NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = M.V.Andres Found 47 matches. 2023LA04 Prog.Part.Nucl.Phys. 129, 104006 (2023) E.G.Lanza, L.Pellegri, A.Vitturi, M.V.Andres Theoretical studies of Pygmy Resonances
doi: 10.1016/j.ppnp.2022.104006
2019LA21 Eur.Phys.J. A 55, 235 (2019) E.G.Lanza, L.Pellegri, M.V.Andres, F.Catara, A.Vitturi Low-lying dipole and quadrupole states
doi: 10.1140/epja/i2019-12797-y
2018MA36 Phys.Lett. B 782, 112 (2018) N.S.Martorana, G.Cardella, E.G.Lanza, L.Acosta, M.V.Andres, L.Auditore, F.Catara, E.De Filippo, S.De Luca, D.Dell'Aquila, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, D.Santonocito, A.Trifiro, M.Trimarchi, M.Vigilante, A.Vitturi First measurement of the isoscalar excitation above the neutron emission threshold of the Pygmy Dipole Resonance in 68Ni NUCLEAR REACTIONS 12C(68Ni, γ), E=28 MeV/nucleon; measured reaction products, Eγ, Iγ. 68Ni; deduced σ(E), σ(θ), γ-ray decay of the pygmy resonance.
doi: 10.1016/j.physletb.2018.05.019
2018MA46 Acta Phys.Pol. B49, 475 (2018) N.S.Martorana, G.Cardella, E.G.Lanza, L.Acosta, M.V.Andres, L.Auditore, F.Catara, E.De Filippo, S.De Luca, D.Dell'Aquila, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, D.Santonocito, A.Trifiro, M.Trimarchi, M.Vigilante, A.Vitturi Experimental Study of the Pygmy Dipole Resonance in the 68Ni Nucleus NUCLEAR REACTIONS 9Be(70Zn, x), E=40 MeV/nucleon; measured fragmentation products, mainly 66,67,68Ni; 12C(p, x), E=24 MeV; measured protons, γ-rays; deduced Q-value spectrum, deduced total Doppler-corrected γ-ray energy spectrum in coincidence with 66,67,68Ni detected with CsI(Tl) of CHIMERA in coincidence with inelastic and with elastic channels, not normalized σ(θ), yield of Pygmy Dipole Resonance (PDR) obtained using subtraction of other channels. NEWCHIM-CHIMERA Collaboration standard tagging system, which allows event-by-event measurement of the isotopic composition.
doi: 10.5506/aphyspolb.49.475
2016GA04 Phys.Rev. C 93, 024309 (2016) D.Gambacurta, F.Catara, M.Grasso, M.Sambataro, M.V.Andres, E.G.Lanza Nuclear excitations as coupled one and two random-phase-approximation modes NUCLEAR STRUCTURE 16O; calculated low-lying levels and giant resonances (dipole, quadrupole and octupole), J, π, monopole (E0), dipole (E1), isoscalar quadrupole (E2), and isoscalar octupole (E3) response functions. Double random-phase approximation (DRPA) method to include two -particle two-hole (2p-2h) configurations and by coupling them with the 1p-1h ones and among themselves. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.024309
2015LA11 Phys.Rev. C 91, 054607 (2015) E.G.Lanza, A.Vitturi, M.V.Andres Microscopic nuclear form factors for the pygmy dipole resonance NUCLEAR REACTIONS 68Ni(12C, X), E=10 MeV/nucleon; calculated form factors, σ(θ), RPA transition densities for the pygmy dipole resonant (PDR) state and isoscalar giant dipole resonance (ISGDR) states using DWBA and DWUCK4 computer code. Comparison with other theoretical calculations using different macroscopic collective models.
doi: 10.1103/PhysRevC.91.054607
2011AC02 Phys.Rev. C 84, 044604 (2011) L.Acosta, A.M.Sanchez-Benitez, M.E.Gomez, I.Martel, F.Perez-Bernal, F.Pizarro, J.Rodriguez-Quintero, K.Rusek, M.A.G.Alvarez, M.V.Andres, J.M.Espino, J.P.Fernandez-Garcia, J.Gomez-Camacho, A.M.Moro, C.Angulo, J.Cabrera, E.Casarejos, P.Demaret, M.J.G.Borge, D.Escrig, O.Tengblad, S.Cherubini, P.Figuera, M.Gulino, M.Freer, C.Metelko, V.Ziman, R.Raabe, I.Mukha, D.Smirnov, O.R.Kakuee, J.Rahighi Elastic scattering and α-particle production in 6He + 208Pb collisions at 22 MeV NUCLEAR REACTIONS 208Pb(6He, 6He), [secondary 6He beam from 7Li(p, 2p), E=30 MeV primary reaction], E=22 MeV; measured particle spectra, yields, σ(θ), 4He production rates and 4He energy distribution spectrum. DWBA analysis. Discussed neutron transfer mechanism for 4He production.
doi: 10.1103/PhysRevC.84.044604
2011LA22 Phys.Rev. C 84, 064602 (2011) E.G.Lanza, A.Vitturi, M.V.Andres, F.Catara, D.Gambacurta Excitations of pygmy dipole resonances in exotic and stable nuclei via Coulomb and nuclear fields NUCLEAR REACTIONS 132Sn(α, α'), (40Ca, 40Ca'), (48Ca, 48Ca'), E=30, 60, 100 MeV; 208Pb(17O, 17O'), E=20, 50 MeV; calculated form factors for PDR states and GDR, partial wave cross sections, differential cross sections. 100Sn, 120Sn, 132Sn, 208Pb; calculated isovector strength distributions B(E1), RPA transition strengths for low-lying states. Hartree-Fock plus RPA random phase approximation (RPA), with Skyrme interaction.
doi: 10.1103/PhysRevC.84.064602
2010VI02 Pramana 75, 73 (2010) A.Vitturi, E.G.Lanza, M.V.Andres, F.Catara, D.Gambacurta Excitation of pygmy dipole resonance in neutron-rich nuclei via Coulomb and nuclear fields NUCLEAR REACTIONS 208Pb(132Sn, 132Sn'), E=6, 10, 20, 50 MeV/nucleon; 4He, 40,48Ca(132Sn, 132Sn'), E=10 MeV/nucleon; 132Sn; calculated σ(θ), σ(E), transition densities of dipole state, B(E1), form factors.
doi: 10.1007/s12043-010-0066-z
2009AC02 Eur.Phys.J. A 42, 461 (2009); Erratum Eur.Phys.J. A 42, 623 (2009) L.Acosta, M.A.G.Alvarez, M.V.Andres, M.J.G.Borge, M.Cortes, J.M.Espino, D.Galaviz, J.Gomez-Camacho, A.Maira, I.Martel, A.M.Moro, I.Mukha, F.Perez-Bernal, E.Reillo, D.Rodriguez, K.Rusek, A.M.Sanchez-Benitez, O.Tengblad Signature of a strong coupling with the continuum in 11Be + 120Sn scattering at the Coulomb barrier NUCLEAR REACTIONS 120Sn(11Be, 11Be), (11Be, 11Be'), E=2.91 MeV/nucleon; measured particle spectra using DSSSD array at REX-ISOLDE; deduced σ(θ). Comparison with coupled-channel calculations. Secondary radioactive halo nuclide beam.
doi: 10.1140/epja/i2009-10822-6
2009LA11 Phys.Rev. C 79, 054615 (2009) E.G.Lanza, F.Catara, D.Gambacurta, M.V.Andres, Ph.Chomaz Multiphonon excitations and pygmy resonances in tin isotopes NUCLEAR REACTIONS 100,120,132Sn(γ, γ'), E not given; calculated proton and neutron densities, isoscalar strength distributions for monopole, quadrupole and octupole states, isovector strength distributions for dipole states, transition probabilities, transition densities for low-lying dipole state for pygmy dipole resonance and giant dipole resonance. Microscopic RPA and boson expansion calculations. 120,132Sn(208Pb, X), E=500 MeV/nucleon; calculated relativistic Coulomb inelastic cross sections using coupled-channel method.
doi: 10.1103/PhysRevC.79.054615
2008SA09 Nucl.Phys. A803, 30 (2008) A.M.Sanchez-Benitez, D.Escrig, M.A.G.Alvarez, M.V.Andres, C.Angulo, M.J.G.Borge, J.Cabrera, S.Cherubini, P.Demaret, J.M.Espino, P.Figuera, M.Freer, J.E.Garcia-Ramos, J.Gomez-Camacho, M.Gulino, O.R.Kakuee, I.Martel, C.Metelko, A.M.Moro, F.Perez-Bernal, J.Rahighi, K.Rusek, D.Smirnov, O.Tengblad, P.Van Duppen, V.Ziman Study of the elastic scattering of 6He on 208Pb at energies around the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, 6He), E=14, 16, 18, 22 MeV; measured σ(θ). Comparison with optical model calculations, including Coulomb dipole polarizability and dispersion relations.
doi: 10.1016/j.nuclphysa.2008.01.030
2007ES06 Nucl.Phys. A792, 2 (2007) D.Escrig, A.M.Sanchez-Benitez, A.M.Moro, M.A.G.Alvarez, M.V.Andres, C.Angulo, M.J.G.Borge, J.Cabrera, S.Cherubini, P.Demaret, J.M.Espino, P.Figuera, M.Freer, J.E.Garcia-Ramos, J.Gomez-Camacho, M.Gulino, O.R.Kakuee, I.Martel, C.Metelko, F.Perez-Bernal, J.Rahighi, K.Rusek, D.Smirnov, O.Tengblad, V.Ziman α-particle production in the scattering of 6He by 208Pb at energies around the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, α), E=14, 16, 18, 22 MeV; measured Eα, Iα, σ(E, θ); deduced reaction mechanism features using DWBA analysis.
doi: 10.1016/j.nuclphysa.2007.05.012
2007LA28 Nucl.Phys. A788, 112c (2007) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, M.Fallot, J.A.Scarpaci Triple Giant Resonance Excitations: A Microscopic Approach NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=25, 50, 100 MeV/nucleon; 208Pb(208Pb, 208Pb'), E=641 MeV/nucleon; calculated σ(E), one-, two-, and three-phonon components, giant resonance excitation. Microscopic extended RPA with anharmonicity.
doi: 10.1016/j.nuclphysa.2007.01.056
2006KA01 Nucl.Phys. A765, 294 (2006) O.R.Kakuee, M.A.G.Alvarez, M.V.Andres, S.Cherubini, T.Davinson, A.Di Pietro, W.Galster, J.Gomez-Camacho, A.M.Laird, M.Lamehi-Rachti, I.Martel, A.M.Moro, J.Rahighi, A.M.Sanchez-Benitez, A.C.Shotter, W.B.Smith, J.Vervier, P.J.Woods Long range absorption in the scattering of 6He on 208Pb and 197Au at 27 MeV NUCLEAR REACTIONS 197Au(6He, 6He), E=27 MeV; measured quasi-elastic σ(θ); 208Pb(6He, 6He), E=27 MeV; analyzed elastic σ(θ); deduced optical model parameters, role of Coulomb dipole polarisability, reaction mechanism features.
doi: 10.1016/j.nuclphysa.2005.11.012
2006LA30 Phys.Rev.C 74, 064614 (2006) E.G.Lanza, F.Catara, M.V.Andres, Ph.Chomaz, M.Fallot, J.A.Scarpaci Microscopic calculations of double and triple giant resonance excitations in heavy ion collisions NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=50 MeV/nucleon; 208Pb(208Pb, 208Pb'), E=641 MeV/nucleon; calculated σ(E), one-, two-, and three-phonon components, giant resonance excitation. Microscopic extended RPA with anharmonicity, effects of four phonon states estimated.
doi: 10.1103/PhysRevC.74.064614
2005SA52 J.Phys.(London) G31, S1953 (2005) A.M.Sanchez-Benitez, D.Escrig, M.A.G.Alvarez, M.V.Andres, C.Angulo, M.J.G.Borge, J.Cabrera, S.Cherubini, J.M.Espino, P.Figuera, M.Freer, J.E.Garcia-Ramos, J.Gomez-Camacho, M.Gulino, O.R.Kakuee, I.Martel, C.Metelco, A.M.Moro, J.Rahighi, K.Rusek, D.Smirnov, O.Tengblad, P.Van Duppen, V.Ziman Scattering of 6He at energies around the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, 6He), (6He, α), E=14, 16, 17, 18, 22 MeV; measured σ(θ); deduced reaction mechanism features.
doi: 10.1088/0954-3899/31/10/109
2003AN22 Nucl.Phys. A724, 113 (2003) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Deviations from the adiabatic approximation in heavy-ion dynamic polarization potentials
doi: 10.1016/S0375-9474(03)01521-5
2003FA17 Nucl.Phys. A729, 699 (2003) M.Fallot, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza, J.A.Scarpaci Anharmonic vibrations in nuclei NUCLEAR STRUCTURE 40Ca, 208Pb; calculated two- and three-phonon states configurations, strength distributions, mixing features, giant resonance effects.
doi: 10.1016/j.nuclphysa.2003.10.001
2003KA60 Nucl.Phys. A728, 339 (2003) O.R.Kakuee, J.Rahighi, A.M.Sanchez-Benitez, M.V.Andres, S.Cherubini, T.Davinson, W.Galster, J.Gomez-Camacho, A.M.Laird, M.Lamehi-Rachti, I.Martel, A.C.Shotter, W.B.Smith, J.Vervier, P.J.Woods Elastic scattering of the halo nucleus 6He from 208Pb above the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, 6He), E=27 MeV; measured elastic σ(θ); deduced optical model parameters, role of Coulomb dipole polarisability.
doi: 10.1016/j.nuclphysa.2003.08.030
2002AN01 Phys.Rev. C65, 014608 (2002) M.V.Andres, F.Catara, E.G.Lanza, Ph.Chomaz, M.Fallot, J.A.Scarpaci Microscopic Description of Coulomb and Nuclear Excitation of Multiphonon States in 40Ca + 40Ca Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=50 MeV/nucleon; calculated inelastic σ(E), population of one- and two-phonon states; deduced role of anharmonicities and nonlinearities. RPA approach.
doi: 10.1103/PhysRevC.65.014608
2001AL03 Nucl.Phys. A679, 359 (2001) C.E.Alonso, M.V.Andres, J.M.Arias, E.G.Lanza, A.Vitturi Coupling of Dipole Mode to γ-Unstable Quadrupole Oscillations
doi: 10.1016/S0375-9474(00)00360-2
1999AN07 Phys.Rev.Lett. 82, 1387 (1999) Dipole Polarizability in the Scattering of 11Li Below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=24 MeV; calculated σ(θ); deduced dipole polarizability role.
doi: 10.1103/PhysRevLett.82.1387
1999AN51 Phys.Lett. 470B, 6 (1999) M.V.Andres, E.G.Lanza, P.Van Isacker, C.Volpe, F.Catara Excitation of Multiple Giant Dipole Resonances: From spherical to deformed nuclei NUCLEAR STRUCTURE 148,150,152,154Sm, 238U; calculated multiple GDR B(E1) distributions. Interacting boson model. NUCLEAR REACTIONS 208Pb(238U, 238U'), E=0.5 GeV/nucleon; 148,150,152,154Sm(208Pb, 208Pb'), E=0.5 GeV/nucleon; calculated Coulomb excitation σ(E); deduced multiple GDR, deformation effects.
doi: 10.1016/S0370-2693(99)01220-4
1999LA33 Nucl.Phys. (Supplement) A654, 792c (1999) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Microscopic Description of Multiphonon States Excitation in Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=50, 641 MeV/nucleon; calculated GDR, double-GDR excitation σ and σ(E). Comparison with data. Microscopic approach.
doi: 10.1016/S0375-9474(00)88548-6
1999VO04 Nucl.Phys. A647, 246 (1999) C.Volpe, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza Boson Expansion Methods Applied to a Two-Level Model in the Study of Multiple Giant Resonances
doi: 10.1016/S0375-9474(99)00016-0
1998LA17 Nucl.Phys. A636, 452 (1998) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Microscopic Description of Coulomb and Nuclear Excitation of Multiphonon States in Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=50 MeV/nucleon; calculated inelastic σ(Ex, L) ; deduced nuclear, Coulomb contributions, role of anharmonicities, nonlinearities.
doi: 10.1016/S0375-9474(98)00222-X
1997AN01 Nucl.Phys. A612, 82 (1997) M.V.Andres, J.A.Christley, J.Gomez-Camacho, M.A.Nagarajan Dipole Coulomb Excitation in 11Be Scattering NUCLEAR REACTIONS, ICPND 197Au(11Be, 11Be'), E=30 MeV; calculated σ(θ), fusion σ vs spin; deduced projectile dipole Coulomb excitation related features. Dynamic polarization potentials, coupled-channels approach.
doi: 10.1016/S0375-9474(96)00324-7
1997AN18 Nucl.Phys. A625, 685 (1997) M.V.Andres, J.A.Christley, J.Gomez-Camacho, M.A.Nagarajan Spin-Orbit Dynamic Polarization Potential Due to Dipole Coulomb Excitation NUCLEAR REACTIONS 197Au(11Be, 11Be), E=30 MeV; calculated reaction σ, σ(θ), vector analyzing power; deduced Coulomb excitation role.
doi: 10.1016/S0375-9474(97)00388-6
1997LA07 Nucl.Phys. A613, 445 (1997) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Role of Anharmonicities and Nonlinearities in Heavy Ion Collisions a Microscopic Approach NUCLEAR REACTIONS 208Pb, 40Ca(208Pb, 208Pb'), E=0.641, 1 GeV/nucleon; calculated Coulomb excitation σ vs excitation energy, relativistic energies. Microscopic approach beyond RPA, anharmonicities, nonlinearities. NUCLEAR STRUCTURE 40Ca, 208Pb; calculated 1- giant resonances; deduced anharmonicities, nonlinearities role. Microscopic approach beyond RPA.
doi: 10.1016/S0375-9474(96)00444-7
1996VO08 Nucl.Phys. A599, 347c (1996) C.Volpe, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza Are Giant Resonances Harmonic Vibrations ( Question ) NUCLEAR REACTIONS 208Pb(136Xe, 136Xe'), E=700 MeV/nucleon; calculated one-, two-phonon states excitation in projectile by Coulomb excitation; deduced small anharmonicities, nonlinearities role.
doi: 10.1016/0375-9474(96)00077-2
1995AN06 Nucl.Phys. A583, 817c (1995) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Dynamic Polarization Potential Induced by Dipole Coulomb Excitation to Break-Up States in 11Li Scattering NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=50 MeV; calculated σ(θ). Polarization potential due to direct Coulomb excitation into the continuum.
doi: 10.1016/0375-9474(94)00765-F
1995BA60 Yad.Fiz. 58, No 4, 604 (1995); Phys.Atomic Nuclei 58, 548 (1995) E.B.Balbutsev, A.V.Unzhakova, M.V.Andres, F.Catara, E.G.Lanza Role of Low-Lying Isoscalar Dipole Modes in the Polarization Potential NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=2-8 GeV; calculated GDR, GQR other multipolarities contribution to real, imaginary part of local polarization potential. Wigner function moments method.
1995VO04 Nucl.Phys. A589, 521 (1995) C.Volpe, F.Catara, Ph.Chomaz, M.V.Andres, E.G.Lanza Anharmonicities and Non-Linearities in the Excitation of Double Giant Resonances NUCLEAR REACTIONS 208Pb(136Xe, X), E=700 MeV/nucleon; analyzed data; deduced anharmonicities, nonlinearities role in GDR excitation. Quantum anharmonic oscillator.
doi: 10.1016/0375-9474(95)00195-7
1994AN21 Nucl.Phys. A579, 273 (1994) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Dynamic Polarization Potential Induced by Dipole Coulomb Excitation NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=50 MeV; calculated σ(θ). Dipole Coulomb excitation induced dynamic polarization potential.
doi: 10.1016/0375-9474(94)90806-0
1994GO28 Nucl.Phys. A580, 156 (1994) J.Gomez-Camacho, M.V.Andres, M.A.Nagarajan Analytic Approximations for the Dynamic Polarization Effects Due to Coulomb Excitation NUCLEAR REACTIONS 184W(18O, 18O), (18O, 18O'), E=75, 90 MeV; calculated σ(θ); deduced dynamic polarization potential parameters. Coupled-channels approach.
doi: 10.1016/0375-9474(94)90820-6
1993AN01 Phys.Rev. C47, 902 (1993) M.V.Andres, F.Catara, E.G.Lanza Reply to ' Comment on ' Dynamical Polarization Potential Due to the Excitation of Collective States ' ' NUCLEAR REACTIONS 40Ca(16O, 16O), E < 600 MeV; calculated dynamical polarization potential parameters vs E; deduced form factors role.
doi: 10.1103/PhysRevC.47.902
1992MA11 Phys.Lett. 279B, 218 (1992) I.Martel, J.Gomez-Camacho, M.V.Andres Reorientation and Coupling Effects in Polarized Heavy Ion Fusion NUCLEAR REACTIONS 208Pb(polarized 23Na, X), E=100-120 MeV; calculated partial fusion σ(E), analyzing power; deduced effects of ground state reorientation, coupling to rotational states. Tidal symmetry model.
doi: 10.1016/0370-2693(92)90382-E
1991AN20 Phys.Rev. C44, 2709 (1991) M.V.Andres, F.Catara, E.G.Lanza Dynamical Polarization Potential Due to the Excitation of Collective States NUCLEAR REACTIONS 40Ca(16O, 16O), E=104 MeV; 40Ca(40Ca, 40Ca), E=143 MeV; calculated σ(θ); deduced potential parameters energy dependence. Dynamical polarization potential, Feshbach formalism.
doi: 10.1103/PhysRevC.44.2709
1989AN01 Phys.Rev. C39, 99 (1989) M.V.Andres, F.Catara, Ph.Chomaz, E.G.Lanza Random-Phase-Approximation-Based Dynamical Polarization Potential NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E(cm)=55.45-888 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.39.99
1989CH29 Europhys.Lett. 9, 125 (1989) Ph.Chomaz, Y.Blumenfeld, M.V.Andres, F.Catara, E.G.Lanza Importance of Giant-Resonance Excitation for the Surface Properties of the Heavy-Ion Optical Potential NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated response functions. RPA. NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(40Ca, 40Ca), E=33 MeV/nucleon; calculated transmission factor vs l. RPA based heavy-ion potential.
doi: 10.1209/0295-5075/9/2/006
1988AN01 Phys.Lett. 202B, 292 (1988) M.V.Andres, N.Rowley, M.A.Nagarajan Effect of Deformation on the Elastic and Quasielastic Scattering of Heavy Ions Near the Coulomb Barrier NUCLEAR REACTIONS 154Sm(16O, 16O), (16O, 16O'), (16O, X), E(cm)=63.45 MeV; calculated elastic, fusion σ(θ).
doi: 10.1016/0370-2693(88)90473-X
1988AN05 Nucl.Phys. A481, 600 (1988) M.V.Andres, N.Rowley, M.A.Nagarajan Deviations from Shape-Effect Relations in the Polarization of Inelastically Scattered Heavy Ions NUCLEAR REACTIONS 154Sm(polarized 16O, 16O), (polarized 16O, 16O'), E=60 MeV; calculated σ(θ), polarization vs θ. Coupled-channels method.
doi: 10.1016/0375-9474(88)90347-8
1988AN12 J.Phys.(London) G14, 1331 (1988) M.V.Andres, F.Catara, Ph.Chomaz, E.G.Lanza Polarisation Potential and Sub-Barrier Fusion in a Multiphonon Excitation Model NUCLEAR REACTIONS, ICPND 40Ca(40Ca, X), E(cm) ≈ 50-70 MeV; 48Ca(40Ca, X), E(cm)=48-68 MeV; calculated fusion σ(E). Adiabatic polarization potential.
doi: 10.1088/0305-4616/14/10/009
1987NA13 Phys.Lett. 192B, 297 (1987) M.A.Nagarajan, M.V.Andres, M.Lozano Polarization Effects Due to Coupling of Elastic to Compound States NUCLEAR REACTIONS 24Mg, 28Si, 40Ca(16O, 16O), E=33-140 MeV; calculated σ vs L; deduced polarization potential.
doi: 10.1016/0370-2693(87)90109-2
1986AN18 Nucl.Phys. A455, 561 (1986) M.V.Andres, M.Lozano, M.Barranco, M.Pi, X.Vinas, K.A.Gridnev Nuclear Transfer Contribution to the Imaginary Nucleus-Nucleus Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=40-139.6 MeV; 40Ca(40Ca, 40Ca), E=129.6-240 MeV; 208Pb(16O, 16O), E=192-1295 MeV; calculated σ(θ). Nucleon transfer role in nucleus-nucleus potential imaginary term.
doi: 10.1016/0375-9474(86)90322-2
1985AN16 Nucl.Phys. A443, 380 (1985) M.V.Andres, J.M.Quesada, M.Lozano, G.Madurga A Level-Density-Dependent Imaginary Potential for Heavy Ions NUCLEAR REACTIONS 28Si, 40Ca(9Be, 9Be), E=14-26 MeV; 24Mg(12C, 12C), E=21, 24 MeV; 24Mg(16O, 16O), E=28-33 MeV; 40Ca(20Ne, 20Ne), E=44.1-70.4 MeV; 40Ca(32S, 32S), E=100-151.5 MeV; calculated real folding potential renormalization constants, σ(θ). Level density dependent heavy ion potential component. NUCLEAR STRUCTURE 9Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 40Ca; calculated neutron, proton, charge density distributions. Woods-Saxon potential.
doi: 10.1016/0375-9474(85)90269-6
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