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NSR database version of April 26, 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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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23148.

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 E_R, 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 T_1/2, 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 ^{147,149,151,153,155}Eu; 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 ^{121,123,125,127,129,131,133,134}Ba, ^{127,129,131,133,135,137,139}La; 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 ^{101,103,105,107}Pd, ^{99,101,103,105}Ru, ^{99,101,103,105}Rh, ^{97,99,101,103}Tc; 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). ^{185,187,189,191,193,195}Pt, ^{185,187,189,191,193,195,197}Au; 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, ^{112,116,120,124}Sn, 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 ^{110,112,114,116}Cd, ^{112,114,116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^{142,144,146,148,150}Nd, ^{144,146,148,150,152}Sm, ^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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