA69 Phys.Rev. C 104, 044616 (2021) Reaction channel contributions to proton scattering at 65 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p), (p, p), E=65 MeV; 40Ca(p, d)39Ca, E=65 MeV; calculated σ(θ), analyzing power iT11(θ); deduced optical potential parameters, dynamical polarization potentials (DPP) for elastic scattering and neutron pickup reaction; deduced that no smoothly varying global OMP could fit proton elastic scattering from both 40Ca and 48Ca, and that breakup of deuteron must be included in calculations of the DPP due to neutron pickup in proton scattering. Coupled reaction channel (CRC) calculations for neutron pickup and coupled channel (CC) calculations for collective states, with l-independent representation of the dynamical polarization potential (DPP).
doi: 10.1103/PhysRevC.104.044616
2020KE10 Phys.Rev. C 102, 064611 (2020) Reaction channel contributions to the triton optical potential NUCLEAR REACTIONS 16O, 40Ca(t, t), (t, t'), (t, α), E=33 MeV; calculated differential σ(θ), analyzing powers Ay(θ), dynamical polarization potentials (DPPs) by coupling to pickup and inelastic channels; deduced undulatory features in the DPPs. Coupled channel (CC) and coupled reaction channel (CRC) calculations using the FRESCO code. Comparison of σ(θ) calculations with experimental data.
doi: 10.1103/PhysRevC.102.064611
2019KE05 Phys.Rev. C 99, 034614 (2019) Pickup coupling contribution to the optical model potential for 30.3 MeV protons and neutrons on 40Ca NUCLEAR REACTIONS 40Ca(n, n), (p, p), E=25, 30.3, 35, 40, 45 MeV; calculated volume integrals of the four components of the dynamic polarization potentials (DPP) induced by (p, d) and (n, d) couplings, change in rms radius of the real central component, change in the total reaction cross section induced by couplings to various states in 39Ca and 39K, the integrated cross section to the specific coupled reaction channels, radial real central, imaginary central, real spin-orbit, and imaginary spin-orbit components of the DPP. Coupled reaction channel (CRC) calculations using the FRESCO code.
doi: 10.1103/PhysRevC.99.034614
2019MA68 Eur.Phys.J. A 55, 147 (2019) The angular momentum dependence of nuclear optical potentials NUCLEAR REACTIONS 16O(p, p), (p, p'), E=30.1 MeV;40Ca(p, p), (p, p'), E=30.3 MeV;40Ca(d, d), (d, d'), E=52 MeV; calculated optical potential components (volume real, volume-imaginary, spinorbit-real, spinorbit-imaginary) of l-independent equivalent of the full l-independent potential of published calculations; calculated Dynamic Polarization Potential (DPP) for scattering of loosely bound nuclei.
doi: 10.1140/epja/i2019-12830-3
2019MA83 Phys.Rev. C 100, 064613 (2019) Reaction channel contributions to the helion optical potential NUCLEAR REACTIONS 16O(3He, 3He), (3He, 3He'), (3He, α), E=32 MeV; 40Ca, 208Pb(3He, 3He), (3He, 3He'), (3He, α), E=33 MeV; calculated σ(θ), Ay(θ), dynamical polarization potentials (DPPs) by coupling to pickup and inelastic channels; deduced undulatory features in the DPPs. Coupled channel (CR) and coupled reaction channel (CRC) calculations using the FRESCO code. Comparison of σ(θ) and Ay(θ) calculations with experimental data.
doi: 10.1103/PhysRevC.100.064613
2019PH03 Phys.Rev. C 100, 054615 (2019) N.T.T.Phuc, R.S.Mackintosh, N.H.Phuc, D.T.Khoa Elastic transfer and parity dependence of the nucleus-nucleus optical potential NUCLEAR REACTIONS 12C(16O, 16O), (16O, X), E=132, 300 MeV; calculated σ(θ, E) for ground-state channels of 16O and 12C using coupled reaction channel (CRC) approach with two- and ten-channel model space calculated parity-dependent core exchange potential (CEP) from S-matrix using inversion method; deduced strong contribution by the complex Majorana term in the total optical potential (OP).
doi: 10.1103/PhysRevC.100.054615
2018KE01 Phys.Rev. C 97, 014605 (2018) Reaction channel coupling effects for nucleons on 16O: Induced undularity and proton-neutron potential differences NUCLEAR REACTIONS 16O(p, p), (n, n), E=30.1 MeV; calculated σ(θ), Ay(θ), phase shifts, and compared with experimental data; calculated dynamical polarization potentials (DPPs) by coupling to pickup channels; deduced undulatory features in the DPPs, and compared with corresponding features of empirical optical model potentials (OMPs). Coupled channel (CR) and coupled reaction channel (CRC) calculations using FRESCO code by including couplings to the 6.13 MeV, 3- state and 22 MeV, 2+ GQR in 16O.
doi: 10.1103/PhysRevC.97.014605
2018MA52 Phys.Rev. C 98, 024624 (2018) Remarkable independence of dynamical polarization potentials of the underlying potential NUCLEAR REACTIONS 40Ca(polarized p, p), E=30.3 MeV; analyzed Ay(θ) data with the inclusion of coupling to the 3/2+ ground state of 39Ca in a search for the conventional Wood-Saxon parameters, dynamical polarization potentials (DPP) with coupling to the 3/2+ g.s. and 5/2+ lumped state in 39Ca; deduced that DPP caused by coupling to pickup channels is qualitatively and almost quantitatively unaffected by substantial changes in the bare potential.
doi: 10.1103/PhysRevC.98.024624
2017MA06 Phys.Rev. C 95, 024602 (2017) G.Marquinez-Duran, N.Keeley, K.W.Kemper, R.S.Mackintosh, I.Martel, K.Rusek, A.M.Sanchez-Benitez Influence of single-neutron stripping on near-barrier 6He 208Pb and 8He + 208Pb elastic scattering NUCLEAR REACTIONS 208Pb(6He, 6He), (8He, 8He), E=22 MeV; analyzed σ(θ) data, total reaction cross sections for the bare and summed 1n-stripping cross sections; deduced optical model parameters, dynamic polarization potentials, and effect of single-neutron stripping on elastic scattering. Coupled reaction channels (CRC) and S-matrix calculations.
doi: 10.1103/PhysRevC.95.024602
2017MA19 Eur.Phys.J. A 53, 66 (2017) Elastic scattering phenomenology
doi: 10.1140/epja/i2017-12257-x
2016MA52 Phys.Rev. C 94, 034602 (2016) Evidence for L-dependence generated by channel coupling: 16O scattering from 12C at 115.9 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=115.9 MeV; calculated σ(θ), elastic channel S matrix from existing coupled channel (CC) calculations inverted; deduced angular momentum dependence of optical potentials.
doi: 10.1103/PhysRevC.94.034602
2015MA12 Phys.Rev. C 91, 024616 (2015) R.S.Mackintosh, Y.Hirabayashi, S.Ohkubo Emergence of a secondary rainbow and the dynamical polarization potential for 16O on 12C at 330 MeV NUCLEAR REACTIONS 12C(16O, 16O), E≈300 MeV; analyzed dynamic polarization potential (DPP) and secondary rainbow effect using S-matrix to potential, SL to V(r) inversion, and coupled channel calculations; deduced effect of direct coupling between the collective states of 12C and 16O. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024616
2014KE05 Phys.Rev. C 90, 044602 (2014) Dynamic polarization potential and dynamical nonlocality in nuclear potentials: Nucleon-nucleus potential NUCLEAR REACTIONS 40Ca(p, d), (n, d), E=30.3 MeV; calculated angular distributions; deduced dynamical polarization potential (DPP); investigated effects of non-locality induced by phonon couplings. Coupled-channel (CC) and distorted wave Born approximations (DWBA) calculations.
doi: 10.1103/PhysRevC.90.044602
2014MA83 Phys.Rev. C 90, 044601 (2014) Phonon coupling effects in proton scattering from 40Ca NUCLEAR REACTIONS 40Ca(p, p), (p, p'), E=20-90 MeV; calculated dynamical polarization potential (DPP) with full coupling to the GQR, 3- state and multi-phonon states, inelastic scattering σ(E); deduced l-dependent undulatory nature of the contribution of phonon coupling. S-matrix to potential inversion method for coupled channel and optical model potential calculations.
doi: 10.1103/PhysRevC.90.044601
2013MA55 Phys.Rev. C 88, 014608 (2013) Significant features of 8B scattering from 208Pb at 170.3 MeV NUCLEAR REACTIONS 208Pb(8B, 8B), E=170.3 MeV; calculated CDCC breakup S-matrix inversion, σ(θ); deduced dynamic polarization potentials. Continuum discretized coupled channels (CDCC) calculations. Discussed anomalous behavior.
doi: 10.1103/PhysRevC.88.014608
2013MA82 Phys.Rev. C 88, 054603 (2013) Interpreting increases in |SL| due to channel coupling NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=19.04 MeV; 58Ni(7Be, 7Be), E=24.12 MeV; 58Ni(8B, 8B), E=29.26 MeV; 208Pb(6He, 6He), E=66 MeV; calculated σ(θ), change in reaction σ due to breakup coupling and breakup cross section, elastic scattering S matrix SL, dynamic polarization potential (DPP) due to breakup coupling, wrong way (WW) effect. Continuum discretized coupled channel (CDCC) calculations.
doi: 10.1103/PhysRevC.88.054603
2012MA22 Phys.Rev. C 85, 064603 (2012), Erratum Phys.Rev. C 97, 069901 (2018) Coupling effects in proton scattering from 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p), E=30.3 MeV; calculated dynamic polarization potential (DPP), analyzing powers, effect of (p, d) pickup couplings. Coupled reaction channel (CRC) calculations.
doi: 10.1103/PhysRevC.85.064603
2012MA47 Phys.Rev. C 86, 047602 (2012) Increase in lSLl induced by channel coupling: The case of deuteron breakup NUCLEAR REACTIONS 58Ni(d, d), E=56, 79, 120 MeV; calculated elastic scattering matrix magnitude, σ(θ), dynamic polarization potentials (DPP) induced by S-wave and d-wave breakup (BU). Continuum discretized coupled channels (CDCC) calculations. Anomalous effect of couplings on S-matrix, relation of non-locality of optical model potentials. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.047602
2011KE02 Phys.Rev. C 83, 044608 (2011) Dynamic polarization potential due to pickup coupling for proton scattering from 6He NUCLEAR REACTIONS 6,8He(p, d), E=71 MeV/nucleon; calculated dynamic polarization potentials (DPP), σ(θ), Ay(θ) using coupled-channel analysis. Influence of deuteron breakup.
doi: 10.1103/PhysRevC.83.044608
2011MA38 Phys.Rev. C 83, 057601 (2011) Addendum to "Strong coupling effects in proton scattering from 8He" NUCLEAR REACTIONS 8He(p, p), E=25, 61.3 MeV/nucleon; analyzed σ(θ) and analyzing powers, radial dependence of dynamic polarization potentials (DPP) using the continuum-discretized coupled channels (CDCC) formalism applied to the (p, d) coupling channels. Breakup of the outgoing deuteron.
doi: 10.1103/PhysRevC.83.057601
2011PA37 Phys.Rev. C 84, 064611 (2011) Dynamic polarization potential due to 6Li breakup on 12C NUCLEAR REACTIONS 12C(6Li, 6Li), E=90-318 MeV; calculated σ(E, θ), breakup coupling, energy dynamic of dynamic polarization potentials (DPP), S-matrix inversion compared with trivially equivalent local potential (TELP). Continuum discretized coupled-channels (CDCC) formalism with a two-body cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064611
2010KE06 Nucl.Phys. A834, 792c (2010) N.Keeley, R.S.Mackintosh, C.Beck Breakup Coupling Effects on Near-Barrier 6Li, 7Be and 8B + 58Ni Elastic Scattering Compared NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=19.4 MeV; 58Ni(7Be, 7Be), E=24.12 MeV; 58Ni(8B, 8B), E=29.26 MeV; calculated σ(θ) using CDCC code FRESCO; deduced L-dependence of S-matrix, effect of coupling.
doi: 10.1016/j.nuclphysa.2010.01.148
2010MA17 Phys.Rev. C 81, 034612 (2010) Strong coupling effects in proton scattering from 8He NUCLEAR REACTIONS 8He(p, p), (polarized p, p)E=15.66, 25, 61.3 MeV/nucleon; calculated differential σ(θ), analyzing powers; deduced dynamic polarization potentials (DPP) using coupled reaction channel (CRC) model with influence of deuteron coupling on proton scattering and including coupling to the triton partition.
doi: 10.1103/PhysRevC.81.034612
2009MA03 Phys.Rev. C 79, 014611 (2009) 6He breakup dynamic polarization potential reexamined NUCLEAR REACTIONS 208Pb(6He, X), E=22, 27, 32 MeV; calculated dynamic polarization potentials. Continuum-discretized coupled channels calculations.
doi: 10.1103/PhysRevC.79.014611
2008KE05 Phys.Rev. C 77, 054603 (2008) Pickup coupling effects in deuteron scattering: The case of d + 40Ca NUCLEAR REACTIONS 40Ca(d, 3He), (d, α), (d, t), (d, d), (d, p), E=52 MeV; calculated spectroscopic factors, σ(θ), rms radii, dynamic polarization parameters. Coupled reaction channels calculations followed by S-matrix approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.054603
2007MA59 Phys.Rev. C 76, 024601 (2007) Strong pickup-channel coupling effects in proton scattering: The case of p+10Be
doi: 10.1103/PhysRevC.76.024601
2005GI07 Phys.Rev. C 71, 064311 (2005) L.Giot, P.Roussel-Chomaz, C.E.Demonchy, W.Mittig, H.Savajols, N.Alamanos, F.Auger, A.Gillibert, C.Jouanne, V.Lapoux, L.Nalpas, E.C.Pollacco, J.L.Sida, F.Skaza, M.D.Cortina-Gil, J.Fernandez-Vazquez, R.S.Mackintosh, A.Pakou, S.Pita, A.Rodin, S.Stepantsov, G.M.Ter-Akopian, K.Rusek, I.J.Thompson, R.Wolski Investigation of 6He cluster structures NUCLEAR REACTIONS 1H(6He, α), E=25 MeV/nucleon; measured σ(θ); deduced particle transfer contributions, entrance potential dependence. 6He deduced spectroscopic factors for t+t and α+2n cluster configurations. 1H(6He, p), E=25 MeV/nucleon; measured σ(θ). 3He(α, α), E(cm)=28.7 MeV; calculated σ(θ). SPEG spectrometer and MUST array at GANIL. DWBA and coupled-channels calculations.
doi: 10.1103/PhysRevC.71.064311
2005GI18 Eur.Phys.J. A 25, Supplement 1, 267 (2005) L.Giot, P.Roussel-Chomaz, N.Alamanos, F.Auger, M.-D.Cortina-Gil, Ch.E.Demonchy, J.Fernandez, A.Gillibert, C.Jouanne, V.Lapoux, R.S.Mackintosh, W.Mittig, L.Nalpas, A.Pakou, S.Pita, E.C.Pollacco, A.Rodin, K.Rusek, H.Savajols, J.L.Sida, F.Skaza, S.Stepantsov, G.Ter-Akopian, I.Thompson, R.Wolski Study of the ground-state wave function of 6He via the 6He(p, t)α transfer reaction NUCLEAR REACTIONS 1H(6He, α), E=25 MeV/nucleon; measured σ(θ); deduced particle transfer contributions, entrance potential dependence. 6He deduced spectroscopic factors for t+t and a+2n cluster configurations. SPEG spectrometer and MUST array at GANIL. DWBA and coupled-channels calculations.
doi: 10.1140/epjad/i2005-06-021-5
2005KE03 Phys.Rev. C 71, 057601 (2005) Breakup dynamic polarization potential for 6He + 208Pb: Energy dependence and generic properties NUCLEAR REACTIONS 208Pb(6He, X), E=27, 40, 53, 66 MeV; calculated dynamic polarization potential.
doi: 10.1103/PhysRevC.71.057601
2005SK03 Phys.Lett. B 619, 82 (2005) F.Skaza, N.Keeley, V.Lapoux, N.Alamanos, F.Auger, D.Beaumel, E.Becheva, Y.Blumenfeld, F.Delaunay, A.Drouart, A.Gillibert, L.Giot, K.W.Kemper, R.S.Mackintosh, L.Nalpas, A.Pakou, E.C.Pollacco, R.Raabe, P.Roussel-Chomaz, J.-A.Scarpaci, J.-L.Sida, S.Stepantsov, R.Wolski Important pickup coupling effect on 8He(p, p) elastic scattering NUCLEAR REACTIONS 1H(8He, p), (8He, d), E=15.7 MeV/nucleon; measured deuteron and proton spectra, σ(θ). 8He(p, p), E=15.7 MeV/nucleon; deduced effect of coupling to pickup reaction. Coupled-channels framework, dynamic polarization potential.
doi: 10.1016/j.physletb.2005.05.061
2004KU02 J.Phys.(London) G30, R1 (2004) The application of inversion to nuclear scattering
doi: 10.1088/0954-3899/30/R01
2004MA70 Nucl.Phys. A742, 3 (2004) The p + 6He interaction from Ec.m. = 0.5 to 25 MeV NUCLEAR REACTIONS 6He(p, X), 6Li(n, X), E(cm)=0.5-25 MeV; calculated interaction potentials. S-matrix inversion, resonating group model.
doi: 10.1016/j.nuclphysa.2004.06.002
2004MA72 Phys.Rev. C 70, 024604 (2004) Breakup dynamic polarization potential for 6He+208Pb at 27 MeV NUCLEAR REACTIONS 208Pb(6He, X), E=27 MeV; calculated dynamic polarization potential.
doi: 10.1103/PhysRevC.70.024604
2003CO08 Nucl.Phys. A723, 45 (2003) Data-to-potential inversion for tensor polarized deuterons scattered from 4He NUCLEAR REACTIONS 4He(polarized d, d), E=4-13 MeV; analyzed σ(θ), analyzing powers; deduced potential. Iterative perturbative procedure.
doi: 10.1016/S0375-9474(03)01082-0
2003HE02 Nucl.Phys. A713, 63 (2003) H.Heiberg-Andersen, R.S.Mackintosh, J.S.Vaagen A new phenomenological τ-α interaction NUCLEAR REACTIONS 4He(3He, 3He), E=20-30 MeV; calculated σ(θ), analyzing powers, parity dependence features, three-nucleon exchange process. 7Be deduced level energy. Phenomenological interaction, comparisons with data.
doi: 10.1016/S0375-9474(02)01291-5
2003MA08 Phys.Rev. C 67, 034607 (2003) Dynamic polarization potential for 6He+p due to breakup NUCLEAR REACTIONS 1H(6He, 6He), E(cm)=21.57, 35.06 MeV; calculated σ(θ), breakup contribution to dynamic polarization potential. Iterative-perturbative inversion method.
doi: 10.1103/PhysRevC.67.034607
2003MA67 Nucl.Phys. A728, 415 (2003) Theoretical and empirical d + 4He potentials: an anomalous Majorana component? NUCLEAR REACTIONS 2H(α, α), E ≈ 10-120 MeV; calculated, analyzed scattering potential, parity dependence, related features. Resonating group method, iterative perturbative procedure.
doi: 10.1016/j.nuclphysa.2003.09.005
2002BO58 Phys.Rev. C 66, 064602 (2002) Investigation of the coupling potential by means of S-matrix inversion NUCLEAR REACTIONS 12C, 24Mg(12C, 12C), 28Si(16O, 16O), E=93.8, 126.7 MeV; calculated coupling potential, effect on inelastic scattering potential. S-matrix inversion.
doi: 10.1103/PhysRevC.66.064602
2000CO22 Nucl.Phys. A677, 187 (2000) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev An Inversion Procedure for Coupled-Channel Scattering: Determining the deuteron-nucleus tensor interaction NUCLEAR REACTIONS 58Ni(d, d'), E=56 MeV; 4He(d, d'), E=8-13 MeV; 56Fe(d, d'), E=30 MeV; calculated scattering potential. 4He(d, d'), E=10 MeV; calculated σ(θ), analyzing powers. S-matrix to potential inversion procedure, coupled channels approach.
doi: 10.1016/S0375-9474(00)00309-2
1999CO11 Phys.Rev. C59, 2361 (1999) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev Spin 1 Inversion: A Majorana tensor force for deuteron alpha scattering NUCLEAR REACTIONS 4He(polarized d, d'), E ≈ 10 MeV; analyzed σ(θ), tensor analyzing powers; deduced tensor interaction. S-matrix to potential inversion.
doi: 10.1103/PhysRevC.59.2361
1999KU21 Yad.Fiz. 62, No 7, 1187 (1999); Phys.Atomic Nuclei 62, 1114 (1999) V.I.Kukulin, V.N.Pomerantsev, S.G.Cooper, R.S.Mackintosh Majorana Tensor FOrce for Deuteron-Nucleus Interactions NUCLEAR REACTIONS 4He(d, d), E not given; analyzed data; deduced parity-dependent tensor component in internucleus interaction. Coupled-channel inversion technique.
1999MA02 Nucl.Phys. A645, 399 (1999) R.S.Mackintosh, S.G.Cooper, V.I.Kukulin Determination of 6Li-4He Interaction from Multi-Energy Scattering Data NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=19.6, 27.7, 37.5 MeV; analyzed σ(θ), vector analyzing power vs theta; deduced interaction potential. Energy dependent components, Majorana terms.
doi: 10.1016/S0375-9474(98)00623-X
1998CO17 Phys.Rev. C58, R31 (1998) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, E.V.Kuznetsova New Technique for Phase Shift Analysis: Multienergy Solution of Inverse Scattering Problem NUCLEAR REACTIONS 4He(polarized d, d), E=3-12 MeV; analyzed σ(θ), iT11(θ); deduced phase shifts. Direct inversion from multienergy data to potentials.
doi: 10.1103/PhysRevC.58.R31
1998MA48 J.Phys.(London) G24, 1599 (1998) Using Inverse Scattering Methods to Study Inter-Nucleus Potentials NUCLEAR REACTIONS 4He(polarized d, d), E=3-11.5 MeV; calculated σ(θ), iT11(θ). Iterative-perturbative method, applications to exotic nuclei discussed.
doi: 10.1088/0954-3899/24/8/039
1997MA24 J.Phys.(London) G23, 565 (1997) The Energy Dependence of the Nucleon-Nucleus Potential NUCLEAR REACTIONS 16O(n, n), E=4-20 MeV; 40Ca(n, n), E=12-20 MeV; calculated nucleon-nucleus potential vs E; deduced energy-dependent inversion procedure related features. Comparison between different approaches.
doi: 10.1088/0954-3899/23/5/009
1997MA63 Nucl.Phys. A625, 651 (1997) Deuteron-α Interaction by Inversion of RGM S-Matrix: Determination of spin-orbit potential for spin-one projectile NUCLEAR REACTIONS 4He(d, d), E(cm)=17-55 MeV; calculated potential; deduced spin-orbit role. Iterative-perturbative procedure.
doi: 10.1016/S0375-9474(97)00495-8
1996CO20 Phys.Rev. C54, 3133 (1996) Energy Dependent Potentials Determined by Inversion: The p + α potential up to 65 MeV NUCLEAR REACTIONS 16O(p, p), E not given; calculated zero energy potentials. 4He(p, p), E ≤ 65 MeV; calculated phase shifts vs E; deduced zero energy potentials. Inversion of resonating group methods phase shifts.
doi: 10.1103/PhysRevC.54.3133
1995AI02 J.Phys.(London) G21, 577 (1995) S.Ait-Tahar, R.S.Mackintosh, M.A.Russell A Note on the Implications of Causality for l-Dependent Potentials NUCLEAR REACTIONS 16O(16O, 16O), E(cm) ≤ 80 MeV; calculated l-dependence of potential real part; deduced dispersion correction dependent term role, l-dependent potentials causality implications.
doi: 10.1088/0954-3899/21/4/009
1995CO01 Nucl.Phys. A582, 283 (1995) 11Li + 28Si and 11Li + 12C Elastic Scattering Studied by Inversion NUCLEAR REACTIONS 28Si(11Li, 11Li), E=319 MeV; 12C(11Li, 11Li), E=637 MeV; analyzed σ(θ). Inversion technique, two-step phenomenology.
doi: 10.1016/0375-9474(94)00477-5
1995CO18 Nucl.Phys. A592, 338 (1995) Quantitative Contribution of Antisymmetry to the Nucleon-Nucleus Potential NUCLEAR REACTIONS 4He(p, p), E(cm)=50 MeV; 3He(p, p), E(cm)=10-40 MeV; 3H(n, n), E(cm)=14.63-17.25 MeV; 6Li(n, n), E(cm)=8.57, 12 MeV; 16O(n, n), E=10-30 MeV; 40Ca(n, n), E=10, 30 MeV; calculated local equivalent potentials to single configuration RGM S-matricies. Iterative-pertubative inversion techniques.
doi: 10.1016/0375-9474(95)00310-W
1995MA37 Nucl.Phys. A589, 377 (1995) Exchange Contributions to Nucleus-Nucleus Potentials Deduced from RGM Phase Shifts Using Inversion NUCLEAR REACTIONS 3He(α, α), E(cm)=60 MeV; 16O(α, α), E(cm)=18 MeV; 3H(α, α), E(cm)=20 MeV; calculated resonating group method phase shifts; deduced potentials.
doi: 10.1016/0375-9474(95)00171-V
1994CO10 Phys.Rev. C50, 1308 (1994) S.G.Cooper, R.S.Mackintosh, A.Csoto, R.G.Lovas Local 4He-p Potentials from Resonating-Group Method Phase Shifts NUCLEAR REACTIONS 4He(p, p), E ≤ 20 MeV; calculated phase shifts vs E; deduced phase equivalent potentials, local potentials comparison. Multi-channel resonating group method.
doi: 10.1103/PhysRevC.50.1308
1994CO14 Nucl.Phys. A576, 308 (1994) 16O + 16O Elastic Scattering at 350 MeV Studied by Inversion NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; analyzed σ(θ). Two-step method including inversion.
doi: 10.1016/0375-9474(94)90261-5
1994CR02 Phys.Rev. C49, 1091 (1994) R.Crespo, R.C.Johnson, J.A.Tostevin, R.S.Mackintosh, S.G.Cooper Equivalent Local Potentials to Multiple Scattering Calculations of Nucleon-Nucleus Scattering NUCLEAR REACTIONS 16O(p, p), E=100, 135, 200 MeV; calculated local phase equivalent potentials. Multiple scattering expansion of the optical potential.
doi: 10.1103/PhysRevC.49.1091
1994RA06 Phys.Rev. C49, 1621 (1994) G.H.Rawitscher, D.Lukaszek, R.S.Mackintosh, S.G.Cooper Local Representation of the Exchange Nonlocality in n-16O Scattering NUCLEAR REACTIONS 16O(n, n), E=20, 50 MeV; analyzed σ(θ). Microscopic folding model, exchange nonlocality local representation.
doi: 10.1103/PhysRevC.49.1621
1993AI02 Nucl.Phys. A561, 285 (1993) S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper Local Representation of a Deep Parity and l-Dependent 16O + 20Ne Potential NUCLEAR REACTIONS 20Ne(16O, 16O), E=24.5 MeV; calculated σ(θ). Interative perturbative inversion method.
doi: 10.1016/0375-9474(93)90154-P
1993AI03 Nucl.Phys. A562, 101 (1993) S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper, T.Wada Energy Dependence of a Local Equivalent Potential for RGM Phase Shifts for 16O + 16O NUCLEAR REACTIONS 16O(16O, 16O), E=30-500 MeV; calculated σ(θ). Local equivalent potential for resonating group method phase shifts.
doi: 10.1016/0375-9474(93)90034-U
1993MA09 Phys.Rev. C47, 1716 (1993) Studying the 16O + 12C Dynamic Polarization Potential by Inversion NUCLEAR REACTIONS 12C(16O, 16O), E=168-311 MeV; calculated σ(θ); deduced dynamic polarization features. Coupled-channels, continuum discretized coupled-channels S-matricies, S(l)-V(r) inversion.
doi: 10.1103/PhysRevC.47.1716
1993MC01 Nucl.Phys. A552, 401 (1993) M.A.McEwan, S.G.Cooper, R.S.Mackintosh Elastic-Scattering Phenomenology by Inversion: (I). 12C + 12C from 140 to 2400 MeV NUCLEAR REACTIONS 12C(12C, 12C), E=0.14-2.4 GeV; calculated σ(θ); deduced potential parameters. Local internuclear potential, two-step procedure.
doi: 10.1016/0375-9474(93)90501-N
1992AI01 Nucl.Phys. A542, 499 (1992) S.Ait-Tahar, S.G.Cooper, R.S.Mackintosh An l-Independent Representation of Deep l-Dependent 16O + 16O Potential NUCLEAR REACTIONS 16O(16O, 16O), E=30-150 MeV; calculated l-independent equivalents of l-dependent potentials.
doi: 10.1016/0375-9474(92)90108-V
1992CO01 Phys.Rev. C45, 770 (1992) S.G.Cooper, M.A.McEwan, R.S.Mackintosh Elastic Scattering Phenomenology by Inversion: 16O on 12C at 608 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=608 MeV; calculated model parameters. Optical model, S-matrix approach, inversion techniques.
doi: 10.1103/PhysRevC.45.770
1992HA12 Nucl.Phys. A540, 171 (1992) P.R.Hayes, N.M.Clarke, K.I.Pearce, M.B.Becha, R.S.Mackintosh, J.B.A.England, L.Zybert, G.M.Field, S.Roman A Comparison of 3H and 3He Scattering from Light Deformed Nuclei NUCLEAR REACTIONS 22,20Ne(t, t'), (3He, 3He'), E=33.4 MeV; measured σ(θ); 26,24Mg(t, t'), (3He, 3He'), E ≈ 34 MeV; analyzed data; deduced potential parameters. 20,22Ne, 26,24Mg deduced deformation lengths, multipole moments. Coupled channel analysis.
doi: 10.1016/0375-9474(92)90199-T
1991CO05 Phys.Rev. C43, 1001 (1991) Proton-4He Potential Derived from Phase Shifts NUCLEAR REACTIONS 4He(p, p), E=0-23 MeV; analyzed phase shifts; deduced parity dependent potential. Iterative-perturbative inversion analysis.
doi: 10.1103/PhysRevC.43.1001
1990CO11 Nucl.Phys. A511, 29 (1990) Nucleon Wavefunctions for Elastic Scattering in the Presence of Dynamically Induced Non-Locality NUCLEAR REACTIONS 40Ca(p, p), E=30.3 MeV; 48Ca(p, p), E=65 MeV; calculated dynamic polarization potential.
doi: 10.1016/0375-9474(90)90025-H
1990CO15 Nucl.Phys. A513, 373 (1990) The O + Pb Interaction Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-102 MeV; calculated interaction potential parameters. Inversion procedure.
doi: 10.1016/0375-9474(90)90103-S
1990CO29 Nucl.Phys. A517, 285 (1990) S-Matrix to Potential Inversion of Low-Energy α-12C Phase Shifts NUCLEAR REACTIONS 12C(α, α), E < inelastic threshold; calculated phase shift vs E.
doi: 10.1016/0375-9474(90)90036-L
1990CO38 Z.Phys. A337, 357 (1990) An l-Independent Representation of a Majorana Potential NUCLEAR REACTIONS 20Ne(α, α), E=54.1 MeV; calculated σ(θ). S-matrix equivalent to parity dependent potential.
1989CO11 Phys.Rev. C40, 502 (1989) p-4He Scattering: Inversion of phase shifts at 64.9 MeV NUCLEAR REACTIONS 4He(p, p), E=64.9 MeV; analyzed phase shift; deduced Schrodinger, Dirac potentials parameters.
doi: 10.1103/PhysRevC.40.502
1989MA25 Nucl.Phys. A494, 123 (1989) Studing the Heavy-Ion Dynamic Polarization Potential NUCLEAR REACTIONS 12C(16O, 16O), E=139.2 MeV; calculated potential parameters. Dynamic polarization potential.
doi: 10.1016/0375-9474(89)90201-7
1988CL04 J.Phys.(London) G14, 1399 (1988) N.M.Clarke, P.R.Hayes, M.B.Becha, K.I.Pearce, R.J.Griffiths, J.B.A.England, L.Zybert, C.N.Pinder, G.M.Field, R.S.Mackintosh New Measurements of the Mass and Energy Levels of 22F NUCLEAR REACTIONS 22Ne(t, 3He), E=33.4 MeV; measured σ(E(3He)), σ(θ); deduced Q. 22F deduced levels, J, π, mass. Shell model calculation. NUCLEAR STRUCTURE 22F; calculated levels. Shell model.
doi: 10.1088/0305-4616/14/11/011
1988MA05 Nucl.Phys. A476, 287 (1988) R.S.Mackintosh, S.G.Cooper, A.A.Ioannides Apparent Emissive Effects in Local Optical Potentials NUCLEAR REACTIONS 16O(p, p), E=34.1 MeV; calculated real, imaginary potentials; deduced emissive effect role.
doi: 10.1016/0375-9474(88)90485-X
1988MA30 Nucl.Phys. A483, 173 (1988) R.S.Mackintosh, A.A.Ioannides, S.G.Cooper Stationary State Currents in Nuclear Reactions: Rotational coupling in alpha-particle scattering NUCLEAR REACTIONS 20Ne(α, α), E=104 MeV; calculated potentials. Stationary state currents.
doi: 10.1016/0375-9474(88)90530-1
1988MA31 Nucl.Phys. A483, 195 (1988) R.S.Mackintosh, A.A.Ioannides, S.G.Cooper Stationary State Currents in Proton Scattering: Alternative representation of ' emissive ' potentials NUCLEAR REACTIONS 16O, 40Ca(p, p), E=34.1 MeV; calculated potentials. Stationary state currents.
doi: 10.1016/0375-9474(88)90531-3
1987CO27 Nucl.Phys. A472, 101 (1987) S.G.Cooper, R.S.Mackintosh, A.A.Ioannides Systematics of the Pickup Contribution to the Nucleon-Nucleus Interaction NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=30.3-65 MeV; 48Ca(p, p), (n, n), E=65 MeV; calculated potential parameters. 48Ca(polarized p, p), E=65 MeV; calculated σ(θ), analyzing power vs θ. Finite-range coupled reaction channel model.
doi: 10.1016/0375-9474(87)90222-3
1987IO02 Nucl.Phys. A467, 482 (1987) S-Matrix to Potential Inversion at Fixed Energy. (II). Inclusion of spin; CRC effects in proton scattering NUCLEAR REACTIONS 40Ca(p, p), E=30.3 MeV; calculated potential parameter characteristics. S-matrix to potential inversion.
doi: 10.1016/0375-9474(87)90541-0
1987MA39 Nucl.Phys. A472, 85 (1987) R.S.Mackintosh, S.G.Cooper, A.A.Ioannides Do We Understand Deuteron Scattering at all ( Question ): The polarization potential due to mass-three channels NUCLEAR REACTIONS 40Ca(d, d), E=52, 80, 200 MeV; calculated potential parameters, S-matrix elements. Effective local polarization potential.
doi: 10.1016/0375-9474(87)90221-1
1986IO01 Phys.Lett. 169B, 113 (1986) Universal Features of the Breakup Contribution to the Composite Particle Optical Potential NUCLEAR REACTIONS 58Ni(d, d), E=80 MeV; 12C(6Li, 6Li), E=156 MeV; calculated breakup polarization potential characteristics; deduced S, S+D channel, continuum-continuum coupling roles.
doi: 10.1016/0370-2693(86)90632-5
1986MA47 Phys.Lett. 178B, 1 (1986) R.S.Mackintosh, A.A.Ioannides, I.J.Thompson Finite-Range Coupled Reaction Channel Calculation of Pickup Contribution to the Proton Optical-Model Potential NUCLEAR REACTIONS 40Ca(p, d), E=30.3 MeV; calculated potential parameter characteristics. Finite-range coupled reaction channel calculations.
doi: 10.1016/0370-2693(86)90459-4
1985IO01 Nucl.Phys. A438, 354 (1985) A Method for S-Matrix to Potential Inversion at Fixed Energy (I). Method Description and Evaluation NUCLEAR REACTIONS 16O(p, p), E=35.2 MeV; calculated σ(θ). S-matrix to potential inversion at fixed energy.
doi: 10.1016/0375-9474(85)90380-X
1985IO04 Phys.Lett. 161B, 43 (1985) Potential Model Representation of Channel Coupling and the Coulomb Barrier Anomaly NUCLEAR REACTIONS 208Pb(16O, 16O), E=80 MeV; calculated potential parameters, renormalization; deduced channel coupling role. Potential inversion procedure, iterative-perturbative S-Matrix.
doi: 10.1016/0370-2693(85)90605-7
1983KO06 Nucl.Phys. A395, 248 (1983) A.M.Kobos, G.R.Satchler, R.S.Mackintosh An Optical Potential Description of 16O + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(16O, 16O), E(cm)=21.1-34.8 MeV; analyzed σ(θ); deduced optical model, potential parameters. Double folded potential, model independent correction term.
doi: 10.1016/0375-9474(83)90099-4
1982KO23 Nucl.Phys. A389, 205 (1982) A.M.Kobos, R.S.Mackintosh, J.R.Rook Uncertainty in the Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 16O(p, p), (polarized p, p), E=30 MeV; calculated S-matrix element vs (L), Wolfenstein R-parameter; deduced nucleon-nucleus optical potential features. Phase shift analysis.
doi: 10.1016/0375-9474(82)90516-4
1982KO25 Phys.Rev. C26, 1766 (1982) Evaluation of Model-Independent Optical Potentials for the 16O + 40Ca System NUCLEAR REACTIONS 40Ca(16O, 16O), E(cm)=35.7 MeV; analyzed data; deduced potentials. Optical, full, restricted spline model analyses.
doi: 10.1103/PhysRevC.26.1766
1982MA35 Phys.Lett. 116B, 95 (1982) Potential Model Representation of 6Li Break-Up through a Simple Inversion Procedure NUCLEAR REACTIONS 12C(6Li, 6Li), E=156 MeV; calculated projectile breakup effects; deduced adiabatic breakup local potential equivalent. Inversion method, iterative perturbation approach.
doi: 10.1016/0370-2693(82)90983-2
1980MA19 Phys.Lett. 92B, 59 (1980) Application of Model Independent Analyses to the Evaluation of M3Y Heavy Ion Folding Model NUCLEAR REACTIONS 40Ca, 24Mg(6Li, 6Li), E=88 MeV; 40Ca(6Li, 6Li), E=30 MeV; 28Si(16O, 16O), E=55 MeV; analyzed data. Model independent spline interpolation method.
doi: 10.1016/0370-2693(80)90303-2
1979KO01 J.Phys.(London) G5, 97 (1979) The Phenomenology of Proton Elastic Scattering and Evidence for Angular-Momentum-Dependent Optical-Model Potentials NUCLEAR REACTIONS 16O(p, p), E=23-52 MeV; 40Ca(p, p), E=17-48 MeV; 58Ni(p, p), E=40, 100 MeV; 56Fe(p, p), E=30.3 MeV; calculated σ(θ), A(θ). L-dependent optical model.
doi: 10.1088/0305-4616/5/1/012
1979MA01 Nucl.Phys. A313, 173 (1979) Inelastic Scattering Calculations with Projected Hartree-Fock Wave Functions NUCLEAR REACTIONS 20Ne(p, p'), E=24.5 MeV; 24Mg(p, p'), E=49.5 MeV; calculated σ(θ). Projected Hartree-Fock wave functions, coupled-channels formalism.
doi: 10.1016/0375-9474(79)90574-8
1978GE02 Phys.Lett. 73B, 250 (1978) Evaluation of Local Equivalent Methods for Treating Exchange in Elastic Proton Scattering NUCLEAR REACTIONS 40Ca(p, p), E=15-55 MeV; calculated σ, polarization.
doi: 10.1016/0370-2693(78)90506-3
1978MA25 J.Phys.(London) G4, L135 (1978) Evidence for an Imaginary Spin-Orbit Term in the Proton Optical Potential NUCLEAR STRUCTURE 40Ca, 16O; calculated proton optical potential parameter.
doi: 10.1088/0305-4616/4/6/006
1978SV01 Phys.Rev. C18, 983 (1978) Spin-Orbit Force and the Deformation of 12C NUCLEAR STRUCTURE 12C; calculated deformation.
doi: 10.1103/PhysRevC.18.983
1977HA09 J.Phys.(London) G3, L19 (1977) Nuclear Shape Determination: The Effect of Density-Dependent Interactions NUCLEAR MOMENTS 20Ne, 24Mg, 154Sm; calculated quadrupole moment.
doi: 10.1088/0305-4616/3/2/001
1977KO22 Acta Phys.Pol. B8, 887 (1977) The Contribution of Pickup Channels to the Helion Optical Potential NUCLEAR REACTIONS 58Ni(3He, 3He), (3He, α), E=37.7, 51.3 MeV; calculated σ(θ).
1977MA09 Nucl.Phys. A280, 86 (1977) Nuclear Shape Measurement and the Validity of the Collective Model for Light Nuclei NUCLEAR STRUCTURE 20Ne, 24Mg; calculated collective properties.
doi: 10.1016/0375-9474(77)90295-0
1977MA15 Phys.Lett. 68B, 213 (1977) Evidence for Explicit Angular Momentum Dependence of the Proton Optical Model Potential NUCLEAR REACTIONS 40Ca(polarized p, p), E=30.3 MeV; calculated σ(θ), A(θ).
doi: 10.1016/0370-2693(77)90272-6
1976MA19 Z.Phys. A276, 25 (1976) A Comment on the Use of Folding Models for Inelastic Alpha-Particle Scattering NUCLEAR REACTIONS 20Ne(α, α'), E=104 MeV; calculated folding model parameters.
doi: 10.1007/BF01414589
1976MA29 Phys.Lett. 62B, 127 (1976) The Real and Imaginary Proton Optical Potentials: The Importance of Deuteron Channels NUCLEAR REACTIONS 40Ca(p, p), E=30 MeV; calculated potential with deuteron channel, σ(θ).
doi: 10.1016/0370-2693(76)90484-6
1976MA36 Nucl.Phys. A266, 379 (1976) Neutron Component Deformations, Folding Models and Satchler's Theorem NUCLEAR STRUCTURE 24Mg, 20Ne, 154Sm, 166Er, 232Th, 238U; calculated potential parameters. Folding model.
doi: 10.1016/0375-9474(76)90365-1
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