NSR Query Results


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NSR database version of April 11, 2024.

Search: Author = A.M.Moro

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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
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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
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2023LE12      Phys.Rev. C 108, 034612 (2023)

J.Lei, A.M.Moro

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
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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
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2023PU01      Phys.Rev. C 108, 024613 (2023)

P.Punta, J.A.Lay, A.M.Moro

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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2809. Data from this article have been entered in the XUNDL database. For more information, click here.


2022HA15      Prog.Part.Nucl.Phys. 125, 103951 (2022)

K.Hagino, K.Ogata, A.M.Moro

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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1026.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2684.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1004.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0265.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0235.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8032. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2633. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1856.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2458.


2019LE01      Phys.Rev.Lett. 122, 042503 (2019)

J.Lei, A.M.Moro

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
Citations: PlumX Metrics


2019LE17      Phys.Rev.Lett. 123, 232501 (2019)

J.Lei, A.M.Moro

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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2018GO21      Phys.Lett. B 785, 511 (2018)

M.Gomez-Ramos, A.M.Moro

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
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2018LE02      Phys.Rev. C 97, 011601 (2018)

J.Lei, A.M.Moro

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2416.


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
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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
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2017GO04      Phys.Rev. C 95, 034609 (2017)

M.Gomez-Ramos, A.M.Moro

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
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2017GO08      Phys.Rev. C 95, 044612 (2017)

M.Gomez-Ramos, A.M.Moro

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
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2017LE02      Phys.Rev. C 95, 044605 (2017)

J.Lei, A.M.Moro

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2259.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2502.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2527.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2326.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2326.


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
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2016MO13      Few-Body Systems 57, 319 (2016)

A.M.Moro, J.Lei

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2195.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2331.


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
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2015LE15      Phys.Rev. C 92, 044616 (2015)

J.Lei, A.M.Moro

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
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2015LE19      Phys.Rev. C 92, 061602 (2015)

J.Lei, A.M.Moro

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
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2015MO21      Phys.Rev. C 92, 044605 (2015)

A.M.Moro

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1856.


2012KU25      Phys.Rev. C 86, 034601 (2012)

Y.Kucuk, A.M.Moro

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
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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
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2012MO15      Phys.Rev. C 85, 054613 (2012)

A.M.Moro, R.Crespo

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
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2012MO32      Phys.Rev.Lett. 109, 232502 (2012)

A.M.Moro, J.A.Lay

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1958.


2011CR01      Phys.Rev. C 83, 044622 (2011)

R.Crespo, A.Deltuva, A.M.Moro

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1915. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1971. Data from this article have been entered in the XUNDL database. For more information, click here.


2010AV07      Phys.Rev. C 82, 037601 (2010)

M.Avrigeanu, A.M.Moro

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0644.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0474.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1809. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1750.


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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1648.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0440.


2007CR06      Phys.Rev. C 76, 054607 (2007)

R.Crespo, A.M.Moro

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
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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
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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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2007ES06      Nucl.Phys. A792, 2 (2007)

D.Escrig, A.M.Sanchez-Benitez, A.M.Moro, M.A.G.Alvarez, M.V.Andres, C.Angulo, M.J.G.Borge, J.Cabrera, S.Cherubini, P.Demaret, J.M.Espino, P.Figuera, M.Freer, J.E.Garcia-Ramos, J.Gomez-Camacho, M.Gulino, O.R.Kakuee, I.Martel, C.Metelko, F.Perez-Bernal, J.Rahighi, K.Rusek, D.Smirnov, O.Tengblad, V.Ziman

α-particle production in the scattering of 6He by 208Pb at energies around the Coulomb barrier

NUCLEAR REACTIONS 208Pb(6He, α), E=14, 16, 18, 22 MeV; measured Eα, Iα, σ(E, θ); deduced reaction mechanism features using DWBA analysis.

doi: 10.1016/j.nuclphysa.2007.05.012
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1654.


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