NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = A.Moro Found 135 matches. Showing 1 to 100. [Next]2024LI18 Phys.Rev. C 109, 034312 (2024) B.D.Linh, A.Corsi, A.Gillibert, A.Obertelli, P.Doornenbal, C.Barbieri, T.Duguet, M.Gomez-Ramos, J.D.Holt, B.S.Hu, T.Miyagi, A.M.Moro, P.Navratil, K.Ogata, S.Peru, N.T.T.Phuc, N.Shimizu, V.Soma, Y.Utsuno, N.L.Achouri, H.Baba, F.Browne, D.Calvet, F.Chateau, S.Chen, N.Chiga, M.L.Cortes, A.Delbart, J.-M.Gheller, A.Giganon, C.Hilaire, T.Isobe, T.Kobayashi, Y.Kubota, V.Lapoux, H.N.Liu, T.Motobayashi, I.Murray, H.Otsu, V.Panin, N.Paul, W.Rodriguez, H.Sakurai, M.Sasano, D.Steppenbeck, L.Stuhl, Y.L.Sun, Y.Togano, T.Uesaka, K.Wimmer, K.Yoneda, O.Aktas, T.Aumann, L.X.Chung, F.Flavigny, S.Franchoo, I.Gasparic, R.B.Gerst, J.Gibelin, K.I.Hahn, N.T.Khai, D.Kim, T.Koiwai, Y.Kondo, P.Koseoglou, J.Lee, C.Lehr, T.Lokotko, M.MacCormick, K.Moschner, T.Nakamura, S.Y.Park, D.Rossi, E.Sahin, D.Sohler, P.-A.Soderstrom, S.Takeuchi, H.Tornqvist, V.Vaquero, V.Wagner, S.T.Wang, V.Werner, X.Xu, Y.Yamada, D.Yan, Z.Yang, M.Yasuda, L.Zanetti Onset of collectivity for argon isotopes close to N=32
doi: 10.1103/PhysRevC.109.034312
2024WA04 Phys.Rev. C 109, 014624 (2024) K.Wang, Y.Y.Yang, Jin Lei, A.M.Moro, V.Guimaraes, J.G.Li, F.F.Duan, Z.Y.Sun, G.Yang, D.Y.Pang, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Liu, J.L.Lou, H.J.Ong, B.F.Lv, S.Guo, M.Kumar Raju, X.H.Wang, R.H.Li, X.X.Xu, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu Elastic scattering and breakup reactions of the mirror nuclei 12B and 12N on 208Pb using ab initio structure inputs
doi: 10.1103/PhysRevC.109.014624
2023LE12 Phys.Rev. C 108, 034612 (2023) Advancing the Ichimura-Austern-Vincent model with continuum-discretized coupled-channels wave functions for realistic descriptions of two-body projectile breakup
doi: 10.1103/PhysRevC.108.034612
2023PA16 Phys.Rev. C 107, 064613 (2023) K.Palli, A.Pakou, A.M.Moro, P.D.O'Malley, L.Acosta, A.M.Sanchez-Benitez, G.Souliotis, E.F.Aguilera, E.Andrade, D.Godos, O.Sgouros, V.Soukeras, C.Agodi, T.L.Bailey, D.W.Bardayan, C.Boomershine, M.Brodeur, F.Cappuzzello, S.Carmichael, M.Cavallaro, S.Dede, J.A.Duenas, J.Henning, K.Lee, W.S.Porter, F.Rivero, W.von Seeger Quasielastic scattering of 7Be + natZr at sub- and near-barrier energies NUCLEAR REACTIONS Zr(7Be, X), E=20.6, 22.1, 23.7, 28.2 MeV; measured reaction product, charged particles, angular distributions; deduced quasielastic scattering σ(θ), total σ(E), optical model parameters. Optical model analysis. Comparison to phenomenological predictions and Continuum-Discretized Coupled-Channel (CDCC) calculations. Systematics of total fusion cross-sections for 7Li+59Co, 7Li+64Ni, 7Li+124Sn, 7Be+90Zr. Setup consisting of 4 silicon DSSD telescopes at Notre Dame FN tandem accelerator.
doi: 10.1103/PhysRevC.107.064613
2023PU01 Phys.Rev. C 108, 024613 (2023) Transfer reactions of exotic nuclei including core deformations: 11Be and 17C NUCLEAR REACTIONS 16C(d, p)17C, E=17.2 MeV/nucleon; 11Be(p, d)10Be, E=26.9, 35.3 MeV/nucleon; calculated σ(θ), spectroscopic factors. Adiabatic distorted-wave approximation (ADWA) calculations. Comparison to experimental data. NUCLEAR STRUCTURE 17C, 11Be; calculated levels, J, π, wave function components for ground- and first-excited states. Nilsson and a semimicroscopic particle-rotor model using antisymmetrized molecular dynamic calculations of the cores. Comparison to experimental data.
doi: 10.1103/PhysRevC.108.024613
2023SA13 Eur.Phys.J. A 59, 48 (2023) O.C.B.Santos, R.Lichtenthaler, A.M.Moro, K.C.C.Pires, U.Umbelino, A.S.Serra, E.O.N.Zevallo, A.L.de Lara, V.Scarduelli, J.Alcantara-Nunez, A.Lepine-Szily, J.Lei, S.Appannababu, M.Assuncao One-neutron stripping from 8Li projectiles to 9Be target nuclei NUCLEAR REACTIONS 9Be(8Li, 7Li), E=23.8 MeV; measured reaction products; deduced σ(θ), σ(θ, E). Comparison with optical model calculations using standard Woods-Saxon potentials. The RIBRAS (Radioactive Ion Beams in Brasil) facility.
doi: 10.1140/epja/s10050-023-00959-z
2022CA10 Phys.Lett. B 829, 137067 (2022) M.Caamano, T.Roger, A.M.Moro, G.F.Grinyer, J.Pancin, S.Bagchi, S.Sambi, J.Gibelin, B.Fernandez-Dominguez, N.Itagaki, J.Benlliure, D.Cortina-Gil, F.Farget, B.Jacquot, D.Perez-Loureiro, B.Pietras, R.Raabe, D.Ramos, C.Rodriguez-Tajes, H.Savajols, M.Vandebrouck Experimental investigation of ground-state properties of 7H with transfer reactions NUCLEAR REACTIONS 19F, 12C(8He, 7H), E=15.4 MeV/nucleon; measured reaction products. 7H; deduced resonance parameters, mass, T1/2, σ(θ). Comparison with available data.
doi: 10.1016/j.physletb.2022.137067
2022DI05 Phys.Lett. B 832, 137256 (2022) A.Di Pietro, A.C.Shotter, J.P.Fernandez-Garcia, P.Figuera, M.Fisichella, A.M.Moro, M.Alcorta, M.J.G.Borge, T.Davinson, F.Ferrera, A.M.Laird, M.Lattuada, N.Soic, O.Tengblad, D.Torresi, M.Zadro Hints of quasi-molecular states in 13B via the study of 9Li-4He elastic scattering NUCLEAR REACTIONS 4He(9Li, 9Li), (9Li, X), E(cm)=5-9.5 MeV; measured reaction products, TOF. 13B; deduced energy spectrum, broad resonances, σ(θ). R-matrix analysis. The Thick Target Inverse Kinematics technique, the TRIUMF laboratory (Canada) using a 32 MeV 9Li beam delivered by ISAC-II.
doi: 10.1016/j.physletb.2022.137256
2022HA15 Prog.Part.Nucl.Phys. 125, 103951 (2022) Coupled-channels calculations for nuclear reactions: From exotic nuclei to superheavy elements NUCLEAR REACTIONS 12C(p, p), E<200 MeV; 12C, 24Mg(α, X), E<400 MeV; 16O(16O, 16O), E=70 MeV/nucleon; 12C(d, np), E=12 MeV; 1H(6He, 6He), E=25, 41 MeV/nucleon; 1H(11Be, X), E=63.7 MeV/nucleon; 197Au(11Be, X), E(cm)=29.64, 37.1 MeV; 248Cm(48Ca, X), E<200 MeV; calculated σ(θ), σ. Comparison with experimental data. NUCLEAR STRUCTURE 11Li, 12Be, 22C, 24Mg; calculated energy levels, J, π.
doi: 10.1016/j.ppnp.2022.103951
2022KU28 Phys.Lett. B 833, 137294 (2022) K.Kundalia, D.Gupta, Sk M.Ali, Swapan K.Saha, O.Tengblad, J.D.Ovejas, A.Perea, I.Martel, J.Cederkall, J.Park, S.Szwec, A.M.Moro Study of elastic and inelastic scattering of 7Be + 12C at 35 MeV NUCLEAR REACTIONS 12C(7Be, 7Be), (7Be, 7Be'), E=35 MeV; measured reaction products; deduced σ(θ), deformation length. Optical model analyses with Woods-Saxon and double-folding potential using the density dependent M3Y (DDM3Y) effective interaction. CERN HIE-ISOLDE radioactive ion beam facility, utilizing the Scattering Experiments Chamber (SEC) at the XT03 beamline.
doi: 10.1016/j.physletb.2022.137294
2022ZA04 Phys.Rev. C 106, 014622 (2022) V.A.B.Zagatto, M.Gomez-Ramos, L.R.Gasques, A.M.Moro, L.C.Chamon, M.A.G.Alvarez, V.Scarduelli, J.P.Fernandez-Garcia, J.R.B.de Oliveira, A.Lepine-Szily, A.Arazi Elastic, inelastic, and one-neutron transfer angular distributions of 6Li + 120Sn at energies near the Coulomb barrier NUCLEAR REACTIONS 120Sn(6Li, 6Li), (6Li, 7Li), E=19, 24, 27 MeV; measured reaction products, angular distributions; deduced elastic, inelastic and neutron transfer σ(θ). Comparison to continuum-discretized coupled channels (CDCC) calculations. SATURN (silicon array based on telescopes of USP for reactions and nuclear applications) and STAR (silicon telescopes array for reactions) at tandem accelerator at the LAFN-USP laboratory.
doi: 10.1103/PhysRevC.106.014622
2021AU02 Prog.Part.Nucl.Phys. 118, 103847 (2021) T.Aumann, C.Barbieri, D.Bazin, C.A.Bertulani, A.Bonaccorso, W.H.Dickhoff, A.Gade, M.Gomez-Ramos, B.P.Kay, A.M.Moro, T.Nakamura, A.Obertelli, K.Ogata, S.Paschalis, T.Uesaka Quenching of single-particle strength from direct reactions with stable and rare-isotope beams
doi: 10.1016/j.ppnp.2021.103847
2021GO05 Eur.Phys.J. A 57, 57 (2021) M.Gomez-Ramos, J.Gomez-Camacho, J.Lei, A.M.Moro The Hussein-McVoy formula for inclusive breakup revisited NUCLEAR REACTIONS 9Be(14O, 13N), E=80 MeV/nucleon; 9Be(14O, 13O), E=53 MeV/nucleon; calculated integrated nonelastic breakup σ.
doi: 10.1140/epja/s10050-021-00376-0
2021HO15 Phys.Lett. B 822, 136710 (2021) M.Holl, R.Kanungo, Z.H.Sun, G.Hagen, J.A.Lay, A.M.Moro, P.Navratil, T.Papenbrock, M.Alcorta, D.Connolly, B.Davids, A.Diaz Varela, M.Gennari, G.Hackman, J.Henderson, S.Ishimoto, A.I.Kilic, R.Krucken, A.Lennarz, J.Liang, J.Measures, W.Mittig, O.Paetkau, A.Psaltis, S.Quaglioni, J.S.Randhawa, J.Smallcombe, I.J.Thompson, M.Vorabbi, M.Williams Proton inelastic scattering reveals deformation in 8He NUCLEAR REACTIONS 1H(8He, p), E=8.25 MeV/nucleon; measured reaction products, Ep, Ip. 8He; deduced σ(θ), resonance parameters, first 2+ state, quadrupole deformation parameter. Comparison with no-core shell model predictions. Charged particle spectroscopy station IRIS at TRIUMF in Canada.
doi: 10.1016/j.physletb.2021.136710
2021LI58 Phys.Rev. C 104, 044331 (2021) B.D.Linh, A.Corsi, A.Gillibert, A.Obertelli, P.Doornenbal, C.Barbieri, S.Chen, L.X.Chung, T.Duguet, M.Gomez-Ramos, J.D.Holt, A.Moro, P.Navratil, K.Ogata, N.T.T.Phuc, N.Shimizu, V.Soma, Y.Utsuno, N.L.Achouri, H.Baba, F.Browne, D.Calvet, F.Chateau, N.Chiga, M.L.Cortes, A.Delbart, J.-M.Gheller, A.Giganon, C.Hilaire, T.Isobe, T.Kobayashi, Y.Kubota, V.Lapoux, H.N.Liu, T.Motobayashi, I.Murray, H.Otsu, V.Panin, N.Paul, W.Rodriguez, H.Sakurai, M.Sasano, D.Steppenbeck, L.Stuhl, Y.L.Sun, Y.Togano, T.Uesaka, K.Wimmer, K.Yoneda, O.Aktas, T.Aumann, F.Flavigny, S.Franchoo, I.Gasparic, R.-B.Gerst, J.Gibelin, K.I.Hahn, N.T.Khai, D.Kim, T.Koiwai, Y.Kondo, P.Koseoglou, J.Lee, C.Lehr, T.Lokotko, M.MacCormick, K.Moschner, T.Nakamura, S.Y.Park, D.Rossi, E.Sahin, D.Sohler, P.-A.Soderstrom, S.Takeuchi, N.D.Ton, H.Tornqvist, V.Vaquero, V.Wagner, H.Wang, V.Werner, X.Xu, Y.Yamada, D.Yan, Z.Yang, M.Yasuda, L.Zanetti Investigation of the ground-state spin inversion in the neutron-rich 47, 49Cl isotopes NUCLEAR REACTIONS 1H(50Ar, 2p)49Cl, (50Ar, 2n2p)47Cl; 1H(52K, n3p)49Cl; 1H(48Cl, np)47Cl, [secondary ion beams from 9Be(70Zn, X), E=345 MeV/nucleon primary reaction at RIBF-RIKEN facility, followed by separation of ions by BigRIPS separator using Bπ-ΔE-TOF measurement and MINOS hydrogen target system]; measured reaction products, A/Q versus Z plot, scattered ions of 47Cl and 49Cl using the SAMURAI spectrometer and identified by A/Q and Z, Eγ, Iγ, γγ-coin using DALI2+ array of 226 NaI(Tl) detectors. 47,49Cl; deduced levels, J and π for 49Cl, parallel and transverse momentum distributions and L-transfers for 49Cl, inclusive cross sections. Comparison of experimental level structure with shell-model calculations using SDPF-MU interactions, and IMSRG calculation. Comparison of momentum distributions with distorted-wave impulse approximation (DWIA), and transfer to continuum (TC) methods. Comparison of inclusive cross sections with LISE++ theoretical calculations. 49Cl; calculated levels, J, π, T1/2 of levels, B(E2), B(M1) using SDFP-MU shell-model. 45,47,49Cl; calculated levels, J, π, spectroscopic factors using shell-model and ab initio approaches. 41,43,45,47Cl; spin inversion issue not settled. Comparison of experimental and theoretical (from CGF) energy difference between the first 1/2+ and 3/2+ states in 35,36,37,38,39,40,41,43,45,47,49,51,53Cl, 37,38,39,40,41,43,45,47,49,51,53,55K.
doi: 10.1103/PhysRevC.104.044331
2021MO04 Phys.Rev. C 103, 014604 (2021) L.Moschini, A.M.Moro, A.Vitturi Role of continuum in nuclear direct reactions with one-neutron halo nuclei: A one-dimensional model
doi: 10.1103/PhysRevC.103.014604
2021SA25 Phys.Rev. C 103, 064601 (2021) O.C.B.Santos, R.Lichtenthaler, K.C.C.Pires, U.Umbelino, E.O.N.Zevallos, A.L.de Lara, A.S.Serra, V.Scarduelli, J.Alcantara-Nunez, V.Guimaraes, A.Lepine-Szily, J.C.Zamora, A.M.Moro, S.Appannababu, M.Assuncao, A.Barioni, R.Linares, V.A.B.Zagatto, P.N.de Faria, M.C.Morais, V.Morcelle, J.M.B.Shorto, J.Lei Evidence of the effect of strong stripping channels on the dynamics of the 8Li + 58Ni reaction NUCLEAR REACTIONS 58Ni(8Li, 8Li), (8Li, 8Li'), (8Li, 7Li), E=23.9, 26.1, 28.7, 30 MeV, [secondary 8Li beam produced in 9Be(7Li, 8Li), E=26-32 MeV using the RIBRAS facility at the 8-UD Pelletron accelerator of the University of Sao Paulo]; measured reaction products, two-dimensional ΔE-E particle spectra, elastic σ(θ). Comparison with optical model and continuum discretized coupled channels (CDCC) calculations for the elastic and nonelastic breakup or particle-transfer processes.
doi: 10.1103/PhysRevC.103.064601
2021SP06 Phys.Lett. B 820, 136477 (2021) R.Sparta, A.Di Pietro, P.Figuera, O.Tengblad, A.M.Moro, I.Martel, J.P.Fernandez-Garcia, J.Lei, L.Acosta, M.J.G.Borge, G.Bruni, J.Cederkall, T.Davinson, J.D.Ovejas, L.M.Fraile, D.Galaviz, J.H.Jensen, B.Jonson, M.La Cognata, A.Perea, A.M.Sanchez-Benitez, N.Soic, S.Vinals Probing proton halo effects in the 8B+64Zn collision around the Coulomb barrier NUCLEAR REACTIONS 64Zn(8B, 8B), (8B, X)7Be, E=4.9 MeV/nucleon; measured reaction products. 8B; deduced σ(θ, E). Comparison with continuum-discretized coupled-channels (CDCC) calculations.
doi: 10.1016/j.physletb.2021.136477
2021WA12 Phys.Rev. C 103, 024606 (2021) K.Wang, Y.Y.Yang, A.M.Moro, V.Guimaraes, J.Lei, D.Y.Pang, F.F.Duan, J.L.Lou, J.C.Zamora, J.S.Wang, Z.Y.Sun, H.J.Ong, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, X.X.Xu, Z.H.Gao, G.Yang, S.Y.Jin, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu, for the RIBLL Collaboration Elastic scattering and breakup reactions of the proton drip-line nucleus 8B on 208Pb at 238 MeV NUCLEAR REACTIONS 208Pb(3He, 3He), E=55 MeV; 208Pb(8B, 8B), (8B, X), E=238 MeV; 208Pb(7Be, 7Be), (7Be, X), E=175 MeV, [3He, 7Be and 8B secondary beams from 9Be(12C, X), E=59.7 MeV primary reaction followed by ΔE-E particle identification of fragments at RIBLL-HIRFL-Lanzhou facility]; measured reaction products, particle spectra, using double-sided silicon strip detectors (DSSDs) and a CsI(Tl) crystal array; deduced σ(θ) for elastic scattering and inelastic breakup (NEB) of 8B and 7Be, no significant Coulomb rainbow suppression. Comparison with optical model and continuum discretized coupled channels (CDCC) calculations.
doi: 10.1103/PhysRevC.103.024606
2020DU18 Phys.Lett. B 811, 135942 (2020) F.F.Duan, Y.Y.Yang, K.Wang, A.M.Moro, V.Guimaraes, D.Y.Pang, J.S.Wang, Z.Y.Sun, J.Lei, A.Di Pietro, X.Liu, G.Yang, J.B.Ma, P.Ma, S.W.Xu, Z.Bai, X.X.Sun, Q.Hu, J.L.Lou, X.X.Xu, H.X.Li, S.Y.Jin, H.J.Ong, Q.Liu, J.S.Yao, H.K.Qi, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu Scattering of the halo nucleus 11Be from a lead target at 3.5 times the Coulomb barrier energy NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, X), E=140 MeV; 208Pb(10Be, X), (10Be, X), E=127 MeV; 208Pb(9Be, 9Be), (9Be, X), E=88 MeV; measured reaction products. 9,10,11Be; deduced σ(θ), σ(E), σ. Comparison with continuum discretized coupled channel (CDCC) as well as by the XCDCC calculations.
doi: 10.1016/j.physletb.2020.135942
2020GO16 Phys.Rev. C 102, 064613 (2020) M.Gomez-Ramos, A.Deltuva, A.M.Moro Benchmarking Faddeev and transfer-to-the-continuum calculations for (p, pN) reactions NUCLEAR REACTIONS 1H(11Be, np)10Be, E=100-400 MeV/nucleon; calculated transverse and longitudinal momentum distributions for removal of proton from different orbitals, and as function of binding energy. Distorted-wave impulse approximation, the Faddeev-AGS type formalism, and the transfer-to-the-continuum (TC) method, with realistic Reid93 interaction. Benchmarking the observables in proton-removal reactions.
doi: 10.1103/PhysRevC.102.064613
2020MO40 Phys.Lett. B 811, 135959 (2020) A.M.Moro, J.A.Lay, J.Gomez Camacho Determining B(E1) distributions of weakly bound nuclei from breakup cross sections using Continuum Discretized Coupled Channels calculations. Application to 11Be NUCLEAR REACTIONS 208Pb(11Be, X), E=69, 520 MeV/nucleon; analyzed available data. 11Be; deduced σ(θ), σ(E), B(E1) using of continuum discretized coupled channels (CDCC) calculations, in which both nuclear and Coulomb forces are taken into account to all orders.
doi: 10.1016/j.physletb.2020.135959
2020PE15 Phys.Lett. B 811, 135939 (2020) X.Pereira-Lopez, B.Fernandez-Dominguez, F.Delaunay, N.L.Achouri, N.A.Orr, W.N.Catford, M.Assie, S.Bailey, B.Bastin, Y.Blumenfeld, R.Borcea, M.Caamano, L.Caceres, E.Clement, A.Corsi, N.Curtis, Q.Deshayes, F.Farget, M.Fisichella, G.de France, S.Franchoo, M.Freer, J.Gibelin, A.Gillibert, G.F.Grinyer, F.Hammache, O.Kamalou, A.Knapton, T.Kokalova, V.Lapoux, J.A.Lay, B.Le Crom, S.Leblond, J.Lois-Fuentes, F.M.Marques, A.Matta, P.Morfouace, A.M.Moro, T.Otsuka, J.Pancin, L.Perrot, J.Piot, E.Pollacco, D.Ramos, C.Rodriguez-Tajes, T.Roger, F.Rotaru, M.Senoville, N.de Sereville, R.Smith, O.Sorlin, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, T.Suzuki, J.C.Thomas, N.Timofeyuk, M.Vandebrouck, J.Walshe, C.Wheldon Low-lying single-particle structure of 17C and the N=14 sub-shell closure NUCLEAR REACTIONS 2H(16C, p)17C, E=17.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), γ-ray energies, J, π, level scheme, spectroscopic factors. Comparison with shell model and particle-core model calculations.
doi: 10.1016/j.physletb.2020.135939
2019CO12 Phys.Lett. B 797, 134843 (2019) A.Corsi, Y.Kubota, J.Casal, M.Gomez-Ramos, A.M.Moro, G.Authelet, H.Baba, C.Caesar, D.Calvet, A.Delbart, M.Dozono, J.Feng, F.Flavigny, J.-M.Gheller, J.Gibelin, A.Giganon, A.Gillibert, K.Hasegawa, T.Isobe, Y.Kanaya, S.Kawakami, D.Kim, Y.Kiyokawa, M.Kobayashi, N.Kobayashi, T.Kobayashi, Y.Kondo, Z.Korkulu, S.Koyama, V.Lapoux, Y.Maeda, F.M.Marques, T.Motobayashi, T.Miyazaki, T.Nakamura, N.Nakatsuka, Y.Nishio, A.Obertelli, A.Ohkura, N.A.Orr, S.Ota, H.Otsu, T.Ozaki, V.Panin, S.Paschalis, E.C.Pollacco, S.Reichert, J.-Y.Rousse, A.T.Saito, S.Sakaguchi, M.Sako, C.Santamaria, M.Sasano, H.Sato, M.Shikata, Y.Shimizu, Y.Shindo, L.Stuhl, T.Sumikama, Y.L.Sun, M.Tabata, Y.Togano, J.Tsubota, T.Uesaka, Z.H.Yang, J.Yasuda, K.Yoneda, J.Zenihiro Structure of 13Be probed via quasi-free scattering NUCLEAR REACTIONS 1H(11Li, X), 246 MeV/nucleon; 1H(14Be, np)13Be, E=265 MeV/nucleon; 1H(17B, X), E=277 MeV/nucleon; measured reaction products, Ep, Ip, En, In, Eγ, Iγ. 12,13Be; deduced σ(E), partial level scheme, scattering lengths, resonance energies and widths, transverse momentum distributions.
doi: 10.1016/j.physletb.2019.134843
2019DI11 Phys.Lett. B 798, 134954 (2019) A.Di Pietro, A.M.Moro, J.Lei, R.de Diego Insights into the dynamics of breakup of the halo nucleus 11Be on a 64Zn target NUCLEAR REACTIONS 64Zn(11Be, X)10Be, E=28.7 MeV; analyzed available data; deduced quasielastic and breakup σ(θ), σ(θ, E) using CDCC and extended CDCC (XCDCC) calculations.
doi: 10.1016/j.physletb.2019.134954
2019FE05 Phys.Rev. C 99, 054605 (2019) J.P.Fernandez-Garcia, A.Di Pietro, P.Figuera, J.Gomez-Camacho, M.Lattuada, J.Lei, A.M.Moro, M.Rodriguez-Gallardo, V.Scuderi Breakup mechanisms in the 6He + 64Zn reaction at near-barrier energies NUCLEAR REACTIONS 64Zn(α, α), E=17.4 MeV; measured scattered α particles, differential σ(θ) using LEDA-type detectors and single-sided silicon strip detectors for particle detection at the Louvain la Neuve (Belgium) cyclotron facility; analyzed present data and previous experimental data at E(α)=13.2 MeV by optical model calculations based on the Sao Paulo potential. 64Zn(6He, 6He), (6He, α), E=14.85, 17.9 MeV; measured scattered particles, differential σ(θ) for outgoing 6He and α particles, the latter from 2n transfer process; analyzed present data and previous experimental data at E(6He)=9.8 and 13.5 MeV by optical model calculations, coupled-reaction-channel (CRC), continuum-discretized coupled channel (CDCC), and DWBA inclusive-breakup models.
doi: 10.1103/PhysRevC.99.054605
2019LE01 Phys.Rev.Lett. 122, 042503 (2019) Puzzle of Complete Fusion Suppression in Weakly Bound Nuclei: A Trojan Horse Effect? NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E<50 MeV; calculated σ, σ(E); deduced a new method to compute complete fusion σ in collisions involving weakly bound nuclei.
doi: 10.1103/PhysRevLett.122.042503
2019LE17 Phys.Rev.Lett. 123, 232501 (2019) Unraveling the Reaction Mechanisms Leading to Partial Fusion of Weakly Bound Nuclei NUCLEAR REACTIONS 209Bi(6Li, α), E<40 MeV; calculated σ(θ). Comparison with available data.
doi: 10.1103/PhysRevLett.123.232501
2019VA03 Phys.Rev. C 99, 034306 (2019) V.Vaquero, A.Jungclaus, P.Doornenbal, K.Wimmer, A.M.Moro, K.Ogata, T.Furumoto, S.Chen, E.Nacher, E.Sahin, Y.Shiga, D.Steppenbeck, R.Taniuchi, Z.Y.Xu, T.Ando, H.Baba, F.L.Bello Garrote, S.Franchoo, K.Hadynska-Klek, A.Kusoglu, J.Liu, T.Lokotko, S.Momiyama, T.Motobayashi, S.Nagamine, N.Nakatsuka, M.Niikura, R.Orlandi, T.Y.Saito, H.Sakurai, P.A.Soderstrom, G.M.Tveten, Zs.Vajta, M.Yalcinkaya In-beam γ-ray spectroscopy of 136Te at relativistic energies NUCLEAR REACTIONS C, 197Au(136Te, 136Te'), C(137Te, 136Te), E=139, 140 MeV/nucleon, [secondary 136,137Te beam from 9Be(238U, F), E=345 MeV/nucleon primary reaction]; measured Eγ, Iγ, γγ-coin, σ(θ), exclusive σ following Coulomb excitation to individual excited states using the DALI2 spectrometer array for γ detection, and the BigRIPS and ZeroDegree spectrometers for beam and product identification, respectively at RIBF-RIKEN facility. 136Te; deduced levels, J, π, B(E2) values. Comparison with theoretical predictions, and with previous experimental results. Systematics of B(E2) values for the first 2+ states in 132,134,136Te.
doi: 10.1103/PhysRevC.99.034306
2018GO21 Phys.Lett. B 785, 511 (2018) Binding-energy independence of reduced spectroscopic strengths derived from (p, 2p) and (p, pn) reactions with nitrogen and oxygen isotopes NUCLEAR REACTIONS 13,14,15,16,17,18,21,22,23O, 21N, 12C(p, 2p), 21N, 22,23O(p, np), E=300–450 MeV/nucleon; analyzed available data; calculated σ, spectroscopic factors.
doi: 10.1016/j.physletb.2018.08.058
2018LE02 Phys.Rev. C 97, 011601 (2018) Post-prior equivalence for transfer reactions with complex potentials NUCLEAR REACTIONS 58Ni(d, p), E=80 MeV; calculated angle-integrated proton energy spectra in inclusive transfer and breakup reactions; analyzed post-, and prior equivalence using model of Ichimura, Austern and Vincent (IAV) for post-forms and that of Udagawa and Tamura (UT) for prior-forms.
doi: 10.1103/PhysRevC.97.011601
2018MA56 Phys.Rev. C 98, 034615 (2018) G.Marquinez-Duran, I.Martel, A.M.Sanchez-Benitez, L.Acosta, J.L.Aguado, R.Berjillos, A.R.Pinto, T.Garcia, J.A.Duenas, K.Rusek, N.Keeley, K.W.Kemper, M.A.G.Alvarez, M.J.G.Borge, A.Chbihi, C.Cruz, M.Cubero, J.P.Fernandez-Garcia, B.Fernandez-Martinez, J.L.Flores, J.Gomez-Camacho, J.A.Labrador, F.M.Marques, A.M.Moro, M.Mazzocco, A.Pakou, V.V.Parkar, N.Patronis, V.Pesudo, D.Pierroutsakou, R.Raabe, R.Silvestri, N.Soic, L.Standylo, I.Strojek, O.Tengblad, R.Wolski, Z.Abou-Haidar Interaction of 8He with 208Pb at near-barrier energies: 4He and 6He production NUCLEAR REACTIONS 208Pb(8He, 6He), (8He, α), (8He, 8He), E=16, 22 MeV; measured reaction products, and differential σ(θ) using GLORIA detector array of SPIRAL-GANIL facility; deduced σ(2n)/σ(1n) ratio. Comparison with optical model and DWBA calculations. Inferred dominant neutron-stripping mechanism.
doi: 10.1103/PhysRevC.98.034615
2018YO03 Phys.Rev. C 97, 024608 (2018) K.Yoshida, M.Gomez-Ramos, K.Ogata, A.M.Moro Benchmarking theoretical formalisms for (p, pn) reactions: The 15C(p, pn)14C case NUCLEAR REACTIONS 15C(p, pn)14C, at momentum=420 MeV/c; calculated longitudinal and transversal momentum distribution in inverse kinematics using Faddeev equations due to Alt, Grassberger and Sandhas (FAGS), and compared with predictions of distorted-wave impulse approximation (DWIA), and transfer-to-continuum (TC) models.
doi: 10.1103/PhysRevC.97.024608
2017DE12 Phys.Rev. C 95, 044611 (2017) R.de Diego, R.Crespo, A.M.Moro Extracting three-body breakup observables from continuum-discretized coupled-channels calculations with core excitations NUCLEAR REACTIONS 1H(11Be, X), E=63.7 MeV/nucleon; 64Zn(11Be, X), E=28.7 MeV; calculated σ(θ, E) distributions, angle-integrated energy differential σ(E), and double differential σ(E, θ) as a function of the energy. Two- and three-body breakup observables of a two-body halo nucleus. Extended versions of Continuum-Discretized Coupled-Channels (XCDCC) and Transformed Harmonic Oscillator (THOx) methods with core excitation. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.044611
2017GO04 Phys.Rev. C 95, 034609 (2017) Interplay of projectile breakup and target excitation in reactions induced by weakly bound nuclei NUCLEAR REACTIONS 58Ni(d, d), (d, d'), E=80 MeV; 24Mg(d, d), (d, d'), E=70 MeV; 144Sm(6Li, 6Li), (6Li, 6Li'), E=23, 28, 30, 35 MeV; 9Be(6Li, 6Li), (6Li, 6Li'), E=20 MeV; calculated σ(q, E) for elastic and inelastic channels, and compared with experimental data. Extensions of the continuum discretized coupled channels (CDCC) method to include excitation of collective degrees of freedom of the target.
doi: 10.1103/PhysRevC.95.034609
2017GO08 Phys.Rev. C 95, 044612 (2017) Influence of target deformation and deuteron breakup in (d, p) transfer reactions NUCLEAR REACTIONS 10Be(d, p)11Be, E=10-80 MeV; calculated σ(E, θ), ratio between cross sections at the peak as function of the deuteron incident energy using extended continuum-discretized coupled-channel (CDCC) method with the inclusion of target excitations within the coupled-channel Born approximation (CDCC-BA) formulation, and also adiabatic coupled-channel (ACC) method. Comparison with calculations using Faddeev-Grassberger-Sandhas reaction formalism.
doi: 10.1103/PhysRevC.95.044612
2017LE02 Phys.Rev. C 95, 044605 (2017) Comprehensive analysis of large α yields observed in6Li-induced reactions NUCLEAR REACTIONS 208Pb(6Li, αX), E=29, 33, 35, 39 MeV; 144Sm(6Li, 6Li), E=22.1, 35.1 MeV; 159Tb(6Li, αX), E=23, 25, 27, 30, 35 MeV; 118Sn(6Li, 6Li), (6Li, αX), E=18, 19, 20, 21, 22.5, 24 MeV; 59Co(6Li, 6Li), E=18 MeV; 59Co(6Li, αX), E=21.5 MeV; 58Ni(6Li, 6Li), (6Li, αX), E=12, 14, 16, 18, 20 MeV; 209Bi(6Li, αX); analyzed σ(θ) data for α particles and elastic reactions; deduced elastic breakup (EBU) and nonelastic breakup (NEB) components of the inclusive breakup cross sections using continuum-discretized coupled-channels (CDCC) method.
doi: 10.1103/PhysRevC.95.044605
2017PE06 Phys.Rev.Lett. 118, 152502 (2017) V.Pesudo, M.J.G.Borge, A.M.Moro, J.A.Lay, E.Nacher, J.Gomez-Camacho, O.Tengblad, L.Acosta, M.Alcorta, M.A.G.Alvarez, C.Andreoiu, P.C.Bender, R.Braid, M.Cubero, A.Di Pietro, J.P.Fernandez-Garcia, P.Figuera, M.Fisichella, B.R.Fulton, A.B.Garnsworthy, G.Hackman, U.Hager, O.S.Kirsebom, K.Kuhn, M.Lattuada, G.Marquinez-Duran, I.Martel, D.Miller, M.Moukaddam, P.D.O'Malley, A.Perea, M.M.Rajabali, A.M.Sanchez-Benitez, F.Sarazin, V.Scuderi, C.E.Svensson, C.Unsworth, Z.M.Wang Scattering of the Halo Nucleus 11Be on 197Au at Energies around the Coulomb Barrier NUCLEAR REACTIONS 197Au(11Be, X), E=31.9 MeV; measured reaction products; deduced σ, σ(θ), B(E1). Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.118.152502
2017PO13 Eur.Phys.J. A 53, 178 (2017) G.Potel, G.Perdikakis, B.V.Carlson, M.C.Atkinson, W.H.Dickhoff, J.E.Escher, M.S.Hussein, J.Lei, W.Li, A.O.Macchiavelli, A.M.Moro, F.M.Nunes, S.D.Pain, J.Rotureau Toward a complete theory for predicting inclusive deuteron breakup away from stability NUCLEAR REACTIONS 93Nb(d, pn), E=10, 25.5 MeV; calculated σ(ln), σ(θn) assuming both elastic and nonelastic breakup. Compared with published calculations. 40,48,60Ca(d, pn), E=20, 40 MeV; calculated σ(Ep) vs En and vs ln using both elastic and nonelastic breakup and using Hussein-McVoy theory.
doi: 10.1140/epja/i2017-12371-9
2016CH12 Phys.Rev. C 93, 034623 (2016) J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, E.Ideguchi, H.J.Ong, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, N.T.Tho, J.Rangel, A.M.Moro, D.Y.Pang, J.Lee, J.Wu, H.N.Liu, C.Wen Elastic scattering and breakup of 11Be on protons at 26.9A MeV NUCLEAR REACTIONS 1H(11B, 11B), (11B, X), E=26.9 MeV/nucleon, [11B beam from 9Be(13C, X), E=60 MeV/nucleon]; measured 10,11Be, recoiled protons and deuterons, (10,11Be)p-coin, σ(θ) for elastic and breakup reactions using charged particle telescopes and annular silicon detectors at RCNP-Osaka accelerator facility. 11Be; deduced excitation energy spectrum for the ground state and the excited states. Analysis using Chapel Hill 89 (CH89) and Koning-Delaroche (KD) global optical model potentials (OMPs) for elastic scattering, and extended continuum-discretized coupled-channels (XCDCC) formalism for elastic scattering and breakup data.
doi: 10.1103/PhysRevC.93.034623
2016CH51 Phys.Rev. C 94, 064620 (2016) J.Chen, J.L.Lou, Y.L.Ye, J.Rangel, A.M.Moro, D.Y.Pang, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, T.D.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen Elastic scattering and breakup of 11Be on deuterons at 26.9A MeV NUCLEAR REACTIONS 2H(11Be, 11Be), (11Be, X), E=26.9 MeV/nucleon, [secondary 11Be beam from 9Be(13C, X), E=60 MeV/nucleon using EN-course beam line at RCNP-Osaka]; measured projectile-like isotopes and recoil light particles, (deuterons)(11Be)- and (deuterons)(10Be)-coin, angular distributions and angular correlations, elastic σ(θ) and breakup σ(θ) using TELE0 and TELE1 telescopes of double-sided silicon strip detector; deduced excitation energy spectrum for the ground state and unbound excited states of 11Be. Comparison of experimental cross sections with optical model calculations, and with continuum-discretized coupled-channels (XCDCC) formalism.
doi: 10.1103/PhysRevC.94.064620
2016DU18 Phys.Rev. C 94, 024614 (2016) Q.Ducasse, B.Jurado, M.Aiche, P.Marini, L.Mathieu, A.Gorgen, M.Guttormsen, A.C.Larsen, T.Tornyi, J.N.Wilson, G.Barreau, G.Boutoux, S.Czajkowski, F.Giacoppo, F.Gunsing, T.W.Hagen, M.Lebois, J.Lei, V.Meot, B.Morillon, A.M.Moro, T.Renstrom, O.Roig, S.J.Rose, O.Serot, S.Siem, I.Tsekhanovich, G.M.Tveten, M.Wiedeking Investigation of the 238U (d, p) surrogate reaction via the simultaneous measurement of γ-decay and fission probabilities NUCLEAR REACTIONS 238U(d, p)239U*, E=15 MeV; measured particle spectra Eγ, Iγ, (proton)γ- and (proton)(fission events)-coin using ΔE/E silicon telescope SiRi for particles and CACTUS array for γ rays at Oslo Cyclotron Laboratory; corrected data using continuum-discretized coupled channels calculations for elastic breakup, and DWBA for inelastic breakup; deduced excitation energy of 239U versus detected γ-ray energy, ratio between the γ-coincidence and the singles spectra, average angular momentum, γ-decay and fission probabilities as function of excitation energy and compared with JENDL 4.0, ENDF-B/VII.1 and JEFF 3.2 evaluated libraries, and corresponding neutron-induced data; calculated contributions to the total deuteron breakup process (TB) as a function of the excitation energy of 239U. Statistical model calculations for decay probabilities and average angular momentum.
doi: 10.1103/PhysRevC.94.024614
2016GU09 Phys.Rev. C 93, 064607 (2016) V.Guimaraes, J.J.Kolata, E.F.Aguilera, A.Howard, A.Roberts, F.D.Becchetti, R.O.Torres-Isea, A.Riggins, M.Febrarro, V.Scarduelli, P.N.de Faria, D.S.Monteiro, J.F.P.Huiza, A.Arazi, J.Hinnefeld, A.M.Moro, E.S.Rossi, V.Morcelle, A.Barioni, AlanJ.Mitchell Backscattering measurement of 6He on 209Bi: Critical interaction distance NUCLEAR REACTIONS 209Bi(6He, 6He), E=12, 14, 16 MeV, [secondary 6He beam from 2H(7Li, 6He), E=32 MeV]; measured 6He spectra using silicon ΔE-E telescope, σ(θ, E) at the TwinSol facility of Notre Dame Nuclear Structure Laboratory; deduced ratio of elastic to Rutherford cross sections. Comparison with a three-body CDCC calculation, and with experimental data for 209Bi(α, α), (6Li, 6Li), (9Be, 9Be), (12C, 12C), (16O, 16O), and 208Pb(6He, 6He) reactions.
doi: 10.1103/PhysRevC.93.064607
2016LA20 Phys.Rev. C 94, 021602 (2016) J.A.Lay, R.de Diego, R.Crespo, A.M.Moro, J.M.Arias, R.C.Johnson Evidence of strong dynamic core excitation in 19C resonant break-up NUCLEAR REACTIONS 1H(19C, X), E=70 MeV/nucleon; calculated differential σ(θ) for the first and the second 5/2+ resonance using XCDCC and XDDWBA approaches in valence-core model; deduced role of core excitations in the resonant breakup of 19C. Comparison with experimental data. NUCLEAR STRUCTURE 19C; calculated levels, J, π using shell-model with OXBASH and the WBP interaction, and within semimicroscopic core-plus-valence-particle model (P-AMD) using 18C as an inert core. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.021602
2016MA18 Acta Phys.Pol. B47, 841 (2016) G.Marquinez-Duran, A.M.Sanchez-Benitez, I.Martel, L.Acosta, K.Rusek, M.A.G.Alvarez, R.Berjillos, M.J.G.Borge, A.Chbihi, C.Cruz, M.Cubero, J.A.Duenas, J.P.Fernandez-Garcia, B.Fernandez-Martinez, J.L.Flores, J.Gomez-Camacho, N.Keeley, J.A.Labrador, M.Marques, A.M.Moro, M.Mazzocco, A.Pakou, V.V.Parkar, N.Patronis, V.Pesudo, D.Pierroutsakou, R.Raabe, R.Silvestri, N.Soic, L.Standylo, I.Strojek, O.Tengblad, R.Wolski, A.H.Zia Study of the Near-barrier Scattering of 8He on 208Pb NUCLEAR REACTIONS 208Pb(8He, 8He), E=22 MeV; measured reaction products; deduced σ.
doi: 10.5506/APhysPolB.47.841
2016MA79 Phys.Rev. C 94, 064618 (2016) G.Marquinez-Duran, I.Martel, A.M.Sanchez-Benitez, L.Acosta, R.Berjillos, J.Duenas, K.Rusek, N.Keeley, M.A.G.Alvarez, M.J.G.Borge, A.Chbihi, C.Cruz, M.Cubero, J.P.Fernandez-Garcia, B.Fernandez-Martinez, J.L.Flores, J.Gomez-Camacho, K.W.Kemper, J.A.Labrador, M.Marques, A.M.Moro, M.Mazzocco, A.Pakou, V.V.Parkar, N.Patronis, V.Pesudo, D.Pierroutsakou, R.Raabe, R.Silvestri, N.Soic, L.Standylo, I.Strojek, O.Tengblad, R.Wolski, Z.Abou-Haidar Precise measurement of near-barrier 8He+ 208Pb elastic scattering: Comparison with 6He NUCLEAR REACTIONS 208Pb(8He, 8He), E=22 MeV, [secondary 8He beam from C(13C, X), E=75 MeV/nucleon primary reaction using SPIRAL2 facility at GANIL]; measured scattered particles and reaction fragments, and angular distributions using the Global Reaction Array (GLORIA) detection system; deduced optical model parameters using optical model analysis for data from the present experiment and those from previous 208Pb(6He, 6He), E=22 MeV reaction, much longer range absorption for 6He as compared to that for 8He.
doi: 10.1103/PhysRevC.94.064618
2016MO06 Acta Phys.Pol. B47, 821 (2016) A.M.Moro, J.Lei, M.Gomez-Ramos, J.M.Arias, R.de Diego, J.Gomez-Camacho, J.A.Lay Recent Developments for the Calculation of Elastic and Non-elastic Breakup of Weakly-bound Nuclei
doi: 10.5506/APhysPolB.47.821
2016MO13 Few-Body Systems 57, 319 (2016) Recent Advances in Nuclear Reaction Theories for Weakly Bound Nuclei: Reexamining the Problem of Inclusive Breakup NUCLEAR REACTIONS 209Bi(6Li, 6Li), (6Li, α), E=30, 38 MeV; analyzed available σ data; deduced Elastic (EBU), non-elastic (NEB) and total breakup (TBU=EBU+NEB) and complete fusion (CF) σ, Eα, Iα. Comparison with available data.
doi: 10.1007/s00601-016-1085-1
2015FE09 Phys.Rev. C 92, 044608 (2015) J.P.Fernandez-Garcia, M.Cubero, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.A.Falou, B.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, M.Rodriguez-Gallardo, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden Simultaneous analysis of the elastic scattering and breakup channel for the reaction 11Li+208Pb at energies near the Coulomb barrier NUCLEAR REACTIONS 208Pb(11Li, 11Li), (11Li, X), (9Li, X), E=24.3, 29.8 MeV, [11Li beam from Ta(p, X), E=500 MeV from radioactive ion beam facility at TRIUMF]; measured 9,11Li elastic scattering and 9Li fragment spectra using detector telescopes, σ(θ), reaction and breakup σ; deduced energy distributions of the outgoing 9Li fragments from breakup of 11Li, B(E1) distributions of 11Li. Comparison to coupled-reaction-channel (CRC) and continuum-discretized coupled-channel (CDCC) calculations.
doi: 10.1103/PhysRevC.92.044608
2015FE10 Phys.Rev. C 92, 054602 (2015) J.P.Fernandez-Garcia, M.Zadro, A.Di Pietro, P.Figuera, M.Fisichella, O.Goryunov, M.Lattuada, C.Marchetta, A.M.Moro, A.Musumarra, V.Ostashko, M.G.Pellegriti, V.Scuderi, E.Strano, D.Torresi Effects of coupling to breakup in the 6, 7Li + 64Zn systems at near-barrier energies NUCLEAR REACTIONS 64Zn(7Li, 7Li), E=13.03, 13.85, 15.08, 16.60, 18.33, 20.18 MeV; measured charged-particle E-ΔE spectra, σ(θ, E) at INFN-LNS, Catania. Enriched target. 64Zn(6Li, 6Li), E(cm)=10.77, 11.69, 12.43, 13.54, 14.92, 16.30, 18.14, 19.98 MeV; analyzed experimental σ(θ, E) distributions. Continuum-discretized coupled-channels (CDCC) method analysis. Discussed effects of couplings to the breakup channels, and inclusion of resonant states in 6,7Li.
doi: 10.1103/PhysRevC.92.054602
2015GO13 Phys.Rev. C 92, 014613 (2015) M.Gomez-Ramos, A.M.Moro, J.Gomez-Camacho, I.J.Thompson Transfer induced by core excitation within an extended distorted-wave Born approximation method NUCLEAR REACTIONS 10Be(d, p)11Be, E=21.4 MeV; 30Ne(d, p)31Ne, E=30 MeV; calculated spectroscopic factors for 11Be, σ(θ) for ground and excited states of 11Be and 31Ne, cross sections excluding and including prompt core-excitation (PCE) effects. Extended distorted-wave Born approximation (DWBA) formalism. Comparison with available experimental data.
doi: 10.1103/PhysRevC.92.014613
2015LE15 Phys.Rev. C 92, 044616 (2015) Reexamining closed-form formulae for inclusive breakup: Application to deuteron- and 6Li-induced reactions NUCLEAR REACTIONS 93Nb(d, pX), E=25.5 MeV; 58Ni(d, pX), E=80, 100 MeV; 209Bi(6Li, 6Li), (6Li, αX), E=24-50 MeV; calculated σ(θ) distributions, angle integrated proton differential σ(Ep) and double-differential σ(Ep), σ(θ) for α particles in 6Li+209Bi reactions, inclusive breakup σ. Comparison with experimental data. DWBA version of the coupled-channels optical theorem for the nonelastic breakup and continuum-discretized coupled-channels (CDCC) framework for the elastic breakup (EBU).
doi: 10.1103/PhysRevC.92.044616
2015LE19 Phys.Rev. C 92, 061602 (2015) Numerical assessment of post-prior equivalence for inclusive breakup reactions NUCLEAR REACTIONS 62Ni(d, pX), E=25.5 MeV; calculated angle-integrated energy differential σ(Ep), double differential σ as a function of the proton energy. 209Bi(6Li, αX), E=36 MeV; calculated angle-integrated energy differential σ(Eα), σ(θ) for α using several models under the general distorted-wave Born approximation (DWBA) approach. Comparison of results from different models, and with experimental data. Post-prior equivalence in the calculation of nonelastic breakup (NEB) cross sections.
doi: 10.1103/PhysRevC.92.061602
2015MO21 Phys.Rev. C 92, 044605 (2015) Three-body model for the analysis of quasifree scattering reactions in inverse kinematics NUCLEAR REACTIONS 12C(p, p), E=200, 398 MeV; analyzed σ(θ) data using a microscopic folding potential. 12C(p, 2p), (p, np), E=400 MeV; calculated relative energy distributions of the outgoing protons, 1H(12C, np), (12C, 2p), E=400 MeV/nucleon; calculated transverse and longitudinal momentum distributions. 1H(23O, np), E=445 MeV/nucleon; calculated differential cross section as a function of the outgoing proton-neutron relative energy, transverse and longitudinal momentum distributions for the 22O residual nucleus. Three-body model approximated by a continuum-discretized coupled-channels (CDCC) wave function. Discussed role of final-state interactions and Pauli principle between the outgoing nucleons.
doi: 10.1103/PhysRevC.92.044605
2014DE15 Phys.Rev. C 89, 064609 (2014) R.de Diego, J.M.Arias, J.A.Lay, A.M.Moro Continuum-discretized coupled-channels calculations with core excitation NUCLEAR REACTIONS 1H(11Be, X), E=10, 63.7, 200 MeV/nucleon; calculated differential breakup σ(θ, E). 64Zn(11Be, X), E=28.7 MeV; calculated quasielastic and breakup differential σ(θ). 208Pb(11Be, X), E=69 MeV/nucleon; calculated breakup differential σ(θ). Scattering of a two-body halo nucleus. Dipole strength distribution for 11Be deduced from Coulomb breakup experiments. Extended version of Continuum-discretized coupled-channels (XCDCC) method with core excitation. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.064609
2014LA02 Phys.Rev. C 89, 014333 (2014) J.A.Lay, A.M.Moro, J.M.Arias, Y.Kanada-En'yo Semi-microscopic folding model for the description of two-body halo nuclei NUCLEAR STRUCTURE 19C, 11Be; calculated levels, J, π, spectroscopic factors for ground state and low-lying resonances for one-neutron halo nuclei. 10Be, 18C; calculated neutron and proton transition densities for ground state and first 2+ state, rms radii. Particle-plus-core model (PRM), particle-core folding potential based in antisymmetrized molecular dynamics (AMD) transition densities (P-AMD), and shell model calculations using WBT interaction. Comparison of levels, J, π with experimental data.
doi: 10.1103/PhysRevC.89.014333
2014MO06 Phys.Lett. B 732, 228 (2014) V.Morcelle, K.C.C.Pires, M.Rodriguez-Gallardo, R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, P.N.de Faria, D.R.Mendes, Jr, A.M.Moro, L.R.Gasques, E.Leistenschneider, R.P.Condori, V.Scarduelli, M.C.Morais, A.Barioni, J.C.Zamora, J.M.B.Shorto Four-body effects in the 6He + 58Ni scattering NUCLEAR REACTIONS 58Ni(6He, 6He), E=12.2, 16.5, 21.7 MeV; measured reaction products; deduced σ, four-body effects. Comparison with continuum-discretized coupled-channels calculation.
doi: 10.1016/j.physletb.2014.03.043
2014PE05 Acta Phys.Pol. B45, 375 (2014) V.Pesudo, M.J.G.Borge, A.M.Moro, E.Nacher, L.Acosta, M.Alcorta, M.A.G.Alvarez, G.C.Ball, P.C.Bender, R.Braid, M.Cubero, A.di Pietro, J.P.Fernandez-Garcia, P.Figuera, M.Fisichella, B.R.Fulton, A.B.Garnsworthy, J.Gomez-Camacho, G.Hackman, O.S.Kirsebom, K.Kuhn, R.Kruecken, M.Lattuada, J.A.Lay, G.Marquinez-Duran, I.Martel, D.Miller, M.Moukaddam, P.D.O'Malley, A.Perea, M.M.Rajabali, A.M.Sanchez-Benitez, F.Sarazin, V.Scuderi, C.E.Svensson, O.Tengblad, C.Unsworth, Z.M.Wang Reaction of the Halo Nucleus 11Be on Heavy Targets at Energies Around the Coulomb Barrier NUCLEAR REACTIONS 197Au(11Be, X), E=31.9 MeV; measured reaction products; deduced σ. Comparison with CDCC calculations.
doi: 10.5506/APhysPolB.45.375
2013FE04 Phys.Rev.Lett. 110, 142701 (2013) J.P.Fernandez-Garcia, M.Cubero, M.Rodriguez-Gallardo, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.A.Falou, B.R.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden 11Li Breakup on 208Pb at Energies Around the Coulomb Barrier NUCLEAR REACTIONS 208Pb(11Li, X), (11Li, 9Li), E=24.3, 29.8 MeV; measured reaction products. 9,11Li; deduced breakup probabilities angular and B(E1) distributions. Comparison with CDCC calculations, available data.
doi: 10.1103/PhysRevLett.110.142701
2013MA19 Acta Phys.Pol. B44, 467 (2013) G.Marquinez-Duran, A.M.Sanchez-Benitez, I.Martel, L.Acosta, K.Rusek, M.A.G.Alvarez, R.Berjillos, M.J.G.Borge, A.Chbihi, C.Cruz, M.Cubero, J.A.Duenas, J.P.Fernandez-Garcia, B.Fernandez Martinez, J.L.Flores, J.Gomez-Camacho, N.Keeley, J.A.Labrador, M.Marques, A.M.Moro, M.Mazzocco, A.Pakou, V.V.Parkar, N.Patronis, V.Pesudo, D.Pierroutsakou, R.Raabe, R.Silvestri, N.Soic, L.Standylo, I.Strojek, O.Tengblad, R.Wolski, A.H.Ziad Elastic Scattering of 8He + 208Pb at 22 MeV NUCLEAR REACTIONS 208Pb(8He, 8He), E=22 MeV; measured reaction products; deduced σ, σ(θ). Global reaction array, comparison with optical model calculations.
doi: 10.5506/APhysPolB.44.467
2013MI05 Phys.Rev. C 87, 054617 (2013) J.P.Mitchell, G.V.Rogachev, E.D.Johnson, L.T.Baby, K.W.Kemper, A.M.Moro, P.Peplowski, A.S.Volya, I.Wiedenhover Structure of 8B from elastic and inelastic 7Be+p scattering NUCLEAR REACTIONS 1H(7Be, 7Be), (7Be, 7Be'), [secondary 7Be from 1H(7Li, 7Bi), E=9 MeV primary reaction], E=18.5, 22, 27.2 MeV; measured particle spectra, (7Be)p-coin, differential σ(E) at FSU accelerator facility. 8B; deduced levels, resonances, J, π, proton and total widths, spectroscopic factors, phase shifts. 7Be(p, p), (p, p'); analysis of excitation function by R-matrix method. 7Li(n, γ); calculated σ as function of excitation energy using TDCSM model. 7Li(n, n), (n, n'), E(cm)=0.1-1.4 MeV; analyzed σ by R-matrix theory. Comparison of σ and phase shifts with predictions of TDCSM model and ab initio no-core shell model coupled with the resonating group method (NCSM/RGM) calculations.
doi: 10.1103/PhysRevC.87.054617
2013SC05 Acta Phys.Pol. B44, 463 (2013) V.Scuderi, A.Di Pietro, A.M.Moro, L.Acosta, F.Amorini, M.J.G.Borge, P.Figuera, M.Fisichella, L.M.Fraile, J.Gomez-Camacho, H.Jeppesen, M.Lattuada, I.Martel, M.Milin, A.Musumarra, M.Papa, M.G.Pellegriti, F.Perez-Bernal, R.Raabe, G.Randisi, F.Rizzo, G.Scalia, O.Tengblad, D.Torresi, A.M.Vidal, D.Voulot, F.Wenander, M.Zadro Elastic Scattering for the 11Be + 64Zn System Close to the Coulomb Barrier NUCLEAR REACTIONS 64Zn(10Be, 10Be), (11Be, 11Be), E not given; measured reaction products; deduced σ, σ(θ). Comparison with optical model calculations.
doi: 10.5506/APhysPolB.44.463
2012CU02 Phys.Rev.Lett. 109, 262701 (2012) M.Cubero, J.P.Fernandez-Garcia, M.Rodriguez-Gallardo, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.Al Falou, B.R.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden Do Halo Nuclei Follow Rutherford Elastic Scattering at Energies Below the Barrier? The Case of 11Li NUCLEAR REACTIONS 208Pb(11Li, 11Li), (9Li, 9Li), E=23.9-43 MeV. 9,11Li; measured reaction products; deduced σ(θ), Rutherford σ. Four-body CDCC calculations with code FRESCO calculations.
doi: 10.1103/PhysRevLett.109.262701
2012DI08 Phys.Rev. C 85, 054607 (2012) A.Di Pietro, V.Scuderi, A.M.Moro, L.Acosta, F.Amorini, M.J.G.Borge, P.Figuera, M.Fisichella, L.M.Fraile, J.Gomez-Camacho, H.Jeppesen, M.Lattuada, I.Martel, M.Milin, A.Musumarra, M.Papa, M.G.Pellegriti, F.Perez-Bernal, R.Raabe, G.Randisi, F.Rizzo, G.Scalia, O.Tengblad, D.Torresi, A.M.Vidal, D.Voulot, F.Wenander, M.Zadro Experimental study of the collision 11Be + 64Zn around the Coulomb barrier NUCLEAR REACTIONS 64Zn(9Be, 9Be), E=29 MeV; 64Zn(10Be, 10Be), E=28.7 MeV; 64Zn(11Be, 11Be), E=28.4 MeV; 197Au(10Be, 10Be), E(cm)=27.9 MeV; 197Au(12C, 12C), E(cm)=25.7 MeV; measured particle spectra, elastic scattering σ(θ) at REX-ISOLDE-CERN facility and at LNS, Catania; deduced S matrix. Optical model and distorted-wave Born-approximation (DWBA) analysis. 64Zn(11Be, X), E=28.4 MeV; measured differential σ(θ) of transfer/breakup events; calculated σ(θ) by continuum-discretized coupled-channel (CDCC) calculations.
doi: 10.1103/PhysRevC.85.054607
2012KU25 Phys.Rev. C 86, 034601 (2012) Exclusive breakup of 17F on 58Ni and 208Pb within the continuum-discretized coupled-channels method NUCLEAR REACTIONS 58Ni, 208Pb(17F, 17F), (17F, X), E=10, 65 MeV/nucleon; calculated elastic σ(θ), differential and integrated breakup σ, σ(θ) angular distribution of protons and 16O fragments following the 17F dissociation, effect of different multipoles, role of Coulomb and nuclear couplings in the breakup cross sections. Continuum-discretized coupled-channels (CDCC) method, assuming 16O+p model for the projectile. Comparison with recent experimental data.
doi: 10.1103/PhysRevC.86.034601
2012LA12 Phys.Rev. C 85, 054618 (2012) J.A.Lay, A.M.Moro, J.M.Arias, J.Gomez-Camacho Particle motion in a deformed potential using a transformed oscillator basis NUCLEAR STRUCTURE 11Be; calculated wave functions of ground and excited states, level energies, level density, B(E1), B(E2). Pseudostate (PS) basis for a particle moving in a deformed potential, transformed harmonic oscillator (THO) functions, using a local scale transformation (LST). 10Be+n two body model. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054618
2012MO15 Phys.Rev. C 85, 054613 (2012) Core excitation effects in the breakup of the one-neutron halo nucleus 11Be on a proton target NUCLEAR REACTIONS 1H(11Be, p), E=63.7 MeV; calculated σ(θ), differential energy cross section for 10Be+n. Core excitation reaction model based on DWBA. Breakup of one-neutron halo 11Be nucleus. Comparison with continuum-discretized coupled-channels calculation, and with experimental data.
doi: 10.1103/PhysRevC.85.054613
2012MO32 Phys.Rev.Lett. 109, 232502 (2012) Interplay Between Valence and Core Excitation Mechanisms in the Breakup of Halo Nuclei NUCLEAR REACTIONS 12C(11Be, X), E=70 MeV/nucleon; analyzed available data; deduced spectroscopic factors, σ(θ), resonant breakup of 11Be. Comparison with DWBA calculations.
doi: 10.1103/PhysRevLett.109.232502
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
2011CR01 Phys.Rev. C 83, 044622 (2011) Core excitation contributions to the breakup of the one-neutron halo nucleus 11Be on a proton NUCLEAR REACTIONS 1H(11Be, X), E=63.7 MeV/nucleon; calculated angular distributions using core excited model, and single-scattering approximation of the three-body Faddeev-Alt-Grassberger-Sandhas equations. Breakup of the 11Be halo nucleus.
doi: 10.1103/PhysRevC.83.044622
2011CR02 Phys.Rev. C 83, 054613 (2011) R.Crespo, M.Rodriguez-Gallardo, A.M.Moro, A.Deltuva, E.Cravo, A.C.Fonseca Resonant breakup of 19C on a proton target NUCLEAR REACTIONS 1H(19C, p), E=70 MeV/nucleon; calculated differential energy distribution for the resonant breakup, σ(θ). Faddeev-Alt, Grassberger, Sandhas (Faddeev-AGS) and continuum-discretized coupled-channels (CDCC) reaction frameworks using three-body model (18C+n+p) for the reaction.
doi: 10.1103/PhysRevC.83.054613
2011FE06 Phys.Rev. C 84, 011301 (2011); Pub.Note JOUR PRVCA 84 029902 (2011) B.Fernandez-Dominguez, J.S.Thomas, W.N.Catford, F.Delaunay, S.M.Brown, N.A.Orr, M.Rejmund, M.Labiche, M.Chartier, N.L.Achouri, H.Al Falou, N.I.Ashwood, D.Beaumel, Y.Blumenfeld, B.A.Brown, R.Chapman, N.Curtis, C.Force, G.de France, S.Franchoo, J.Guillot, P.Haigh, F.Hammache, V.Lapoux, R.C.Lemmon, F.Marechal, A.M.Moro, X.Mougeot, B.Mouginot, L.Nalpas, A.Navin, N.Patterson, B.Pietras, E.C.Pollacco, A.Leprince, A.Ramus, J.A.Scarpaci, N.de Sereville, I.Stephan, O.Sorlin, G.L.Wilson Emergence of the N = 16 shell gap in 21O NUCLEAR REACTIONS 2H(20O, p), E=10.5 MeV/nucleon; measured E(p), I(p), Eγ, Iγ, σ(θ), p20O-, p20Oγ-coin. 21O; deduced levels, J, π, L-transfer, spectroscopic factors, configurations. Adiabatic distorted-wave approximation analysis of σ(θ) data. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.84.011301
2011GU29 J.Phys.:Conf.Ser. 312, 082024 (2011) V.Guimaraes, A.Lepine-Szily, R.Lichtenthaler, P.N.de Faria, A.Barioni, K.C.C.Pires, V.Morcelle, D.R.Mendes, J.C.Zamora, M.C.Morais, R.P.Condori, E.A.Benjamim, D.S.Monteiro, E.Crema, A.M.Moro, J.Lubian Low energy nuclear reactions with RIBRAS, Radioactive Ion Beam in Brazil, system COMPILATION 27Al(6He, X), 59Co(6Li, X), (7Li, X), 58Ni(6Li, X), (7Be, X), (8B, X), 64Zn(6He, X), (6Li, X), (7Li, X), (9Be, X), (16O, X), 209Bi(6He, X), E not given; compiled scaled reaction σ vs scaled energy.
doi: 10.1088/1742-6596/312/4/082024
2011PI08 Phys.Rev. C 83, 064603 (2011) K.C.C.Pires, R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, P.N.de Faria, A.Barioni, D.R.Mendes, Jr., V.Morcelle, R.P.Condori, M.C.Morais, J.C.Zamora, E.Crema, A.M.Moro, M.Rodriguez-Gallardo, M.Assuncao, J.M.B.Shorto, S.Mukherjee Experimental study of 6He+9Be elastic scattering at low energies NUCLEAR REACTIONS 9Be, 197Au(6He, 6He), E=16.2, 21.3 MeV, [6He secondary beam from 9Be(7Li, 6He), E=22.18, 26.10 MeV primary beam]; measured 6He spectra, cross sections, σ(θ), biparametric spectrum. Effect of the collective couplings to the excited states. Coupled channels calculations, using a double-folding potential, and three- and four-body continuum-discretized coupled-channels (CDCC) calculations.
doi: 10.1103/PhysRevC.83.064603
2011RO14 Int.J.Mod.Phys. E20, 947 (2011) M.Rodriguez-Gallardo, A.M.Moro Four-body continuum-discretized coupled-channel calculations applied to 6He reactions around the Coulomb barrier NUCLEAR REACTIONS 64Zn(6He, X), E=13.6 MeV; 120Sn(6He, X), E=17.4 MeV; 208Pb(6He, X), E=22 MeV; calculated σ. THO method, comparison with experimental data.
doi: 10.1142/S0218301311019039
2011TE06 Phys.Rev. C 84, 064616 (2011) E.Tengborn, A.M.Moro, T.Nilsson, M.Alcorta, M.J.G.Borge, J.Cederkall, C.Diget, L.M.Fraile, H.O.U.Fynbo, J.Gomez-Camacho, H.B.Jeppesen, H.T.Johansson, B.Jonson, O.S.Kirsebom, H.H.Knudsen, M.Madurga, G.Nyman, A.Richter, K.Riisager, G.Schrieder, O.Tengblad, N.Timofeyuk, M.Turrion, D.Voulot, F.Wenander The 8Li + 2H reaction studied in inverse kinematics at 3.15 MeV/nucleon using the REX-ISOLDE post-accelerator NUCLEAR REACTIONS 2H(8Li, p), (8Li, d), (8Li, t), [8Li beam from Ta(p, X), E=1.4 GeV primary reaction], E=3.15 MeV/nucleon; measured particle spectra, energy loss, σ(θ). 7,8,9Li; deduced levels, J, π, asymptotic normalization coefficients (ANC), Shell-model spectroscopic amplitudes. Coupled-channels and distorted-wave Born approximation (DWBA) analyses of σ(θ) data. REX-ISOLDE post-accelerator.
doi: 10.1103/PhysRevC.84.064616
2010AV07 Phys.Rev. C 82, 037601 (2010) Improved deuteron elastic breakup energy dependence via the continuum-discretized coupled-channels method NUCLEAR REACTIONS 63Cu, 93Nb(d, d), calculated σ, σ(θ) using continuum-discretized coupled-channels (CDCC) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.037601
2010CR01 Phys.Rev. C 81, 031601 (2010) E.Cravo, R.Crespo, A.M.Moro, A.Deltuva Probing nucleon-nucleon interactions in breakup of the one-neutron halo nucleus 11Be on a proton target NUCLEAR REACTIONS p(11Be, X), E=63.7 MeV/nucleon; calculated nucleon-nucleon (NN) phase shifts for s- and p-waves, σ(E), angular distributions using Faddeev/Alt-Grassberger-Sandhas and continuum-discretized coupled-channels (CDCC) methods for breakup of one-neutron halo nucleus. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.031601
2010DE14 Phys.Rev. C 81, 044605 (2010) P.N.de Faria, R.Lichtenthaler, K.C.C.Pires, A.M.Moro, A.Lepine-Szily, V.Guimaraes, D.R.Mendes, Jr., A.Arazi, M.Rodriguez-Gallardo, A.Barioni, V.Morcelle, M.C.Morais, O.Camargo, Jr., J.Alcantara Nunez, M.Assuncao Elastic scattering and total reaction cross section of 6He+120Sn NUCLEAR REACTIONS 120Sn(6He, 6He), E=17.40, 18.05, 19.80, 20.5 MeV; σ(E, θ). Comparison with optical model and continuum discretized coupled channels (CDCC) calculations.
doi: 10.1103/PhysRevC.81.044605
2010DE34 Phys.Rev. C 82, 034602 (2010) P.N.de Faria, R.Lichtenthaler, K.C.C.Pires, A.M.Moro, A.Lepine-Szily, V.Guimaraes, D.R.Mendes, Jr., A.Arazi, A.Barioni, V.Morcelle, M.C.Morais α-particle production in 6He+120Sn collisions NUCLEAR REACTIONS 120Sn(6He, 6He), (6He, X), E=17.4, 18.04, 19.8, 20.5 MeV, [6He beam from 9Be(7Li, 6He), E=2-26 MeV]; measured α and 6He spectra, σ(E, θ). DWBA analysis. Comparison with breakup and neutron transfer calculations using continuum-discretized coupled-channels (CDCC) approach.
doi: 10.1103/PhysRevC.82.034602
2010FE05 Phys.Lett. B 693, 310 (2010) J.P.Fernandez-Garcia, M.A.G.Alvarez, A.M.Moro, M.Rodriguez-Gallardo Simultaneous analysis of elastic scattering and transfer/breakup channels for the 6He + 208Pb reaction at energies near the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, 6He), (6He, α), E=14, 16, 18, 22, 27 MeV; calculated σ(θ), σ(E), σ, effective potentials. Coupled-Reaction-Channels (CRC) method.
doi: 10.1016/j.physletb.2010.07.060
2010FE09 Nucl.Phys. A840, 19 (2010) J.P.Fernandez-Garcia, M.Rodriguez-Gallardo, M.A.G.Alvarez, A.M.Moro Long range effects on the optical model of 6He around the Coulomb barrier NUCLEAR REACTIONS 27Al(6He, 6He), E=9.5, 11, 12, 13.4 MeV; 208Pb(6He, 6He), E=14, 16, 18, 22, 27 MeV; calculated σ(θ) using an optical model with various potentials and coupled-channels approach. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.03.013
2010LA09 Phys.Rev. C 82, 024605 (2010) J.A.Lay, A.M.Moro, J.M.Arias, J.Gomez-Camacho Exploring continuum structures with a pseudo-state basis NUCLEAR REACTIONS 12C, 208Pb(6He, 6He), E=240 MeV/nucleon; 12C(11Be, 11Be), E=67 MeV/nucleon; calculated differential σ(E), σ(θ), energy breakup differential σ(E), B(E1) and B(E2) transition probabilities for the 6He=α+2n system, and scattering phase shifts. Calculations based on treatment of a weakly bound system in terms square-integrable functions, or pseudo-state (PS) generated by a parametric local scale transformation (LST) to the transformed harmonic oscillator (HO) basis. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.024605
2010LE14 Nucl.Phys. A834, 491c (2010) A.Lepine-Szily, R.Lichtenthaler, V.Guimaraes, D.R.Mendes, Jr, P.N.de Faria, A.Barioni, E.A.Benjamim, K.C.C.Pires, V.Morcelle, R.P.Condori, M.C.Morais, P.Descouvemont, A.M.Moro, M.Rodriguez Gallardo, M.M.Assuncao, J.A.Alcantara Nunez, J.M.B.Shorto, J.C.Zamora, E.Leistenschneider, C.E.F.Lima Scientific program of the Radioactive Ion Beams Facility in Brasil (RIBRAS) NUCLEAR REACTIONS 1H(8Li, α), E=13.2, 14.5, 17.4, 19.0 MeV; measured Eα, Iα(θ=forward); deduced σ(θ=forward), effect of halo nuclei. 9Be(6He, 6He), E=16.2 MeV; measured σ(θ); deduced effect of halo nuclei.
doi: 10.1016/j.nuclphysa.2010.01.074
2010MI12 Phys.Rev. C 82, 011601 (2010) J.P.Mitchell, G.V.Rogachev, E.D.Johnson, L.T.Baby, K.W.Kemper, A.M.Moro, P.N.Peplowski, A.Volya, I.Wiedenhover Low-lying states in 8B NUCLEAR REACTIONS 1H(7Be, 7Be), (7Be, 7Be'), E=18.5, 22.0 MeV, [secondary 7Be beam from primary 1H(7Li, 7Be) reaction]; measured recoil proton and 7Be spectra, (proton)(7Be)-coin, excitation functions and angular distributions. 8B; deduced levels, J, π, partial proton widths and total widths. R-matrix and time-dependent continuum shell model (TDCSM) analysis. Comparison with low-lying level structure of mirror nucleus 8Li.
doi: 10.1103/PhysRevC.82.011601
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
2009BA42 Phys.Rev. C 80, 034617 (2009) A.Barioni, V.Guimaraes, A.Lepine-Szily, R.Lichtenthaler, D.R.Mendes, Jr., E.Crema, K.C.C.Pires, M.C.Morais, V.Morcelle, P.N.de Faria, R.P.Condori, A.M.Moro, D.S.Monteiro, J.M.B.Shorto, J.Lubian, M.Assuncao Elastic scattering and total reaction cross sections for the 8Li+12C system NUCLEAR REACTIONS 12C(8Li, 8Li), (8Li, 9Be)11B, E=23.9 MeV; measured particle spectra, σ, σ(θ); deduced spectroscopic factors. Optical-model analysis with Woods-Saxon and double-folding Sao Paulo potential. Coupled-channel analysis for breakup and inelastic channels. Comparison of spectroscopic factors with shell-model calculations and previous experimental data.
doi: 10.1103/PhysRevC.80.034617
2009BE46 Phys.Rev. C 80, 064617 (2009) T.L.Belyaeva, E.F.Aguilera, E.Martinez-Quiroz, A.M.Moro, J.J.Kolata Astrophysical S17(0) factor extraction from breakup of 8B on 58Ni at energies near the Coulomb barrier NUCLEAR REACTIONS 58Ni(7Be, 7Be), (8B, 8B), (8B, 7Be), (8B, X), E=15-30 MeV; calculated σ(θ) for elastic, single-proton transfer and breakup channels using continuum-discretized coupled channels (CDCC) method. Comparison with experimental data; deduced astrophysical S17(O) factor.
doi: 10.1103/PhysRevC.80.064617
2009MO36 Phys.Rev. C 80, 054605 (2009) A.M.Moro, J.M.Arias, J.Gomez-Camacho, F.Perez-Bernal Analytical transformed harmonic oscillator basis for continuum discretized coupled channels calculations NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; 40Ca(6Li, 6Li), (6Li, X), E=156 MeV; 208Pb(6He, 6He), (6He, X), E=22 MeV, 240 MeV/nucleon; calculated elastic σ(θ), and breakup S-matrix elements using continuum-discretized coupled-channels (CDCC) method.
doi: 10.1103/PhysRevC.80.054605
2009MO39 Phys.Rev. C 80, 064606 (2009) A.M.Moro, F.M.Nunes, R.C.Johnson Theory of (d, p) and (p, d) reactions including breakup: Comparison of methods NUCLEAR REACTIONS 11Be(p, d), E=38.4 MeV/nucleon; 10Be(d, p), E=12.5 MeV/nucleon; calculated σ and σ(θ) using continuum discretized coupled channel (CDCC) and full three body integral (AGS) equations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.064606
2009RO26 Phys.Rev. C 80, 051601 (2009) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations NUCLEAR REACTIONS 208Pb(6He, X), E=22 MeV; calculated σ(θ), angular distributions , B(E1) and B(E2) distributions using continuum-discretized coupled channels calculations. calculated . Comparison with experimental data.
doi: 10.1103/PhysRevC.80.051601
2008RO16 Phys.Rev. C 77, 064609 (2008) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, R.C.Johnson, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations using a transformed harmonic oscillator basis NUCLEAR REACTIONS 12C(6He, 6He), E=229.8 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 208Pb(6He, 6He), E=22 MeV; calculated energy spectra, σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064609
2008RU10 Phys.Rev. C 78, 034603 (2008) O.A.Rubtsova, V.I.Kukulin, A.M.Moro Continuum discretization methods in a composite particle scattering off a nucleus: Benchmark calculations NUCLEAR REACTIONS 58Ni(d, d), E=12, 21.6, 80 MeV; calculated σ, σ(θ). Continuum discretized coupled channels method, wave-packet continuum discretization method.
doi: 10.1103/PhysRevC.78.034603
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
2007AL08 Phys.Rev. C 75, 024608 (2007) J.S.Al-Khalili, R.Crespo, R.C.Johnson, A.M.Moro, I.J.Thompson Few-body multiple scattering calculations for 6He on protons NUCLEAR REACTIONS 1H(α, α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; calculated elastic σ(θ). Multiple scattering expansion, comparison with data.
doi: 10.1103/PhysRevC.75.024608
2007AM10 Eur.Phys.J. Special Topics 150, 1 (2007) H.Amro, F.D.Becchetti, Y.Chen, H.Jiang, M.Ojaruega, M.J.Golobish, H.C.Griffin, J.J.Kolata, B.Skorodumov, G.Peaslee, P.A.DeYoung, P.Mears, D.Denby, J.Brown, J.D.Hinnefeld, A.M.Moro 7Be-induced α -transfer reaction on 12C NUCLEAR REACTIONS 12C(7Be, 3He), E=34 MeV; measured σ and angular distributions.
doi: 10.1140/epjst/e2007-00250-4
2007BE19 Phys.Lett. B 647, 30 (2007) E.A.Benjamim, A.Lepine-Szily, D.R.Mendes, Jr., R.Lichtenthaler, V.Guimaraes, P.R.S.Gomes, L.C.Chamon, M.S.Hussein, A.M.Moro, A.Arazi, I.Padron, J.Alcantara Nunez, M.Assuncao, A.Barioni, O.Camargo, Jr., R.Z.Denke, P.N.de Faria, K.C.C.Pires Elastic scattering and total reaction cross section for the 6He + 27Al system NUCLEAR REACTIONS 27Al(6He, 6He), E=9.5, 11.0, 12.0, 13.4 MeV; measured σ, σ(θ). 6He deduced radius, deformation parameters. 27Al(6Li, 6Li), (7Li, 7Li), (9Be, 9Be), (16O, 16O), E≈7-45 MeV; analysed total σ. 6,7Li, 9Be, 16O deduced deformation parameters. Sao Paulo potential.
doi: 10.1016/j.physletb.2007.01.048
2007CR06 Phys.Rev. C 76, 054607 (2007) Polarization observables in the elastic scattering of protons from 4, 6, 8He NUCLEAR REACTIONS 4,6,8He(p, p), E=297 MeV; calculated matter density, cross sections, polarizations using optical model.
doi: 10.1103/PhysRevC.76.054607
2007CR07 Eur.Phys.J. Special Topics 150, 13 (2007) R.Crespo, A.M.Moro, I.J.Thompson, M.Rodriguez-Gallardo, J.Gomez-Camacho, J.M.Arias Exploring the 6He continuum sea through proton inelastic collisions NUCLEAR REACTIONS 6He(p, p'), E=717 MeV; calculated σ(θ) using the MST framework.
doi: 10.1140/epjst/e2007-00253-1
2007DE59 Phys.Rev. C 76, 064602 (2007) A.Deltuva, A.M.Moro, E.Cravo, F.M.Nunes, A.C.Fonseca Three-body description of direct nuclear reactions: Comparison with the continuum discretized coupled channels method NUCLEAR REACTIONS 12C(d, X), E=56 MeV; 58Ni(d, X), E=80 MeV; p(11Be, X), E=38.4 MeV/nucleon; calculated cross-sections, angular distributions using continuum discretized coupled channels. Comparisons with solution to three-body Faddeev equations and experiment.
doi: 10.1103/PhysRevC.76.064602
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