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NSR database version of May 20, 2024.

Search: Author = M.Lozano

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2022SP01      Phys.Rev. C 105, 024323 (2022)

P.Spagnoletti, P.A.Butler, L.P.Gaffney, K.Abrahams, M.Bowry, J.Cederkall, T.Chupp, G.de Angelis, H.De Witte, P.E.Garrett, A.Goldkuhle, C.Henrich, A.Illana, K.Johnston, D.T.Joss, J.M.Keatings, N.A.Kelly, M.Komorowska, J.Konki, T.Kroll, M.Lozano, B.S.Nara Singh, D.O'Donnell, J.Ojala, R.D.Page, L.G.Pedersen, C.Raison, P.Reiter, J.A.Rodriguez, D.Rosiak, S.Rothe, M.Scheck, M.Seidlitz, T.M.Shneidman, B.Siebeck, J.Sinclair, J.F.Smith, M.Stryjczyk, P.Van Duppen, S.Vinals, V.Virtanen, K.Wrzosek-Lipska, N.Warr, M.Zielinska

Coulomb excitation of 222Rn

NUCLEAR REACTIONS 120Sn, 60Ni(222Rn, 222Rn'), E=4.23 MeV/nucleon [secondary 222Rn beam produced in Th(p, X), E=1.4 GeV reaction]; measured reaction products, Eγ, Iγ, (particle)γ-coin. 222Rn; deduced levels, J, π, E1, E2 and E3 matrix elements, high-spin levels, bands, intrinsic quadrupole and octupole moments. GOSIA analysis of Coulomb excitation cross sections. Miniball HPGe array at HIE-ISOLDE. Systematics of quadrupole moments and other parameters in even-A Ra and Rn isotopes.

doi: 10.1103/PhysRevC.105.024323
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2020BU01      Phys.Rev.Lett. 124, 042503 (2020)

P.A.Butler, L.P.Gaffney, P.Spagnoletti, K.Abrahams, M.Bowry, J.Cederkall, G.de Angelis, H.De Witte, P.E.Garrett, A.Goldkuhle, C.Henrich, A.Illana, K.Johnston, D.T.Joss, J.M.Keatings, N.A.Kelly, M.Komorowska, J.Konki, T.Kroll, M.Lozano, B.S.Nara Singh, D.O'Donnell, J.Ojala, R.D.Page, L.G.Pedersen, C.Raison, P.Reiter, J.A.Rodriguez, D.Rosiak, S.Rothe, M.Scheck, M.Seidlitz, T.M.Shneidman, B.Siebeck, J.Sinclair, J.F.Smith, M.Stryjczyk, P.Van Duppen, S.Vinals, V.Virtanen, N.Warr, K.Wrzosek-Lipska, M.Zielinska

Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive 222Ra and 228Ra Beams

NUCLEAR REACTIONS 60Ni, 120Sn(222Ra, 222Ra'), (228Ra, 228Ra'), E=4.31 MeV/nucleon; measured reaction products, Eγ, Iγ. 222,228Ra; deduced γ-ray energies, dipole moments, quadrupole moments, E2 and E3 matrix elements, octupole collectivity.

doi: 10.1103/PhysRevLett.124.042503
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2020BU20      Nat. Commun. 11, 3560 (2020)

P.A.Butler, L.P.Gaffney, P.Spagnoletti, J.Konki, M.Scheck, J.F.Smith, K.Abrahams, M.Bowry, J.Cederkall, T.Chupp, G.de Angelis, H.De Witte, P.E.Garrett, A.Goldkuhle, C.Henrich, A.Illana, K.Johnston, D.T.Joss, J.M.Keatings, N.A.Kelly, M.Komorowska, T.Kroll, M.Lozano, B.S.Nara Singh, D.O'Donnell, J.Ojala, R.D.Page, L.G.Pedersen, C.Raison, P.Reiter, J.A.Rodriguez, D.Rosiak, S.Rothe, T.M.Shneidman, B.Siebeck, M.Seidlitz, J.Sinclair, M.Stryjczyk, P.Van Duppen, S.Vinals, V.Virtanen, N.Warr, K.Wrzosek-Lipska, M.Zielinska

Addendum: The observation of vibrating pear-shapes in radon nuclei

NUCLEAR REACTIONS 120Sn(222Rn, 222Rn'), E=4.23 MeV/nucleon; 120Sn(224Rn, 224Rn'), (226Rn, 226Rn'), E=5.08 MeV/nucleon; analyzed available data with updated computer codes. 222,224,226Rn; deduced additional γ-ray energies for high-spin transitions, J, π, level schemes, octupole-vibrational bands. Comparison with systematics of radon isotopes. Root analysis files.

doi: 10.1038/s41467-020-17309-y
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2019BU29      Nat. Commun. 10, 2473 (2019)

P.A.Butler, L.P.Gaffney, P.Spagnoletti, J.Konki, M.Scheck, J.F.Smith, K.Abrahams, M.Bowry, J.Cederkall, T.Chupp, G.de Angelis, H.De Witte, P.E.Garrett, A.Goldkuhle, C.Henrich, A.Illana, K.Johnston, D.T.Joss, J.M.Keatings, N.A.Kelly, M.Komorowska, T.Kroll, M.Lozano, B.S.Nara Singh, D.O'Donnell, J.Ojala, R.D.Page, L.G.Pedersen, C.Raison, P.Reiter, J.A.Rodriguez, D.Rosiak, S.Rothe, T.M.Shneidman, B.Siebeck, M.Seidlitz, J.Sinclair, M.Stryjczyk, P.Van Duppen, S.Vinals, V.Virtanen, N.Warr, K.Wrzosek-Lipska, M.Zielinska

The observation of vibrating pear-shapes in radon nuclei

NUCLEAR REACTIONS 120Sn(222Rn, 222Rn'), E=4.23 MeV/nucleon; 120Sn(224Rn, 224Rn'), (226Rn, 226Rn'), E=5.08 MeV/nucleon; measured reaction products, Eγ, Iγ, γ-γ-coin., X-rays. 222,224,226Rn; deduced γ-ray energies, J, π, level schemes, octupole-vibrational bands, high-spin transitions. Comparison with systematics of radon isotopes. HIE-ISOLDE accelerator, Miniball spectrometer.

doi: 10.1038/s41467-019-10494-5
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2013PR06      Nucl.Instrum.Methods Phys.Res. A727, 1 (2013)

J.Praena, P.F.Mastinu, M.Pignatari, J.M.Quesada, J.Garcia-Lopez, M.Lozano, N.Dzysiuk, R.Capote, G.Martin-Hernandez

Measurement of the MACS of 181Ta(n, γ) at kT=30 KeV as a test of a method for Maxwellian neutron spectra generation

NUCLEAR REACTIONS 181Ta, 197Au(n, γ), E<120 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian-averaged σ. Comparison with experimental results, ENDF libraries.

doi: 10.1016/j.nima.2013.05.151
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2011BE47      Eur.Phys.J. A 47, 160 (2011)

F.Belloni, M.Calviani, N.Colonna, P.Mastinu, P.M.Milazzo, U.Abbondanno, G.Aerts, H.Alvarez, F.Alvarez-Velarde, S.Andriamonje, J.Andrzejewski, L.Audouin, G.Badurek, M.Barbagallo, P.Baumann, F.Becvar, E.Berthoumieux, F.Calvino, D.Cano-Ott, R.Capote, C.Carrapico, P.Cennini, V.Chepel, E.Chiaveri, G.Cortes, A.Couture, J.Cox, M.Dahlfors, S.David, I.Dillmann, C.Domingo-Pardo, W.Dridi, I.Duran, C.Eleftheriadis, M.Embid-Segura, A.Ferrari, R.Ferreira-Marques, K.Fujii, W.Furman, I.Goncalves, E.Gonzalez-Romero, A.Goverdovski, F.Gramegna, C.Guerrero, F.Gunsing, B.Haas, R.Haight, M.Heil, A.Herrera-Martinez, M.Igashira, E.Jericha, F.Kappeler, Y.Kadi, D.Karadimos, D.Karamanis, M.Kerveno, P.Koehler, E.Kossionides, M.Krticka, C.Lamboudis, H.Leeb, A.Lindote, I.Lopes, M.Lozano, S.Lukic, J.Marganiec, S.Marrone, T.Martinez, C.Massimi, M.H.Meaze, A.Mengoni, C.Moreau, M.Mosconi, F.Neves, H.Oberhummer, S.O'Brien, J.Pancin, C.Papachristodoulou, C.Papadopoulos, C.Paradela, N.Patronis, A.Pavlik, P.Pavlopoulos, L.Perrot, M.T.Pigni, R.Plag, A.Plompen, A.Plukis, A.Poch, J.Praena, C.Pretel, J.Quesada, T.Rauscher, R.Reifarth, M.Rosetti, C.Rubbia, G.Rudolf, P.Rullhusen, J.Salgado, C.Santos, L.Sarchiapone, I.Savvidis, C.Stephan, G.Tagliente, J.L.Tain, D.Tarrio, L.Tassan-Got, L.Tavora, R.Terlizzi, G.Vannini, P.Vaz, A.Ventura, D.Villamarin, M.C.Vincente, V.Vlachoudis, R.Vlastou, F.Voss, S.Walter, M.Wiescher, K.Wisshak

Measurement of the neutron-induced fission cross-section of 243Am relative to 235U from 0.5 to 20 MeV

NUCLEAR REACTIONS 235U, 243Am(n, F), E=0.5-20 MeV; measured fission products using n_TOF fast ionization chamber; deduced σ; calculated σ using EMPIRE code. Compared with other data, ENDF/B-VII.0, JENDL-4.0, JEFF-3.1.1, ROSFOND, BROND-2.2.

doi: 10.1140/epja/i2011-11160-x
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2011TA17      Phys.Rev. C 84, 015801 (2011)

G.Tagliente, P.M.Milazzo, K.Fujii, U.Abbondanno, G.Aerts, H.Alvarez, F.Alvarez-Velarde, S.Andriamonje, J.Andrzejewski, L.Audouin, G.Badurek, P.Baumann, F.Becvar, F.Belloni, E.Berthoumieux, S.Bisterzo, F.Calvino, M.Calviani, D.Cano-Ott, R.Capote, C.Carrapico, P.Cennini, V.Chepel, E.Chiaveri, N.Colonna, G.Cortes, A.Couture, J.Cox, M.Dahlfors, S.David, I.Dillmann, C.Domingo-Pardo, W.Dridi, I.Duran, C.Eleftheriadis, M.Embid-Segura, A.Ferrari, R.Ferreira-Marques, W.Furman, R.Gallino, I.Goncalves, E.Gonzalez-Romero, F.Gramegna, C.Guerrero, F.Gunsing, B.Haas, R.Haight, M.Heil, A.Herrera-Martinez, E.Jericha, F.Kappeler, Y.Kadi, D.Karadimos, D.Karamanis, M.Kerveno, E.Kossionides, M.Krticka, C.Lamboudis, H.Leeb, A.Lindote, I.Lopes, M.Lozano, S.Lukic, J.Marganiec, S.Marrone, T.Martnez, C.Massimi, P.Mastinu, A.Mengoni, C.Moreau, M.Mosconi, F.Neves, H.Oberhummer, S.O'Brien, J.Pancin, C.Papachristodoulou, C.Papadopoulos, C.Paradela, N.Patronis, A.Pavlik, P.Pavlopoulos, L.Perrot, M.T.Pigni, R.Plag, A.Plompen, A.Plukis, A.Poch, J.Praena, C.Pretel, J.Quesada, T.Rauscher, R.Reifarth, M.Rosetti, C.Rubbia, G.Rudolf, P.Rullhusen, J.Salgado, C.Santos, L.Sarchiapone, I.Savvidis, C.Stephan, J.L.Tain, L.Tassan-Got, L.Tavora, R.Terlizzi, G.Vannini, P.Vaz, A.Ventura, D.Villamarin, M.C.Vincente, V.Vlachoudis, R.Vlastou, F.Voss, S.Walter, M.Wiescher, K.Wisshak

Neutron capture on 94Zr: Resonance parameters and Maxwellian-averaged cross sections

NUCLEAR REACTIONS 94Zr(n, γ), E=0.001-60 keV; measured E(n), I(n), capture yield using CERN n_TOF neutron source; deduced resonance parameters ER, gamma and neutron widths, capture kernels; calculated Maxwellian-averaged capture cross sections. 95Zr; deduced resonances, J, l-values, R-matrix analysis. Comparison with previous studies. Discussed astrophysical implications.

doi: 10.1103/PhysRevC.84.015801
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2008DO05      J.Phys.(London) G35, 014020 (2008)

C.Domingo-Pardo, U.Abbondanno, G.Aerts, H.Alvarez, F.Alvarez-Velarde, S.Andriamonje, J.Andrzejewski, P.Assimakopoulos, L.Audouin, G.Badurek, P.Baumann, F.Becvar, E.Berthoumieux, S.Bisterzo, F.Calvino, M.Calviani, D.Cano-Ott, R.Capote, C.Carrapico, P.Cennini, V.Chepel, N.Colonna, G.Cortes, A.Couture, J.Cox, M.Dahlfors, S.David, I.Dillmann, W.Dridi, I.Duran, C.Eleftheriadis, M.Embid-Segura, L.Ferrant, A.Ferrari, R.Ferreira-Marques, K.Fujii, W.Furman, R.Gallino, I.Goncalves, E.Gonzalez-Romero, F.Gramegna, C.Guerrero, F.Gunsing, B.Haas, R.Haight, M.Heil, A.Herrera-Martinez, M.Igashira, E.Jericha, Y.Kadi, F.Kappeler, D.Karadimos, D.Karamanis, M.Kerveno, P.Koehler, E.Kossionides, M.Krticka, C.Lamboudis, H.Leeb, A.Lindote, I.Lopes, M.Lozano, S.Lukic, J.Marganiec, S.Marrone, C.Massimi, P.Mastinu, A.Mengoni, P.M.Milazzo, M.Mosconi, F.Neves, H.Oberhummer, S.O'Brien, J.Pancin, C.Papachristodoulou, C.Papadopoulos, C.Paradela, N.Patronis, A.Pavlik, P.Pavlopoulos, L.Perrot, M.T.Pigni, R.Plag, A.Plompen, A.Plukis, A.Poch, C.Pretel, J.Quesada, T.Rauscher, R.Reifarth, C.Rubbia, G.Rudolf, P.Rullhusen, J.Salgado, C.Santos, L.Sarchiapone, I.Savvidis, C.Stephan, G.Tagliente, J.L.Tain, L.Tassan-Got, L.Tavora, R.Terlizzi, G.Vannini, P.Vaz, A.Ventura, D.Villamarin, M.C.Vincente, V.Vlachoudis, R.Vlastou, F.Voss, S.Walter, M.Wiescher, K.Wisshak

The measurement of the 206Pb(n, γ) cross section and stellar implications

NUCLEAR REACTIONS 206Pb(n, γ), E=0.001-1000 keV; measured Eγ, Iγ, capture cross sections. Deduced maxwellian averaged sections.

doi: 10.1088/0954-3899/35/1/014020
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2003QU01      Comput.Phys.Commun. 153, 97 (2003)

J.M.Quesada, R.Capote, A.Molina, M.Lozano

Dispersion relations in the nuclear optical model

doi: 10.1016/S0010-4655(03)00157-7
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2003QU02      Phys.Rev. C 67, 067601 (2003)

J.M.Quesada, R.Capote, A.Molina, M.Lozano, J.Raynal

Analytical expressions for the dispersive contributions to the nucleon-nucleus optical potential

doi: 10.1103/PhysRevC.67.067601
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2002MO09      Phys.Rev. C65, 034616 (2002)

A.Molina, R.Capote, J.M.Quesada, M.Lozano

Dispersive Spherical Optical Model of Neutron Scattering from 27Al up to 250 MeV

NUCLEAR REACTIONS 27Al(n, n), E=0.1-250 MeV; calculated σ, σ(θ), Ay(θ); deduced nonlocality effects. Dispersive spherical optical model, relativistic kinematics, comparison with data.

doi: 10.1103/PhysRevC.65.034616
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1996DA26      Phys.Rev. C54, 1217 (1996)

C.H.Dasso, R.J.Liotta, M.Lozano

Dynamic Effective Potential for α-Particle Bound and Quasibound States

NUCLEAR REACTIONS 208Pb(α, α), E=16-480 MeV; analyzed data; deduced average potential V0(E).

RADIOACTIVITY 212Po(α); calculated T1/2, penetration probability vs r(c). Dynamic effective potential.

doi: 10.1103/PhysRevC.54.1217
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1992AL04      Nucl.Phys. A540, 261 (1992)

C.E.Alonso, M.I.Gallardo, M.Lozano, A.Vitturi

Algebraic Description of Multistep Processes in Very-Heavy Ion Reactions

NUCLEAR REACTIONS 112Sn(120Sn, 120Sn), E(cm)=280-380 MeV; calculated σ(θ), transfer channel σ. Algebraic S-matrix model.

doi: 10.1016/0375-9474(92)90203-V
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1991DE09      Nucl.Phys. A528, 242 (1991)

J.de Boer, J.Fernandez Niello, E.Hauber, E.G.Vogt, C.H.Dasso, M.Lozano, G.Pollarolo

Dynamical Effects in Heavy-Ion Interactions at Bombarding Energies Near the Coulomb Barrier. A Study for the 16O + 120Sn System

NUCLEAR REACTIONS 120Sn(16O, 16O), (16O, 16O'), E=46, 50, 54 MeV; measured σ(θ); deduced model parameters, dynamical effects role. Optical model.

doi: 10.1016/0375-9474(91)90427-8
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1988AL19      J.Phys.(London) G14, 877 (1988)

C.E.Alonso, J.M.Arias, M.Lozano

Europium Isotopes Studied with the IBFA-2 Model

NUCLEAR STRUCTURE 147,149,151,153,155Eu; calculated levels, μ, quadrupole moment, B(E2), isotope shifts. Interacting boson model.

doi: 10.1088/0305-4616/14/7/008
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1988DA08      Phys.Rev. C37, 1774 (1988)

C.H.Dasso, M.Lozano, A.Vitturi

Direct Versus Sequential Four-Particle Transfer in Heavy Ion Collisions with Superfluid Nuclei: Sn + Sn reaction

NUCLEAR REACTIONS 112Sn(120Sn, 116Sn), E(cm)=200-260 MeV; calculated direct, sequential reaction amplitude ratio.

doi: 10.1103/PhysRevC.37.1774
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1987AL21      J.Phys.(London) G13, 1269 (1987)

C.E.Alonso, J.M.Arias, M.Lozano

Nuclear Structure Studies of the Odd-Mass Ba and La Isotopes with the IBFA-2 Model

NUCLEAR STRUCTURE 121,123,125,127,129,131,133,134Ba, 127,129,131,133,135,137,139La; calculated levels, B(λ), μ, isotope shifts, charge radii. Interacting boson-fermion model.

doi: 10.1088/0305-4616/13/10/015
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1987AR14      Nucl.Phys. A466, 295 (1987)

J.M.Arias, C.E.Alonso, M.Lozano

Odd-Even Nuclei in the A = 100 Nuclear Region

NUCLEAR STRUCTURE 101,103,105,107Pd, 99,101,103,105Ru, 99,101,103,105Rh, 97,99,101,103Tc; calculated levels, B(λ), μ, δ, single particle transfer spectroscopic strengths.

doi: 10.1016/0375-9474(87)90443-X
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1987LO01      Phys.Rev. C35, 367 (1987)

M.Lozano, A.Vitturi

Effect of Elastic Transfer in Sub-Barrier Fusion between Similar Nuclei

NUCLEAR REACTIONS, ICPND 16,18O(16O, X), E(cm)=7-13 MeV; calculated fusion σ(E), target dependent enhancement factors. Sub-barrier fusion.

doi: 10.1103/PhysRevC.35.367
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1987LO09      Phys.Rev. C36, 452 (1987)

M.Lozano

Dispersive Contribution to the Nucleus-Nucleus Potential

NUCLEAR REACTIONS 58,60,64Ni, 70Ge(16O, 16O), E(cm) ≈ 30-50 MeV; 90Zr(16O, 16O), E(cm) ≈ 35-55 MeV; 208Pb(16O, 16O), E(cm) ≈ 75-95 MeV; calculated potential parameters; deduced dispersive contributions.

doi: 10.1103/PhysRevC.36.452
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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
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1986AL16      Phys.Lett. 177B, 130 (1986)

C.E.Alonso, J.M.Arias, M.Lozano

Backbending of Dy Isotopes Described with the Neutron-Protron IBA Plus Two-Quasiparticle Model

NUCLEAR STRUCTURE 154,156,158Dy; calculated levels, B(λ). Neutron-protron interacting boson model.

doi: 10.1016/0370-2693(86)91041-5
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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
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1986AR03      Phys.Rev. C33, 1482 (1986)

J.M.Arias, C.E.Alonso, M.Lozano

Test of the Proton-Neutron Interacting Boson-Fermion Model in the Region around A = 190

NUCLEAR STRUCTURE 189,187Ir; calculated levels, band systematics, intruder band, β(λ). 185,195Ir; calculated levels, band systematics. 191,193Ir; calculated levels, band systematics, quadrupole moments, μ, B(M1). 185,187,189,191,193,195Pt, 185,187,189,191,193,195,197Au; calculated levels, band systematics. Interacting boson model.

doi: 10.1103/PhysRevC.33.1482
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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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1985DA25      Phys.Rev. C32, 2195 (1985)

C.H.Dasso, M.Lozano, G.Pollarolo

Simple Estimates of Excitation Energy Sharing between Heavy and Light Fragments in Heavy-Ion Reactions

NUCLEAR REACTIONS 238U(56Fe, X), E=476 MeV; 208Pb(86Kr, X), E=1565 MeV; calculated total kinetic energy loss vs fragment excitation; deduced heavy, light fragment excitation energy sharing.

doi: 10.1103/PhysRevC.32.2195
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1985GO11      Nucl.Phys. A440, 543 (1985)

J.Gomez-Camacho, M.Lozano, M.A.Nagarajan

Coupled-Channel Calculations for the Elastic Scattering of 7Li by 40,48Ca at 89 MeV

NUCLEAR REACTIONS 40,48Ca(7Li, 7Li), (7Li, 7Li'), E=89 MeV; calculated σ(θ). Coupled-channels method.

doi: 10.1016/0375-9474(85)90245-3
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1985GO20      Phys.Lett. 161B, 39 (1985)

J.Gomez-Camacho, M.Lozano, M.A.Nagarajan

Coupled Channel Effects in the Scattering of 6,7Li by 58Ni

NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=12, 14, 16, 18, 20, 50.6, 73.7 MeV; 58Ni(7Li, 7Li), E=14.2, 16.3, 18.3, 20.3 MeV; calculated σ(θ). Coupled-channels formalism, effective interactions, model densities.

doi: 10.1016/0370-2693(85)90604-5
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1984LO06      J.Phys.(London) G10, 1071 (1984)

M.Lozano, A.Mandly, G.Madurga

Fusion Barriers for Heavy Systems with 1000 < Z1Z2 < 3000

NUCLEAR REACTIONS 65Cu(86Kr, X), E(cm)=157.4-308.2 MeV; 165Ho(40Ar, X), E(cm)=181, 240.9 MeV; 56Fe(136Xe, X), E(cm)=225 MeV; 139La(86Kr, X), E(cm)=312, 376.8, 438.6 MeV; 165Ho(84Kr, X), E=298.2, 326 MeV; 209Bi(84Kr, X), E(cm)=356.7, 374.5; calculated fusion σ. 141Pr(35Cl, X), E(cm)=120-135 MeV; 144,148,154Sm(40Ar, X), E(cm)=125-145 MeV; calculated fusion σ(E), barriers. Shell model nuclear density, effective interaction generated folding optical potential.

NUCLEAR STRUCTURE 35Cl, 40Ar, 56Fe, 65Cu, 84,86Kr, 90Zr, 109Ag, 132Xe, 139La, 141Pr, 144,148,154Sm, 165Ho, 209Bi, 238U; calculated nuclear density distribution rms radii.

doi: 10.1088/0305-4616/10/8/012
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1983ES02      J.Phys.(London) G9, 1367 (1983)

J.I.Escudero, X.Vinas, M.Lozano

Evaluation of the Nucleus-Nucleus Potential Calculated in the Sudden Approximation

NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U; calculated binding energies. Thomas-Fermi kinetic energy density, Weizsacker correction term.

NUCLEAR REACTIONS 208Pb(16O, 16O), E=129.5, 192 MeV; 209Bi(40Ar, 40Ar), E=286 MeV; 238U(40Ar, 40Ar), E=286, 340 MeV; calculated σ(θ), s-wave fusion barriers; deduced potential parameters. Sudden approximation, Weizsacker term effects.

doi: 10.1088/0305-4616/9/11/009
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1983QU01      Phys.Lett. 125B, 14 (1983)

J.M.Quesada, M.Lozano, G.Madurga

A Phenomenological Imaginary Part of the Optical Potential for Heavy Ions

NUCLEAR REACTIONS 28Si(16O, 16O), E=33-81 MeV; calculated σ(θ). Optical potential, phenomenological imaginary part.

doi: 10.1016/0370-2693(83)91224-8
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1982LO13      J.Phys.(London) G8, 1259 (1982)

M.Lozano, J.I.Escudero, G.Madurga

Nuclear Structure Effects in Frictionless Formula for Heavy-Ion Fusion

NUCLEAR REACTIONS, ICPND 14N(12C, X), E=10-80 MeV; 12,13C(12C, X), E=10-35 MeV; 10B, 14N(14N, X), E=sub-Coulomb; 14N(14N, X), 14,15N(16O, X), E=near fusion; 24,26Mg, 16O, 27Al, 40Ca(16O, X), 27Al(17O, X), 28Si, 24Mg, 27Al(18O, X), 24Mg, 27Al(20Ne, X), (32S, X), 28Si(28Si, X), 40Ca, 58Ni(32S, X), 58,64,62Ni, 27Al, 54,56Fe, 112,116,120,124Sn, 90Zr, 141Pr(35Cl, X), 110Pd, 109Ag, 121Sb, 165Ho, 197Au, 238U(40Ar, X), 132Xe, 165Ho(56Fe, X), (84Kr, X), E=high; calculated fusion σ vs E. Semi-empirical formalism, final state, entrance channel effects.

NUCLEAR STRUCTURE A=9-238; calculated nuclear density distribution rms radii. Semi-empirical formalism.

doi: 10.1088/0305-4616/8/9/011
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1981VI01      Phys.Rev. C23, 780 (1981)

F.J.Vinas, M.Lozano, G.Madurga

Double Folding with a Density-Dependent Effective Interaction and its Analytical Approximation

NUCLEAR REACTIONS 72,74,76Ge(16O, 16O), (18O, 18O), E=56 MeV; 100Mo, 62Ni(12C, 12C), E=48 MeV; 74Ge(12C, 12C), E=42 MeV; 208Pb(12C, 12C), E=96 MeV; 207Pb(13C, 13C), E=86.1 MeV; 28Si(16O, 16O), E=141.5, 215 MeV; 59Co, 60Ni(16O, 16O), E=141.7 MeV; 209Bi(11B, 11B), E=74.6; 208Pb(16O, 16O), E=129.5, 192 MeV; 209Bi(40Ar, 40Ar), E=286 MeV; analyzed σ(θ); deduced real optical potential parameters, renormalizing factor. Double folding model, nucleon-nucleon effective potential.

doi: 10.1103/PhysRevC.23.780
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1980LO01      Nucl.Phys. A334, 349 (1980)

M.Lozano, G.Madurga

Exponential Optical Potentials for Heavy-Ion Elastic Scattering

NUCLEAR REACTIONS 208Pb(16O, 16O), E=129.5, 192 MeV; 208Pb(12C, 12C), E=96 MeV; 209Bi(11B, 11B), E=74.6 MeV; 62Ni, 100Mo(12C, 12C), E=48 MeV; 74Ge(12C, 12C), E=42 MeV; 60Ni, 59Co, 28Si(16O, 16O), E=141.7 MeV; 207Pb(13C, 13C), E=86.1 MeV; 72,74,76Ge(16O, 16O), (18O, 18O), E=56 MeV; 64Ni(16O, 16O), E=56 MeV; 209Bi, 238U(40Ar, 40Ar), E=340 MeV; calculated σ(θ). Exponential optical potentials.

doi: 10.1016/0375-9474(80)90074-3
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1980LO02      Phys.Lett. 90B, 50 (1980)

M.Lozano, G.Madurga

Nuclear-Structure Dependence of the Fusion Cross Section for Heavy Ions

NUCLEAR REACTIONS 12C(14N, X), (18O, X), (15N, X), (19F, X), E(cm)=0.01-0.05 GeV; 32S(24Mg, X), (27Al, X), 27Al, 48Ti, 56Fe, 62Ni, 116,124Sn(35Cl, X), E=0.03-0.1 GeV; calculated fusion σ(E). Semiclassical model, nuclear matter density distribution.

doi: 10.1016/0370-2693(80)90048-9
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1980MA34      Phys.Lett. B95, 358 (1980)

G.Madurga, M.Lozano, A.Jadraque

The Role of Rainbow Refraction in Heavy Ion Elastic Scattering

NUCLEAR REACTIONS 40Ca(20Ne, 20Ne), (13C, 13C), (6Li, 6Li), 28Si(16O, 16O), E=30-200 MeV; 208Pb, 40Ca(16O, 16O), E=100-300 MeV; 59Co(16O, 16O), 40Ca(40Ca, 40Ca), E=40-200 MeV; analyzed data; deduced strong absorption radius, rainbow distance vs E.

doi: 10.1016/0370-2693(80)90168-9
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1979LO05      Phys.Lett. 82B, 170 (1979)

M.Lozano, G.Madurga, P.E.Hodgson

Critical Radii for Alpha-Particle Elastic Scattering

NUCLEAR STRUCTURE 110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 122,124,126,128,130Te, 142,144,146,148,150Nd, 144,146,148,150,152Sm, 204,206,208Pb; calculated nuclear density distribution using Saxon-Woods single particle functions; deduced method to obtain α-optical potentials from target nucleus structure.

doi: 10.1016/0370-2693(79)90727-5
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