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NSR database version of April 11, 2024.

Search: Author = C.A.Bertulani

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2024BE05      Eur.Phys.J. A 60, 43 (2024)

C.A.Bertulani, D.Bhandari, F.S.Navarra

Unveiling the properties of the dimuonium at the energies available at the Large Hadron Collider at CERN

doi: 10.1140/epja/s10050-024-01250-5
Citations: PlumX Metrics


2023BE20      Phys.Lett. B 846, 138250 (2023)

C.A.Bertulani

Core destruction in knockout reactions

NUCLEAR REACTIONS 9B(7Li, 6He), (7Li, 6Li), 12C(8B, 7Be), (10C, 9C), (9C, 8B), (9Li, 8Li), (12C, 11B), (12C, 11C), (14O, 13N), (16O, 15N), (16O, 15O), 9Be(10Be, 9Li), (10Be, 9Be), (10C, 9C), E<300 MeV/nucleon; calculated one-nucleon-removal stripping σ, projectile core destruction in knockout reactions; deduced model. Comparison with the EXFOR library data.

doi: 10.1016/j.physletb.2023.138250
Citations: PlumX Metrics


2023BE22      Phys.Rev. C 108, 054602 (2023)

C.A.Bertulani

How to extract the electromagnetic response of 6He in relativistic collisions

doi: 10.1103/PhysRevC.108.054602
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2023CH56      Particles 6, 198 (2023)

E.V.Chimanski, R.V.Lobato, A.R.Goncalves, C.A.Bertulani

Bayesian Exploration of Phenomenological EoS of Neutron/Hybrid Stars with Recent Observations

doi: 10.3390/particles6010011
Citations: PlumX Metrics


2023FA11      Phys.Rev. C 108, 044901 (2023)

R.Fariello, D.Bhandari, C.A.Bertulani, F.S.Navarra

Two- and three-photon fusion into charmonium in ultraperipheral nuclear collisions

doi: 10.1103/PhysRevC.108.044901
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2023HO07      Astrophys.J. 950, 133 (2023)

S.Q.Hou, J.B.Liu, T.C.L.Trueman, J.G.Li, M.Pignatari, C.A.Bertulani, X.X.Xu

New 26P(p, γ)27S Thermonuclear Reaction Rate and Its Astrophysical Implications in the rp-process

NUCLEAR REACTIONS 26P(p, γ), E<400 keV; analyzed available data; deduced direct, resonant, and total reaction rates, discrepancies with JINA REACLIB library.

doi: 10r3847/1538-4357/accf9c
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2023TU05      Commun. Phys. 6, 106 (2023)

A.Tumino, G.G.Rapisarda, M.La Cognata, A.Oliva, A.Kievsky, C.A.Bertulani, G.D'Agata, M.Gattobigio, G.L.Guardo, L.Lamia, D.Lattuada, R.G.Pizzone, S.Romano, M.L.Sergi, R.Sparta, M.Viviani

Coulomb-free 1So p - p scattering length from the quasi-freep p + d → p + p + n reaction and its relation to universality

NUCLEAR REACTIONS 2H(p, 2p), E(cm)<1 MeV; analyzed available data; deduced p-p scattering σ, σ(θ), scattering length and effective range from a Bayesian approach analysis.

doi: 10.1038/s42005-023-01221-0
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2023WA24      Eur.Phys.J. A 59, 154 (2023)

F.Wamers, C.Lehr, J.Marganiec-Galazka, F.Aksouh, Yu.Aksyutina, H.Alvarez-Pol, L.Atar, T.Aumann, S.Beceiro Novo, C.A.Bertulani, K.Boretzky, M.J.G.Borge, C.Caesar, M.Chartier, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.O.U.Fynbo, D.Galaviz, H.Geissel, M.Heil, M.Holl, H.T.Johansson, B.Jonson, C.Karagiannis, O.A.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, C.Muntz, T.Nilsson, C.Nociforo, W.Ott, V.Panin, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, K.Riisager, C.Rodriguez-Tajes, D.Rossi, D.Savran, H.Scheit, G.Schrieder, P.Schrock, H.Simon, J.Stroth, K.Summerer, O.Tengblad, H.Weick, C.Wimmer

Diverse mechanisms in proton knockout reactions from the Borromean nucleus 17Ne

NUCLEAR REACTIONS 1H, 12C(17Ne, 2p), (17Ne, 16F), E=500 MeV/nucleon; analyzed available data. 17Ne, 16F; deduced σ(E), resonance parameters, spectroscopic factors. The SIS-18 synchrotron at GSI.

doi: 10.1140/epja/s10050-023-01063-y
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022DU08      Nature(London) 606, 678 (2022)

M.Duer, T.Aumann, R.Gernhauser, V.Panin, S.Paschalis, D.M.Rossi, N.L.Achouri, D.Ahn, H.Baba, C.A.Bertulani, M.Bohmer, K.Boretzky, C.Caesar, N.Chiga, A.Corsi, D.Cortina-Gil, C.A.Douma, F.Dufter, Z.Elekes, J.Feng, B.Fernandez-Dominguez, U.Forsberg, N.Fukuda, I.Gasparic, Z.Ge, J.M.Gheller, J.Gibelin, A.Gillibert, K.I.Hahn, Z.Halasz, M.N.Harakeh, A.Hirayama, M.Holl, N.Inabe, T.Isobe, J.Kahlbow, N.Kalantar-Nayestanaki, D.Kim, S.Kim, T.Kobayashi, Y.Kondo, D.Korper, P.Koseoglou, Y.Kubota, I.Kuti, P.J.Li, C.Lehr, S.Lindberg, Y.Liu, F.M.Marques, S.Masuoka, M.Matsumoto, J.Mayer, K.Miki, B.Monteagudo, T.Nakamura, T.Nilsson, A.Obertelli, N.A.Orr, H.Otsu, S.Y.Park, M.Parlog, P.M.Potlog, S.Reichert, A.Revel, A.T.Saito, M.Sasano, H.Scheit, F.Schindler, S.Shimoura, H.Simon, L.Stuhl, H.Suzuki, D.Symochko, H.Takeda, J.Tanaka, Y.Togano, T.Tomai, H.T.Tornqvist, J.Tscheuschner, T.Uesaka, V.Wagner, H.Yamada, B.Yang, L.Yang, Z.H.Yang, M.Yasuda, K.Yoneda, L.Zanetti, J.Zenihiro, M.V.Zhukov

Observation of a correlated free four-neutron system

NUCLEAR REACTIONS 1H(8He, pα)4NN, E=156 MeV/nucleon; measured reaction products, Ep, Ip, Eα, Iα. 4NN; deduced missing mass spectra, 4NN resonance, resonance parameters. Comparison with theoretical calculations. The Radioactive Ion Beam Factory operated by the RIKEN Nishina Center and the Center for Nuclear Study, University of Tokyo, using the Superconducting Analyzer for Multi-particles from Radio Isotope Beams (SAMURAI).

doi: 10.1038/s41586-022-04827-6
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022LE02      Phys.Lett. B 827, 136957 (2022)

C.Lehr, F.Wamers, F.Aksouh, Yu.Aksyutina, H.Alvarez-Pol, L.Atar, T.Aumann, S.Beceiro Novo, C.A.Bertulani, K.Boretzky, M.J.G.Borge, C.Caesar, M.Chartier, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.O.U.Fynbo, D.Galaviz, H.Geissel, M.Heil, M.Heine, D.H.H.Hoffmann, M.Holl, H.T.Johansson, B.Jonson, C.Karagiannis, O.A.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, B.Loher, K.Mahata, J.Marganiec-Galazka, C.Muntz, T.Nilsson, C.Nociforo, W.Ott, V.Panin, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, K.Riisager, C.Rodriguez-Tajes, D.Rossi, D.Savran, H.Scheit, G.Schrieder, P.Schrock, H.Simon, J.Stroth, K.Summerer, O.Tengblad, H.Weick, C.Wimmer

Unveiling the two-proton halo character of 17Ne: Exclusive measurement of quasi-free proton-knockout reactions

NUCLEAR REACTIONS 1H(17Ne, 2p), E=498 MeV/nucleon; measured reaction products. 17Ne; deduced σ(E), energy levels, two-proton halo. The GSI synchrotron SIS18.

doi: 10.1016/j.physletb.2022.136957
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022LI09      Phys.Rev. C 105, 024613 (2022)

J.Li, C.A.Bertulani, F.Xu

Nuclear spectroscopy with heavy ion nucleon knockout and (p, 2p) reactions

NUCLEAR REACTIONS 9Be(7Li, 6He), E=80 MeV; 9Be(7Li, 6Li), E=120 MeV; 12C(8B, 7Be), E=76, 142, 285, 936, 1440 MeV; 12C(9C, 8B), E=76 MeV; 9Be(9C, 8B), E=100 MeV; 9Be(9Li, 8Li), E=80 MeV; 12C(9Li, 8Li), E=100 MeV; 9Be(10Be, 9Li), E=80 MeV; 9Be(10Be, 9Be), E=80, 120 MeV; 9Be(10C, 9C), E=120 MeV; 12C(10C, 9C), E=120 MeV;12C(12C, 11B), E=250, 400, 1050, 2100 MeV; 12C(12C, 11C), E=250, 1050, 2100 MeV; 12C(14O, 13N), E=305 MeV; 9Be(14O, 13N), E=53 MeV; 9Be(14O, 13O), E=53 MeV; 12C(16O, 15N), (16O, 15O)E=2100 MeV; 12C(p, 2p), (p, pn), E=400 MeV; 1H(14O, 2p), E=351 MeV; 1H(16O, 2p), E=451 MeV; calculated σ, spectroscopic factors, reduction factors. Calculations based on ab initio many-body wave functions with the no-core shell model (NCSM). Comparison to experimental data.

doi: 10.1103/PhysRevC.105.024613
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2022LO16      J.Phys.:Conf.Ser. 2340, 012014 (2022)

R.V.Lobato, E.V.Chimanski, C.A.Bertulani

Cluster Structures with Machine Learning Support in Neutron Star M-R relations

doi: 10.1088/1742-6596/2340/1/012014
Citations: PlumX Metrics


2022ST07      Eur.Phys.J. A 58, 223 (2022)

A.I.Stefanescu, V.Panin, L.Trache, T.Motobayashi, H.Otsu, A.Saastamoinen, T.Uesaka, L.Stuhl, J.Tanaka, D.Tudor, I.C.Stefanescu, A.E.Spiridon, K.Yoneda, H.Baba, M.Kurokawa, Y.Togano, Z.Halasz, M.Sasano, S.Ota, Y.Kubota, D.S.Ahn, T.Kobayashi, Z.Elekes, N.Fukuda, H.Takeda, D.Kim, E.Takada, H.Suzuki, K.Yoshida, Y.Shimizu, H.N.Liu, Y.L.Sun, T.Isobe, J.Gibelin, P.J.Li, J.Zenihiro, F.M.Marques, M.N.Harakeh, G.G.Kiss, A.Kurihara, M.Yasuda, T.Nakamura, S.Park, Z.Yang, T.Harada, M.Nishimura, H.Sato, I.S.Hahn, K.Y.Chae, J.M.Elson, L.G.Sobotka, C.A.Bertulani

Silicon tracker array for RIB experiments at SAMURAI

doi: 10.1140/epja/s10050-022-00873-w
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2022TE05      Eur.Phys.J. A 58, 205 (2022)

E.A.Teixeira, T.Aumann, C.A.Bertulani, B.V.Carlson

Nuclear fragmentation reactions as a probe of neutron skins in nuclei

NUCLEAR REACTIONS 208Pb(p, X), E<500 MeV; 12C(12C, X), E<1000 MeV/nucleon; analyzed available data; deduced σ, neutron skin thickness as a function of the isospin asymmetry parameter.

doi: 10.1140/epja/s10050-022-00849-w
Citations: PlumX Metrics


2021AL17      Eur.Phys.J. A 57, 196 (2021)

N.Alamanos, C.Bertulani, V.Guimaraes

Topical issue on cluster structure and dynamics of nuclei: a tribute to Mahir Hussein

doi: 10.1140/epja/s10050-021-00511-x
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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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2021BE09      Eur.Phys.J. A 57, 67 (2021)

C.A.Bertulani, R.Lobato

Final state interaction in the pn and nn decay channels of 4ΛHe

doi: 10.1140/epja/s10050-021-00390-2
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2021BE33      Phys.Rev. C 104, L061602 (2021)

C.A.Bertulani, A.Idini, C.Barbieri

Examination of the sensitivity of quasifree reactions to details of the bound-state overlap functions

NUCLEAR REACTIONS 9Be(14O, X), (16O, X), (22O, X), (24O, X), E=350 MeV/nucleon; analyzed separation energies, root mean square radii of the overlap wave function, asymptotic normalization coefficients, (p, pN) quasifree cross sections, and nucleon knockout cross sections, tail of the overlap functions, probability of removing a proton from 24O, using potential models in the experimental analysis of knockout reactions, and ab initio computations from self-consistent Green's function theory.

doi: 10.1103/PhysRevC.104.L061602
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2021GO20      Phys.Rev. C 104, 024001 (2021)

M.Gobel, T.Aumann, C.A.Bertulani, T.Frederico, H.-W.Hammer, D.R.Phillips

Neutron-neutron scattering length from the 6He (p, pα) nn reaction

NUCLEAR REACTIONS 2H(π-, γ), (n, p), (d, 2He)2n, E not given; compiled experimental data for neutron-neutron scattering lengths reported between 1998 and 2008. 1H(6He, pα)2n, E=few MeV/nucleon; calculated ground-state nn relative-energy distributions for different nn scattering lengths using halo effective field theory (EFT), s-wave scattering length using a method based on the final-state interaction (FSI) between the neutrons after the sudden knockout of the α particle. Comparison with model calculations using the computer code FaCE. Proposed a novel method to measure the neutron-neutron scattering length in inverse kinematics. Relevance to precise determination of the nn scattering length using data from the approved experiment at RIKEN using the 1H(6He, pα)nn reaction.

doi: 10.1103/PhysRevC.104.024001
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2021PA16      Eur.Phys.J. A 57, 103 (2021)

V.Panin, T.Aumann, C.A.Bertulani

Quasi-free scattering in inverse kinematics as a tool to unveil the structure of nuclei

NUCLEAR REACTIONS 1H(12C, 2p), E=400 MeV/nucleon; analyzed available data; deduced angular correlations between two protons, σ(θ).

doi: 10.1140/epja/s10050-021-00416-9
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2021SP02      Eur.Phys.J. A 57, 20 (2021)

C.Spitaleri, S.Typel, C.A.Bertulani, A.M.Mukhamedzhanov, T.Kajino, M.Lattuada, A.Cvetinovic, S.Messina, G.L.Guardo, N.Soic, M.Milin, S.S.Perrotta, C.Li, P.Colovic, G.D'Agata, D.Dell'Aquila, C.G.Fatuzzo, M.Gulino, S.Q.Hou, M.La Cognata, D.Lattuada, D.Nurkic, R.Popocovski, N.Skukan, S.Szilner, O.Trippella, M.Uroic, N.Vukman

The 3He + 5He → α+α reaction below the Coulomb barrier via the Trojan Horse Method

NUCLEAR REACTIONS 9Be(3He, 2α), E=4 MeV; 3He(5He, α), E(cm)<1 Mev; measured reaction products, Eα, Iα; deduced two α-particles σ(θ, E), σ(θ). Comparison with theoretical calculations, Trojan Horse Method (THM).

doi: 10.1140/epja/s10050-020-00324-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD1037.


2020BA47      Phys.Rev. C 102, 034327 (2020)

S.Bassauer, P.von Neumann-Cosel, P.-G.Reinhard, A.Tamii, S.Adachi, C.A.Bertulani, P.Y.Chan, A.D'Alessio, H.Fujioka, H.Fujita, Y.Fujita, G.Gey, M.Hilcker, T.H.Hoang, A.Inoue, J.Isaak, C.Iwamoto, T.Klaus, N.Kobayashi, Y.Maeda, M.Matsuda, N.Nakatsuka, S.Noji, H.J.Ong, I.Ou, N.Pietralla, V.Yu.Ponomarev, M.S.Reen, A.Richter, M.Singer, G.Steinhilber, T.Sudo, Y.Togano, M.Tsumura, Y.Watanabe, V.Werner

Electric and magnetic dipole strength in 112, 114, 116, 118, 120, 124Sn

NUCLEAR REACTIONS 112,114,116,118,120,124Sn(p, p'), E=295 MeV; measured E(p), I(p), particle spectra through identification via the correlation of energy loss and time of flight (ToF), double differential σ(θ, E(exc)) using Grand Raiden spectrometer at RCNP accelerator facility; deduced photoabsorption cross sections due to E1 and M1 excitations from multipole decomposition analysis (MDA) after subtraction of the ISGMR and ISGQR contributions, σ, energy and width of isovector giant dipole resonance (IVGDR), B(E1) and B(M1) strengths in the excitation energy range of 6-20 MeV, dipole polarizability. Comparison with previous experimental results from (γ, xn) and (γ, γ') experiments.

doi: 10.1103/PhysRevC.102.034327
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020BA50      Phys.Lett. B 810, 135804 (2020)

S.Bassauer, P.von Neumann-Cosel, P.-G.Reinhard, A.Tamii, S.Adachi, C.A.Bertulani, P.Y.Chan, G.Colo, A.D'Alessio, H.Fujioka, H.Fujita, Y.Fujita, G.Gey, M.Hilcker, T.H.Hoang, A.Inoue, J.Isaak, C.Iwamoto, T.Klaus, N.Kobayashi, Y.Maeda, M.Matsuda, N.Nakatsuka, S.Noji, H.J.Ong, I.Ou, N.Paar, N.Pietralla, V.Yu.Ponomarev, M.S.Reen, A.Richter, X.Roca-Maza, M.Singer, G.Steinhilber, T.Sudo, Y.Togano, M.Tsumura, Y.Watanabe, V.Werner

Evolution of the dipole polarizability in the stable tin isotope chain

NUCLEAR REACTIONS 112,114,116,118,120,124Sn(p, p'), E=295 MeV; 116Sn(γ, X), E<30 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E), σ, total dipole polarizability. Comparison with available data.

doi: 10.1016/j.physletb.2020.135804
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2020BE05      Phys.Rev.Lett. 124, 132301 (2020)

Carl.A.Bertulani, Y.Kucuk, R.Lozeva

Fission of Relativistic Nuclei with Fragment Excitation and Reorientation

NUCLEAR REACTIONS 208Pb(238U, F), E=1 GeV/nucleon; analyzed available data; calculated fission and fragmentation σ in relativistic heavy ion collisions.

doi: 10.1103/PhysRevLett.124.132301
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2020DI05      Phys.Lett. B 811, 135962 (2020)

J.Diaz-Cortes, J.Benlliure, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, B.Blank, E.Casarejos, D.Cortina-Gil, D.Dragosavac, V.Fohr, A.Gargano, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, D.Perez-Loureiro, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Systematic reduction of the proton-removal cross section in neutron-rich medium-mass nuclei

NUCLEAR REACTIONS 9Be(238U, X)132Sn/131Sn/131In/128Sn/130Sn/136Sn, E=950 MeV/nucleon; 9Be(132Xe, X)119Sn/124Sn/126Sn, E=1200 MeV/nucleon; 9Be(119Sn, X), (124Sn, X), (126Sn, X), (130Sn, X), (131Sn, X), (132Sn, X), (128Sn, X), (136Sn, X), (131Sn, X), E ∼ 1000 MeV/nucleon; measured reaction products, TOF; deduced single neutron and single proton removal σ. Comparison with the advanced Liege intra-nuclear cascade (INCL) model calculations.

doi: 10.1016/j.physletb.2020.135962
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8031.


2020DO11      Phys.Rev. C 102, 064327 (2020)

L.M.Donaldson, J.Carter, P.von Neumann-Cosel, V.O.Nesterenko, R.Neveling, P.-G.Reinhard, I.T.Usman, P.Adsley, C.A.Bertulani, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, N.Y.Kheswa, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, V.Yu.Ponomarev, B.Rebeiro, A.Richter, N.Yu.Shirikova, E.Sideras-Haddad, A.V.Sushkov, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii

Fine structure of the isovector giant dipole resonance in 142-150Nd and 152Sm

NUCLEAR REACTIONS 142,144,146,148,150Nd, 152Sm(p, p'), E=200 MeV from the Separated Sector Cyclotron (SSC) at iThemba LABS; measured reaction products, E(p), I(p), time-of-flight using the K600 magnetic spectrometer, two multiwire drift chambers (MWDCs) and two plastic scintillators; deduced double-differential σ(E*=10-22 MeV), equivalent photoabsorption spectra, excitation-energy spectra, wavelet power spectra, fine structure of the isovector giant-dipole resonance (IVGDR), fragmentation of the one-particle-one-hole (1p1h) strength into several dominant transitions serving as doorway states in the spherical and intermediate spherical/deformed nuclei. Comparison with predictions of quasiparticle phonon model (QPM), and Skyrme separable random phase approximation (SSRPA).

doi: 10.1103/PhysRevC.102.064327
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0860.


2020LI51      Phys.Rev. C 102, 064601 (2020)

J.J.Li, C.A.Bertulani, Y.Liu, J.L.Lou, D.Y.Pang, X.H.Sun, B.Yang, X.F.Yang, Y.L.Ye

Eikonal method for charge-exchange reactions at intermediate energies

NUCLEAR REACTIONS 26Mg, 120Sn(3He, t), E=140 MeV/nucleon; 13C(13N, 13C), E=105 MeV/nucleon; calculated differential σ(θ) and relativistic kinematical quantities for intermediate and high energy heavy-ion charge exchange reactions using Eikonal method and the DWBA model, with effective nucleon-nucleon interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.064601
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2020OG02      J.Phys.(London) G47, 095101 (2020)

K.Ogata, C.A.Bertulani

Nuclear medium effect on neutron capture reactions during neutron star mergers

NUCLEAR REACTIONS 58,78Ni(n, γ), E<100 keV; calculated reaction rates employing the Koning and Deraloche global optical potential.

doi: 10.1088/1361-6471/ab9d06
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2020PI17      Eur.Phys.J. A 56, 283 (2020)

R.G.Pizzone, C.A.Bertulani, L.Lamia, M.La Cognata, M.L.Sergi, R.Sparta, A.Tumino

Clusters and their fundamental role for Trojan Horse Method

NUCLEAR REACTIONS 6Li(d, α), E(cm)<3 MeV; 7Li(p, α), E(cm)<7 MeV; 2H(d, p), E(cm)<0.9 MeV; analyzed available data; deduced S-factors, momentum distributions within the framework of the Plane Wave Impulse Approximation (PWIA). The Trojan Horse Method (THM).

doi: 10.1140/epja/s10050-020-00285-8
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2020SY01      Phys.Lett. B 809, 135748 (2020)

I.Syndikus, M.Petri, A.O.Macchiavelli, S.Paschalis, C.A.Bertulani, T.Aumann, H.Alvarez-Pol, L.Atar, S.Beceiro Novo, J.Benlliure, J.M.Boillos, K.Boretzky, M.J.G.Borge, B.A.Brown, M.Caamano, C.Caesar, E.Casarejos, W.Catford, J.Cederkall, S.Chakraborty, L.V.Chulkov, D.Cortina-Gil, E.Cravo, R.Crespo, U.Datta Pramanik, I.Dillmann, P.Diaz Fernandez, Z.Elekes, J.Enders, F.Farinon, L.M.Fraile, D.Galaviz, H.Geissel, R.Gernhauser, P.Golubev, K.Gobel, M.Heil, M.Heine, A.Heinz, A.Henriques, M.Holl, H.T.Johansson, B.Jonson, N.Kalantar-Nayestanaki, R.Kanungo, A.Kelic-Heil, T.Kroll, N.Kurz, C.Langer, T.Le Bleis, J.Machado, J.Marganiec-Galazka, E.Nacher, T.Nilsson, C.Nociforo, V.Panin, A.Perea, S.B.Pietri, R.Plag, A.Rahaman, R.Reifarth, A.Revel, G.Ribeiro, C.Rigollet, D.M.Rossi, D.Savran, H.Scheit, H.Simon, O.Sorlin, O.Tengblad, Y.Togano, M.Vandebrouck, V.Volkov, F.Wamers, C.Wheldon, G.L.Wilson, J.S.Winfield, H.Weick, P.Woods, D.Yakorev, M.Zhukov, A.Zilges, K.Zuber

Probing the Z=6 spin-orbit shell gap with (p, 2p) quasi-free scattering reactions

NUCLEAR REACTIONS C, H(17N, X)16C, E=438 MeV/nucleon; C, H(19N, X)18C, E=430 MeV/nucleon; C, H(21N, X)20C, E=422 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ, spectroscopic factors, proton component of spin-orbit splitting.

doi: 10.1016/j.physletb.2020.135748
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2019BE24      Phys.Rev. C 100, 015802 (2019)

C.A.Bertulani, J.Valencia

Neutron skins as laboratory constraints on properties of neutron stars and on what we can learn from heavy ion fragmentation reactions

NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148Sn, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220Pb; calculated neutron skin with the Skyrme interactions SIII, SKP, SKX, HFB9, SLY5, SKXS20, SKO and SKI5.

NUCLEAR REACTIONS 1H, 12C(48Ni, X), (50Ni, X), (52Ni, X), (54Ni, X), (56Ni, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X), (74Ni, X), (76Ni, X), (100Sn, X), (102Sn, X), (104Sn, X), (106Sn, X), (108Sn, X), (110Sn, X), (112Sn, X), (114Sn, X), (116Sn, X), (118Sn, X), (120Sn, X), (122Sn, X), (124Sn, X), (126Sn, X), (128Sn, X), (130Sn, X), (132Sn, X), (134Sn, X), (136Sn, X), (138Sn, X), (178Pb, X), (180Pb, X), (182Pb, X), (184Pb, X), (186Pb, X), (188Pb, X), (190Pb, X), (192Pb, X), (194Pb, X), (196Pb, X), (198Pb, X), (200Pb, X), (202Pb, X), (204Pb, X), (206Pb, X), (208Pb, X), (210Pb, X), (212Pb, X), (214Pb, X), (216Pb, X), (218Pb, X), (220Pb, X), E=1 GeV/nucleon; calculated cross sections for the Coulomb excitation of the isovector GDR, nuclear excitation of the isoscalar GQR and isovector GDR, neutron emission after excitation, and total interaction σ using microscopic model with several Skyrme interactions. Relevance to equation of state (EoS)of nuclear matter and neutron-rich matter to explain the structure of neutron stars.

doi: 10.1103/PhysRevC.100.015802
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2019BE39      Eur.Phys.J. A 55, 240 (2019)

C.A.Bertulani

Pygmy resonances and symmetry energy

doi: 10.1140/epja/i2019-12883-2
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2019BE40      Int.J.Mod.Phys. E28, 1950109(2019)

C.A.Bertulani, L.F.Canto, M.S.Hussein, Shubhchintak, T.V.Nhan Hao

The neutron within the deuteron as a surrogate for neutron-induced reactions

NUCLEAR REACTIONS 59Co, 58Ni, 63Cu, 103Rh, 135Xe, 149Sm, 157Gd, 159Tb, 232Th, 238U(d, p), E<300 MeV; analyzed available data; deduced (n, γ) σ.

doi: 10.1142/S021830131950109X
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2019HO08      Phys.Lett. B 795, 682 (2019)

M.Holl, V.Panin, H.Alvarez-Pol, L.Atar, T.Aumann, S.Beceiro Novo, J.Benlliure, C.A.Bertulani, J.M.Boillos, K.Boretzky, M.Caamano, C.Caesar, E.Casarejos, W.Catford, J.Cederkall, L.Chulkov, D.Cortina-Gil, E.Cravo, I.Dillmann, P.Diaz Fernandez, Z.Elekes, J.Enders, L.M.Fraile, D.Galaviz-Redondo, R.Gernhauser, P.Golubev, T.Heftrich, M.Heil, M.Heine, A.Heinz, A.Henriques, H.T.Johansson, B.Jonson, N.Kalantar-Nayestanaki, R.Kanungo, A.Kelic-Heil, T.Kroll, N.Kurz, C.Langer, T.Le Bleis, S.Lindberg, J.Machado, E.Nacher, M.A.Najafi, T.Nilsson, C.Nociforo, S.Paschalis, M.Petri, R.Reifarth, G.Ribeiro, C.Rigollet, D.M.Rossi, D.Savran, H.Scheit, H.Simon, O.Sorlin, I.Syndikus, O.Tengblad, Y.Togano, M.Vandebrouck, P.Velho, F.Wamers, H.Weick, C.Wheldon, G.L.Wilson, J.S.Winfield, P.Woods, M.Zhukov, K.Zuber

Quasi-free neutron and proton knockout reactions from light nuclei in a wide neutron-to-proton asymmetry range

NUCLEAR REACTIONS 1H(11C, 2p), (10C, np), (11C, np), (12C, np), E=300-400 MeV/nucleon; measured reaction products, Ep, Ip, En, In; deduced σ and momentum distributions. Comparison with DWIA calculations.

doi: 10.1016/j.physletb.2019.06.069
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2019LA13      Astrophys.J. 879, 23 (2019)

L.Lamia, M.Mazzocco, R.G.Pizzone, S.Hayakawa, M.La Cognata, C.Spitaleri, C.A.Bertulani, A.Boiano, C.Boiano, C.Broggini, A.Caciolli, S.Cherubini, G.D'Agata, H.da Silva, R.Depalo, F.Galtarossa, G.L.Guardo, M.Gulino, I.Indelicato, M.La Commara, G.La Rana, R.Menegazzo, J.Mrazek, A.Pakou, C.Parascandolo, D.Piatti, D.Pierroutsakou, S.M.R.Puglia, S.Romano, G.G.Rapisarda, A.M.Sanchez-Benitez, M.L.Sergi, O.Sgouros, F.Soramel, V.Soukeras, R.Sparta, E.Strano, D.Torresi, A.Tumino, H.Yamaguchi, G.L.Zhang

Cross-section Measurement of the Cosmologically Relevant 7Be(n, α)4He Reaction over a Broad Energy Range in a Single Experiment

NUCLEAR REACTIONS 2H(7Be, 2α), E<2 MeV; measured reaction products, Ep, Ip. 8Be; deduced σ, astrophysical reaction rates. Trojan Horse Method.

doi: 10.3847/1538-4357/ab2234
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2019LI10      Phys.Rev.Lett. 122, 072502 (2019)

H.N.Liu, A.Obertelli, P.Doornenbal, C.A.Bertulani, G.Hagen, J.D.Holt, G.R.Jansen, T.D.Morris, A.Schwenk, R.Stroberg, N.Achouri, H.Baba, F.Browne, D.Calvet, F.Chateau, S.Chen, N.Chiga, A.Corsi, M.L.Cortes, A.Delbart, J.-M.Gheller, A.Giganon, A.Gillibert, C.Hilaire, T.Isobe, T.Kobayashi, Y.Kubota, V.Lapoux, 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, D.Kim, T.Koiwai, Y.Kondo, P.Koseoglou, J.Lee, C.Lehr, B.D.Linh, 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.Wang, V.Werner, X.Xu, H.Yamada, D.Yan, Z.Yang, M.Yasuda, L.Zanetti

How Robust is the N=34 Subshell Closure? First Spectroscopy of 52Ar

NUCLEAR REACTIONS 1H(53K, 2p), E=245 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, σ. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.122.072502
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2019OG01      Phys.Rev. C 99, 065808 (2019)

R.Ogura, K.Hagino, C.A.Bertulani

Potential model for nuclear astrophysical fusion reactions with a square-well potential

NUCLEAR REACTIONS 16O(16O, X), E(cm)=6-13 MeV; calculated astrophysical S factor using potential model with various square-well and Woods-Saxon potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.065808
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2019PA25      Phys.Rev.Lett. 122, 162503 (2019)

N.Paul, A.Obertelli, C.A.Bertulani, A.Corsi, P.Doornenbal, J.L.Rodriguez-Sanchez, G.Authelet, H.Baba, D.Calvet, F.Chateau, S.Chen, A.Delbart, J.-M.Gheller, A.Giganon, A.Gillibert, T.Isobe, V.Lapoux, M.Matsushita, S.Momiyama, T.Motobayashi, M.Niikura, H.Otsu, C.Peron, A.Peyaud, E.C.Pollacco, J.-Y.Rousse, H.Sakurai, C.Santamaria, M.Sasano, Y.Shiga, D.Steppenbeck, S.Takeuchi, R.Taniuchi, T.Uesaka, H.Wang, K.Yoneda, T.Ando, T.Arici, A.Blazhev, F.Browne, A.M.Bruce, R.Carroll, L.X.Chung, M.L.Cortes, M.Dewald, B.Ding, Zs.Dombradi, F.Flavigny, S.Franchoo, F.Giacoppo, M.Gorska, A.Gottardo, K.Hadynska-Klek, Z.Korkulu, S.Koyama, Y.Kubota, A.Jungclaus, J.Lee, M.Lettmann, B.D.Linh, J.Liu, Z.Liu, C.Lizarazo, C.Louchart, R.Lozeva, K.Matsui, T.Miyazaki, K.Moschner, S.Nagamine, N.Nakatsuka, C.Nita, S.Nishimura, C.R.Nobs, L.Olivier, S.Ota, Z.Patel, Zs.Podolyak, M.Rudigier, E.Sahin, T.Y.Saito, C.Shand, P.-A.Soderstrom, I.G.Stefan, T.Sumikama, D.Suzuki, R.Orlandi, V.Vaquero, Zs.Vajta, V.Werner, K.Wimmer, J.Wu, Z.Xu

Prominence of Pairing in Inclusive (p, 2p) and (p, pn) Cross Sections from Neutron-Rich Nuclei

NUCLEAR REACTIONS 1H(96Kr, np)95Kr, E ∼ 250 MeV/nucleon; analyzed available data for fifty-five inclusive single nucleon-removal σ; deduced systematically higher cross sections are found for proton removal from nuclei with an even number of protons as compared to odd-proton number projectiles for a given neutron separation energy.

doi: 10.1103/PhysRevLett.122.162503
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2018DO01      Phys.Lett. B 776, 133 (2018)

L.M.Donaldson, C.A.Bertulani, J.Carter, V.O.Nesterenko, P.von Neumann-Cosel, R.Neveling, V.Yu.Ponomarev, P.-G.Reinhard, I.T.Usman, P.Adsley, J.W.Brummer, E.Z.Buthelezi, G.R.J.Cooper, R.W.Fearick, S.V.Fortsch, H.Fujita, Y.Fujita, M.Jingo, W.Kleinig, C.O.Kureba, J.Kvasil, M.Latif, K.C.W.Li, J.P.Mira, F.Nemulodi, P.Papka, L.Pellegri, N.Pietralla, A.Richter, E.Sideras-Haddad, F.D.Smit, G.F.Steyn, J.A.Swartz, A.Tamii

Deformation dependence of the isovector giant dipole resonance: The neodymium isotopic chain revisited

NUCLEAR REACTIONS 144,146,148,150Nd, 152Sm(p, p'), E=200 MeV; measured reaction products, Eγ, Iγ; deduced σ, σ(θ, E), σ(θ). Comparison with DWBA calculations.

doi: 10.1016/j.physletb.2017.11.025
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2018HA28      Astrophys.J. 862, 62 (2018)

M.Hartos, C.A.Bertulani, Shubhchintak, A.M.Mukhamedzhanov, and S.Hou

Impact of the 7Be(α, γ)11C Reaction on the Primordial Abundance of 7Li

NUCLEAR REACTIONS 7Be(α, γ), E(cm)<3 MeV; calculated σ, reaction rates, S-factor. Comparison with available data.

doi: 10.3847/1538-4357/aac9c1
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2018SH06      Phys.Lett. B 778, 30 (2018)

Shubhchintak, C.A.Bertulani, T.Aumann

Maris polarization in neutron-rich nuclei

doi: 10.1016/j.physletb.2017.12.067
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2018WA07      Phys.Rev. C 97, 034612 (2018)

F.Wamers, J.Marganiec, F.Aksouh, Yu.Aksyutina, H.Alvarez-Pol, T.Aumann, S.Beceiro Novo, C.A.Bertulani, K.Boretzky, M.J.G.Borge, M.Chartier, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, H.Emling, O.Ershova, L.M.Fraile, H.O.U.Fynbo, D.Galaviz, H.Geissel, M.Heil, D.H.H.Hoffmann, J.Hoffman, H.T.Johansson, B.Jonson, C.Karagiannis, O.A.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, T.Le Bleis, C.Lehr, R.Lemmon, Yu.A.Litvinov, K.Mahata, C.Muntz, T.Nilsson, C.Nociforo, W.Ott, V.Panin, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, K.Riisager, C.Rodriguez-Tajes, D.Rossi, D.Savran, G.Schrieder, H.Simon, J.Stroth, K.Summerer, O.Tengblad, S.Typel, H.Weick, M.Wiescher, C.Wimmer

Comparison of electromagnetic and nuclear dissociation of 17Ne

NUCLEAR REACTIONS H, C, Pb(17Ne, p15O), (17Ne, p14O), (17Ne, 2p15O), (17Ne, 2p14O), E=500 MeV/nucleon; measured reaction products, mass spectra of 13O, 14O and 15O isotopes, (14O)p-, (14O)2p-, (15O)p-, (15O)2p-coin using lead, carbon, and polyethylene targets and ALADIN-R3B setup at GSI; deduced transverse momentum distributions of 14O and 15O, relative energy spectra, inclusive σ, σ(1p) and σ(2p) for fragmentation of 17Ne in 14O and 15o for different targets, electromagnetic dissociation (EMD) cross sections. Electromagnetic and nuclear dissociations. One-proton knockout, and three body 15O+2p correlations. Comparison of measured cross sections and energy spectra with calculations using three-body 15O+2p model, and Hartree-Bogoliubov theory. Relevance to 15O(2p, γ)17Ne capture reaction in astrophysical rp-process.

doi: 10.1103/PhysRevC.97.034612
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2018XU11      Phys.Rev. C 98, 044622 (2018)

Y.P.Xu, D.Y.Pang, X.Y.Yun, S.Kubono, C.A.Bertulani, C.X.Yuan

Possible determination of high-lying single-particle components with (d, p) reactions

NUCLEAR REACTIONS 12C, 24Mg, 28Si, 40Ca(d, p), E=51.93 MeV; analyzed experimental σ(θ) distributions, spectroscopic amplitudes for neutrons in normal and high-lying single-particle components in the ground and excited states by fitting the angular distributions of the ground and the j-forbidden excited states simultaneously, effects of one-step transfer (OST), two-step transfer (TST) and inelastic excitation processes in neutron pickup reactions. Coupled reaction channel calculations.

doi: 10.1103/PhysRevC.98.044622
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2017AU07      Phys.Rev.Lett. 119, 262501 (2017)

T.Aumann, C.A.Bertulani, F.Schindler, S.Typel

Peeling Off Neutron Skins from Neutron-Rich Nuclei: Constraints on the Symmetry Energy from Neutron-Removal Cross Sections

NUCLEAR REACTIONS 12C, 124,132Sn(p, p), (n, p), E<1000 MeV; analyzed available data; deduced dependence of neutron-removal σ on neutron skin.

doi: 10.1103/PhysRevLett.119.262501
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2017BI09      Phys.Rev.Lett. 118, 252501 (2017)

J.Birkhan, M.Miorelli, S.Bacca, S.Bassauer, C.A.Bertulani, G.Hagen, H.Matsubara, P.von Neumann-Cosel, T.Papenbrock, N.Pietralla, V.Yu.Ponomarev, A.Richter, A.Schwenk, A.Tamii

Electric Dipole Polarizability of 48Ca and Implications for the Neutron Skin

NUCLEAR REACTIONS 48Ca(p, p'), E=295 MeV; 48Ca(γ, X), E<25 MeV; measured reaction products; deduced σ, electric dipole polarizability, B(E1).

doi: 10.1103/PhysRevLett.118.252501
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2017CH45      Phys.Lett. B 774, 559 (2017)

L.X.Chung, C.A.Bertulani, P.Egelhof, S.Ilieva, D.T.Khoa, O.A.Kiselev

The dominance of the ν(0d5/2)2 configuration in the N = 8 shell in 12Be from the breakup reaction on a proton target at intermediate energy

NUCLEAR REACTIONS 1H(12Be, X)11Be, E=700.5 MeV/nucleon; measured reaction products; deduced σ(p). Distorted wave impulse approximation (DWIA) analysis.

doi: 10.1016/j.physletb.2017.09.068
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2017HO27      Phys.Rev. C 96, 064603 (2017)

J.Hong, C.A.Bertulani, A.T.Kruppa

Neutron removal from the deformed halo nucleus 31Ne

NUCLEAR REACTIONS 12C(31Ne, 30Ne), E=230 MeV/nucleon; calculated neutron knockout cross sections and longitudinal momentum distributions as function of deformation using a model to include deformed wave functions and a dynamical knockout formalism that includes the dependence on the nuclear orientation to study the neutron removal. Comparison with experimental data. 31Ne; deduced 3/2- for the deformed halo nucleus.

doi: 10.1103/PhysRevC.96.064603
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2017KU19      Phys.Rev. C 96, 034605 (2017)

R.Kumar, C.A.Bertulani, G.Robinson

Relativistic effects in heavy-ion Coulomb scattering

NUCLEAR REACTIONS 208Pb(208Pb, 208Pb), E=100 MeV/nucleon; investigated relativistic effects such as retardation, relativistic mass change, and inclusion of magnetic interactions in elastic Coulomb scattering of nuclei; analyzed differences of theoretical σ and deflection angles between the two methods: one involving an exact account of interaction retardation, and the second based on the expansion of effective Lagrangians in powers of the ion velocities; deduced that analytical formulas described all aspects of relativistic effects in heavy-ion Coulomb scattering without the need to solve numerically the coupled equations.

doi: 10.1103/PhysRevC.96.034605
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2017LA19      Astrophys.J. 850, 175 (2017)

L.Lamia, C.Spitaleri, C.A.Bertulani, S.Q.Hou, M.La Cognata, R.G.Pizzone, S.Romano, M.L.Sergi, A.Tumino

On the Determination of the 7Be(n, α)4He Reaction Cross Section at BBN Energies

NUCLEAR REACTIONS 7Be(n, α), E(cm)<8 MeV; analyzed available data; deduced σ using Trojan Horse method.

doi: 10.3847/1538-4357/aa965c
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2017MA67      Phys.Rev.Lett. 119, 182503 (2017)

D.Martin, P.von Neumann-Cosel, A.Tamii, N.Aoi, S.Bassauer, C.A.Bertulani, J.Carter, L.Donaldson, H.Fujita, Y.Fujita, T.Hashimoto, K.Hatanaka, T.Ito, A.Krugmann, B.Liu, Y.Maeda, K.Miki, R.Neveling, N.Pietralla, I.Poltoratska, V.Yu.Ponomarev, A.Richter, T.Shima, T.Yamamoto, M.Zweidinger

Test of the Brink-Axel Hypothesis for the Pygmy Dipole Resonance

NUCLEAR REACTIONS 96Mo(polarized p, p'), E=295 MeV; measured reaction products, Ep, Ip; deduced σ(θ), σ(θ, E), gamma strength functions.

doi: 10.1103/PhysRevLett.119.182503
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2017MU06      Phys.Rev. C 95, 024616 (2017)

A.M.Mukhamedzhanov, Shubhchintak, C.A.Bertulani, T.V.Nhan Hao

Internal and external radiative widths in the combined R-matrix and potential-model formalism

NUCLEAR REACTIONS 11,12C, 12,14,15N, 16O(p, γ), E not given; calculated radiative widths of E1 transitions and asymptotic normalization coefficients (ANC) for the following proton resonances: 2.365 MeV, 1/2+ in 13N, 2.69 MeV, 1/2+ in 13O, 3.104 MeV, 1/2- and 3.857 MeV, 5/2- in 17F, 1.191 MeV, 2- in 12N, 12.44 MeV, 1- and 13.090 MeV, 1- in 16O, and 6.79 MeV, 3/2+ in 15O using R-matrix formalism and potential model. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.024616
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2017MU14      Phys.Rev. C 96, 024623 (2017)

A.M.Mukhamedzhanov, Shubhchintak, C.A.Bertulani

Subthreshold resonances and resonances in the R-matrix method for binary reactions and in the Trojan horse method

NUCLEAR REACTIONS 13C(α, n)16O, E(cm)<1.1 MeV; calculated astrophysical S factor as a function of the α-13C relative kinetic energy using the R-matrix approach for resonances and Trojan horse method (THM) for S factor. Comparison with experimental data. Relevance to neutron generation in low-mass AGB stars.

doi: 10.1103/PhysRevC.96.024623
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2017RO22      Phys.Rev. C 96, 034303 (2017)

J.L.Rodriguez-Sanchez, J.Benlliure, C.A.Bertulani, J.Vargas, Y.Ayyad, H.Alvarez-Pol, J.Atkinson, T.Aumann, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, J.Diaz-Cortes, P.Diaz Fernandez, A.Estrade, H.Geissel, A.Kelic-Heil, Yu.A.Litvinov, M.Mostazo, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, H.Weick, J.S.Winfield

Knockout and fragmentation reactions using a broad range of tin isotopes

NUCLEAR REACTIONS C(112Sn, X)103Rh/104Rh/105Rh/106Rh/107Rh/105Pd/106Pd/107Pd/108Pd/107Ag/108Ag/109Ag/110Ag/109Cd/110Cd/111Cd, E=1 GeV/nucleon; measured production cross sections of the most neutron-rich residues in the fragmentation of 112Sn beam at GSI. C(124Sn, 123Sn), (124Sn, 123In), (120Sn, 119Sn), (120Sn, 119In), (120Sn, 118Cd), (112Sn, 111Sn), (112Sn, 111In), (110Sn, 109Sn), (110Sn, 109In), (110Sn, 108Cd), E=1 GeV/nucleon; measured One- and two-nucleon-removal cross sections. Comparison with previous experimental data and with Glauber model calculations.

doi: 10.1103/PhysRevC.96.034303
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2016BE16      Prog.Part.Nucl.Phys. 89, 56 (2016)

C.A.Bertulani, T.Kajino

Frontiers in nuclear astrophysics

doi: 10.1016/j.ppnp.2016.04.001
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2016BE42      Nature(London) 532, 448 (2016)

C.A.Bertulani, V.Zelevinsky

Four neutrons together momentarily

NUCLEAR STRUCTURE 4NN; analyzed available data; deduced evidence for the fleeting existence of this state, implications for neutron stars.

doi: 10.1038/nature17884
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2016MA42      Phys.Lett. B 759, 200 (2016)

J.Marganiec, F.Wamers, F.Aksouh, Yu.Aksyutina, H.Alvarez-Pol, T.Aumann, S.Beceiro Novo, C.A.Bertulani, K.Boretzky, M.J.G.Borge, M.Chartier, A.Chatillon, L.V.Chulkov, D.Cortina-Gil, H.Emling, O.Ershova, L.M.Fraile, H.O.U.Fynbo, D.Galaviz, H.Geissel, M.Heil, D.H.H.Hoffmann, J.Hoffmann, H.T.Johansson, B.Jonson, C.Karagiannis, O.A.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, C.Muntz, T.Nilsson, C.Nociforo, G.Nyman, W.Ott, V.Panin, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, C.Rodriguez-Tajes, D.Rossi, K.Riisager, D.Savran, G.Schrieder, H.Simon, J.Stroth, K.Summerer, O.Tengblad, S.Typel, H.Weick, M.Wiescher, C.Wimmer

Coulomb and nuclear excitations of narrow resonances in 17Ne

NUCLEAR REACTIONS H, C, Pb(17Ne, 2p), E=500 MeV/nucleon; measured reaction products, Ep, Ip. 17Ne; deduced σ(E), excitation energies and σ for resolved resonances in 17Ne, B(E2). Comparison with available data.

doi: 10.1016/j.physletb.2016.05.073
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2016MU04      Phys.Rev. C 93, 045805 (2016)

A.M.Mukhamedzhanov, Shubhchintak, C.A.Bertulani

Primordial α + d → 6Li + γ reaction and second lithium puzzle

NUCLEAR REACTIONS 2H(α, γ)6Li, E=0.05-2 MeV; calculated angular distribution of photons at Big Bang energies of 70, 100, 200, and 400 keV using potential model, total cross sections for E1 and E2 transitions, astrophysical S24(E) factors, 6Li/7Li ratio. Comparison with LUNA collaboration data, and other theoretical calculations.

doi: 10.1103/PhysRevC.93.045805
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2016PA02      Phys.Lett. B 753, 204 (2016)

V.Panin, J.T.Taylor, S.Paschalis, F.Wamers, Y.Aksyutina, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, K.Boretzky, C.Caesar, M.Chartier, L.V.Chulkov, D.Cortina-Gil, J.Enders, O.Ershova, H.Geissel, R.Gernhauser, M.Heil, H.T.Johansson, B.Jonson, A.Kelic-Heil, C.Langer, T.Le Bleis, R.Lemmon, T.Nilsson, M.Petri, R.Plag, R.Reifarth, D.Rossi, H.Scheit, H.Simon, H.Weick, C.Wimmer

Exclusive measurements of quasi-free proton scattering reactions in inverse and complete kinematics

NUCLEAR REACTIONS C, 1H(12C, 2p)10B/11B, E=400 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), σ(E), σ and corresponding spectroscopic factors. Comparison with theoretical calculations employing the eikonal formalism.

doi: 10.1016/j.physletb.2015.11.082
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2016PI01      Eur.Phys.J. A 52, 24 (2016)

R.G.Pizzone, B.T.Roeder, M.McCleskey, L.Trache, R.E.Tribble, C.Spitaleri, C.A.Bertulani, S.Cherubini, M.Gulino, I.Indelicato, M.La Cognata, L.Lamia, G.G.Rapisarda, R.Sparta

Trojan Horse measurement of the 18F(p, α)15O astrophysical S(E)-factor

NUCLEAR REACTIONS 2H(18F, nα), E=52 MeV; measured α-particles using TESCA, 15O using X1-PSD detectors; deduced deuteron breakup momentum distribution. 18F(p, α), E not given; deduced reaction rate vs nuclear temperature, σ(θ), S-factor for individual levels vs E(cm) using Trojan Horse method.

doi: 10.1140/epja/i2016-16024-3
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2016SU11      Phys.Rev. C 93, 044607 (2016)

Y.L.Sun, J.Lee, Y.L.Ye, A.Obertelli, Z.H.Li, N.Aoi, H.J.Ong, Y.Ayyad, C.A.Bertulani, J.Chen, A.Corsi, F.Cappuzzello, M.Cavallaro, T.Furono, Y.C.Ge, T.Hashimoto, E.Ideguchi, T.Kawabata, J.L.Lou, Q.T.Li, G.Lorusso, F.Lu, H.N.Liu, S.Nishimura, H.Suzuki, J.Tanaka, M.Tanaka, D.T.Tran, M.B.Tsang, J.Wu, Z.Y.Xu, T.Yamamoto

Experimental study of the knockout reaction mechanism using 14O at 60 MeV/nucleon

NUCLEAR REACTIONS 12C(14O, 13O), (14O, 11O), E=60 MeV/nucleon, [secondary 14O beam from 9Be(16O, X), E=80 MeV/nucleon primary reaction]; measured particle spectra using a hodoscope of scintillation detectors at RCNP-Osaka, two-body and three-body events from decay of excited states of 13O to p+12N and p+p+11C, the latter from sequential decay via the excited states of 12N, p(11C)- and 2p(11C)-coin; deduced one-neutron removal σ and 2pn-removal reactions, and compared with theoretical calculations by intra-nuclear cascade (INC) and eikonal models for knockout reactions. 12C(14O, X)10C/11C/12C/13C/12N/13N/14N, E=60 MeV/nucleon; measured yields.

doi: 10.1103/PhysRevC.93.044607
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2015AN16      Phys.Rev. C 92, 064903 (2015)

E.Andrade II, I.Gonzalez, A.Deppman, C.A.Bertulani

Evidence of subnucleonic degrees of freedom in J/ψ photoproduction in ultraperipheral collisions at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.92.064903
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2015CH28      Phys.Rev. C 91, 047303 (2015)

W.J.Chen, C.A.Bertulani, F.R.Xu, Y.N.Zhang

Odd-even mass staggering with Skyrme-Hartree-Fock-Bogoliubov theory

NUCLEAR STRUCTURE A=100-135, Z=50; A=178-214, Z=82; calculated odd-even mass differences; analyzed isoscalar and isovector pairing interactions; deduced pairing strengths from Skyrme-Hartree-Fock-Bogoliubov model with SLy4, SkP, SkM*, SkO, and SV-min forces. Comparison with experimental values.

doi: 10.1103/PhysRevC.91.047303
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2015HA21      Phys.Rev. C 92, 031305 (2015)

T.Hashimoto, A.M.Krumbholz, P.-G.Reinhard, A.Tamii, P.von Neumann-Cosel, T.Adachi, N.Aoi, C.A.Bertulani, H.Fujita, Y.Fujita, E.Ganioglu, K.Hatanaka, E.Ideguchi, C.Iwamoto, T.Kawabata, N.T.Khai, A.Krugmann, D.Martin, H.Matsubara, K.Miki, R.Neveling, H.Okamura, H.J.Ong, I.Poltoratska, V.Yu.Ponomarev, A.Richter, H.Sakaguchi, Y.Shimbara, Y.Shimizu, J.Simonis, F.D.Smit, G.Susoy, T.Suzuki, J.H.Thies, M.Yosoi, J.Zenihiro

Dipole polarizability of 120Sn and nuclear energy density functionals

NUCLEAR REACTIONS 120Sn(polarized p, p'), E=295 MeV; measured scattered proton spectra, p(θ) using Grand Raiden spectrometer at RCNP-Osaka; analyzed polarization transfer observables; deduced ISGQR excitation, B(E1), precise electric dipole polarizability αD, nuclear symmetry energy and its density dependence. Comparison with other experimental data. Comparison with model calculations based on Skyrme interactions and on relativistic Hamiltonians.

doi: 10.1103/PhysRevC.92.031305
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2015KR05      Phys.Lett. B 744, 7 (2015)

A.M.Krumbholz, P.von Neumann-Cosel, T.Hashimoto, A.Tamii, T.Adachi, C.A.Bertulani, H.Fujita, Y.Fujita, E.Ganioglu, K.Hatanaka, C.Iwamoto, T.Kawabata, N.T.Khai, A.Krugmann, D.Martin, H.Matsubara, R.Neveling, H.Okamura, H.J.Ong, I.Poltoratska, V.Yu.Ponomarev, A.Richter, H.Sakaguchi, Y.Shimbara, Y.Shimizu, J.Simonis, F.D.Smit, G.Susoy, J.H.Thies, T.Suzuki, M.Yosoi, J.Zenihiro

Low-energy electric dipole response in 120Sn

NUCLEAR REACTIONS 120Sn(p, p'), E=295 MeV; measured reaction products, Ep, Ip; deduced σ, σ(θ, E), B(E1). Comparison with available data.

doi: 10.1016/j.physletb.2015.03.023
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2015ST01      Phys.Rev.Lett. 114, 012701 (2015)

I.Stetcu, C.A.Bertulani, A.Bulgac, P.Magierski, K.J.Roche

Relativistic Coulomb Excitation within the Time Dependent Superfluid Local Density Approximation

NUCLEAR REACTIONS 238U(238U, 238U'), E not given; calculated the total energy spectrum of emitted electromagnetic radiation, damping resonance width. Goldhaber-Teller model.

doi: 10.1103/PhysRevLett.114.012701
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2015TO15      Eur.Phys.J. A 51, 132 (2015)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala, C.A.Bertulani

First-order neutron-deuteron scattering in a three-dimensional approach

NUCLEAR REACTIONS 2H(n, 2n), E=25, 190 MeV; calculated energy correlation between the first and the second neutron (coming from deuteron breakup), σ(θ) vs "kinematic S parameter", analyzing power using co-called "3D" formalism.

doi: 10.1140/epja/s2015-15132-x
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2014MA26      Acta Phys.Pol. B45, 229 (2014)

J.Marganiec, F.Wamers, F.Aksouh, Y.Aksyutina, H.Alvarez-Pol, T.Aumann, S.Beceiro, C.Bertulani, K.Boretzky, M.J.G.Borge, M.Chartier, A.Chatillon, L.Chulkov, D.Cortina-Gil, I.Egorova, H.Emling, O.Ershova, C.Forssen, L.M.Fraile, H.Fynbo, D.Galaviz, H.Geissel, L.Grigorenko, M.Heil, D.H.H.Hoffmann, J.Hoffmann, H.Johansson, B.Jonson, M.Karakoc, C.Karagiannis, O.Kiselev, J.V.Kratz, R.Kulessa, N.Kurz, C.Langer, M.Lantz, K.Larsson, T.Le Bleis, R.Lemmon, Yu.A.Litvinov, K.Mahata, C.Muntz, T.Nilsson, C.Nociforo, G.Nyman, W.Ott, V.Panin, Yu.Parfenova, S.Paschalis, A.Perea, R.Plag, R.Reifarth, A.Richter, K.Riisager, C.Rodriguez-Tajes, D.Rossi, G.Schrieder, N.Shulgina, H.Simon, J.Stroth, K.Summerer, J.Taylor, O.Tengblad, E.Tengborn, H.Weick, M.Wiescher, C.Wimmer, M.Zhukov

Study of the 15O(2p, γ)17Ne Cross Section by Coulomb Dissociation of 17Ne for the rp Process of Nucleosynthesis

NUCLEAR REACTIONS Pb(17Ne, 2p)15O, E=500 MeV/nucleon; measured reaction products, Eγ, Iγ, Ep, Ip; deduced σ, σ(E), resonances. Comparison with theoretical calculations, R3BROOT package.

doi: 10.5506/APhysPolB.45.229
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2014MU10      Phys.Rev. C 90, 034604 (2014)

A.M.Mukhamedzhanov, D.Y.Pang, C.A.Bertulani, A.S.Kadyrov

Surface-integral formalism of deuteron stripping

NUCLEAR REACTIONS 14C(d, p), E=23.4 MeV; 16O(d, p), E=36 MeV; calculated differential σ(θ), spectroscopic factors, neutron widths for deuteron stripping reactions to bound and resonant states. Distorted-wave Born approximation (DWBA), continuum-discretized coupled channels (CDCC), and surface-integral formalism.

doi: 10.1103/PhysRevC.90.034604
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2014PI08      Few-Body Systems 55, 1001 (2014)

R.G.Pizzone, C.Spitaleri, M.L.Sergi, L.Lamia, A.Tumino, C.A.Bertulani, L.Blokhintsev, V.Burjan, V.Kroha, M.La Cognata, J.Mrazek, A.M.Mukhamedzhanov, R.Sparta

Trojan Horse Particle Invariance: An Extensive Study

doi: 10.1007/s00601-014-0829-z
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2014TS04      Phys.Lett. B 739, 19 (2014)

K.Tshoo, Y.Satou, C.A.Bertulani, H.Bhang, S.Choi, T.Nakamura, Y.Kondo, S.Deguchi, Y.Kawada, Y.Nakayama, K.N.Tanaka, N.Tanaka, Y.Togano, N.Kobayashi, N.Aoi, M.Ishihara, T.Motobayashi, H.Otsu, H.Sakurai, S.Takeuchi, K.Yoneda, F.Delaunay, J.Gibelin, F.M.Marques, N.A.Orr, T.Honda, T.Kobayashi, T.Sumikama, Y.Miyashita, K.Yoshinaga, M.Matsushita, S.Shimoura, D.Sohler, J.W.Hwang, T.Zheng, Z.H.Li, Z.X.Cao

Neutron occupancy of the 0d5/2 orbital and the N=16 shell closure in 24O

NUCLEAR REACTIONS 1H(24O, n), E=62 MeV/nucleon; measured reaction products, En, In. 23O; deduced σ(E), energy levels, J, π, spectroscopic factors. Comparison with experimental data, USDB shell-model calculations.

doi: 10.1016/j.physletb.2014.10.033
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2013AU03      Phys.Rev. C 88, 064610 (2013)

T.Aumann, C.A.Bertulani, J.Ryckebusch

Quasifree (p, 2p) and (p, pn) reactions with unstable nuclei

NUCLEAR REACTIONS 1H(12C, 2p), (12C, np), (12C, p), E=0.3-4 GeV/nucleon; calculated total and elastic σ(E), proton and neutron knockout probabilities, longitudinal, transverse, and total momentum distributions. 1H(23O, np), (68Ni, n), (68Ni, np), (11Be, 10Be), (11Be, np), (8Be, 2p), 12C(68Ni, n), (11Be, 10Be), (8B, 7Be), E=500 MeV/nucleon; calculated σ for neutron removal as function of S(n), distance to the c.m. of 68Ni, and mass number, neutron skin of even-even Ni isotopes, longitudinal and transverse momentum distributions for 11Be and 68Ni. 1H(20O, np), (20O, 2p), E=500 MeV/nucleon; calculated full width at half-maximum (FWHM) of transverse momentum distributions as function of S(p) and S(n). Comparison with experimental data. Eikonal theory to describe total cross sections and momentum distributions of the recoiled residual nucleus in quasifree reactions.

doi: 10.1103/PhysRevC.88.064610
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2013AV06      Phys.Rev. C 88, 044319 (2013)

P.Avogadro, C.A.Bertulani

Role of pairing in the description of giant monopole resonances

NUCLEAR STRUCTURE 90,92,94Zr, 92,96Mo, 106,108,110,112,114,116Cd, 112,114,116,118,120,122,124,174Sn, 144Sm, 204,206,208Pb; calculated centroids of isoscalar giant monopole resonances (ISGMR), pairing strengths. Fully self-consistent quasi-particle random phase approximation on top of Hartree Fock Bogoliubov, including density dependence of pairing interactions (HFB+QRPA+DDDI). Skyrme functionals (SLy5, SkM* and Skxs20). Comparison with experimental data.

doi: 10.1103/PhysRevC.88.044319
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2013BE08      Acta Phys.Pol. B44, 531 (2013)

C.A.Bertulani

Nucleosynthesis: What Direct Reactions Can Do for It?

doi: 10.5506/APhysPolB.44.531
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2013CH22      Phys.Rev. C 87, 054616 (2013)

B.Chen, F.Sammarruca, C.A.Bertulani

Microscopic in-medium nucleon-nucleon cross sections with improved Pauli blocking effects

doi: 10.1103/PhysRevC.87.054616
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2013IZ01      Phys.Rev. C 88, 065808 (2013)

R.Izsak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.A.Bertulani, Zs.Fulop, T.Baumann, D.Bazin, K.Ieki, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, A.Gade, D.Galaviz, C.R.Hoffman, W.A.Peters, H.Schelin, M.Thoennessen, G.I.Veres

Determining the 7Li(n, γ) cross section via Coulomb dissociation of 8Li

NUCLEAR REACTIONS C, Pb(8Li, n), [8Li secondary beam from 9Be(18O, X), E=120 MeV/nucleon primary reaction], E=69.5 MeV/nucleon; 8Li(γ, n)7Li, [γ from 8Li beam impinging on C and Pb targets], E(8Li)=69.5 MeV/nucleon; measured TOF, position and angle of 8Li particles, neutron spectra from Coulomb dissociation of 8Li, E(n), I(n) using MONA neutron detector array at NSCL-MSU cyclotron facility; reconstructed neutron 7Li energy spectra and momentum vectors; deduced σ(E) for 7Li(n, γ)8Li reaction. Surrogate method. Comparison of σ with previous experimental results, and with low-energy effective field theory calculations.

doi: 10.1103/PhysRevC.88.065808
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2013KA09      Phys.Rev. C 87, 024607 (2013)

M.Karakoc, A.Banu, C.A.Bertulani, L.Trache

Coulomb distortion and medium corrections in nucleon-removal reactions

NUCLEAR REACTIONS 12C, 9Be, 7Li, 4He, 1H(17C, 16B), 12C(23Al, 22Mg), E=35 MeV/nucleon; 12C(23Al, 22Mg), E=50 MeV/nucleon; 12C(17C, 16B), E=100, 200, 400, 800, 1000 MeV/nucleon; 9Be(15O, 14N), E=56 MeV/nucleon; 9Be(11Be, 10Be), E=60 MeV/nucleon; 12C(24O, 23O), E=920 MeV/nucleon; 12C(33Mg, 32Mg), E=898 MeV/nucleon; calculated nucleon removal cross sections, Coulomb scattering effects, shapes and magnitude of longitudinal and transverse momentum distributions with Coulomb corrections, and with medium modifications of nucleon-nucleon interactions. State-of-the-art eikonal method. Comparison with experimental data, including previous experimental data for 12C(p, X), E=20-100 MeV.

doi: 10.1103/PhysRevC.87.024607
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2013PI03      Phys.Rev. C 87, 025805 (2013)

R.G.Pizzone, C.Spitaleri, C.A.Bertulani, A.M.Mukhamedzhanov, L.Blokhintsev, M.La Cognata, L.Lamia, A.Rinollo, R.Sparta, A.Tumino

Updated evidence of the Trojan horse particle invariance for the 2H(d, p)3H reaction

NUCLEAR REACTIONS 2H(6Li, pt)α, E=14 MeV; measured proton and triton spectra by energy-loss method, momentum distribution, σ(θ) at INFN-LNS facility in Catania; deduced momentum distribution width, quasifree (QF) contribution, astrophysical S(E) factor for 2H(d, p) reaction via Trojan-horse method (THM) after 6Li breakup. 2H(3He, pt), E(cm)<0.9 MeV; analyzed averaged astrophysical S(E) factor for 2H(d, p) reaction measured via THM after 3He breakup. PWIA analysis. Comparison with previous experimental studies.

doi: 10.1103/PhysRevC.87.025805
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2012AD07      Phys.Rev. C 85, 044904 (2012), Pub.Note Phys.Rev. C 85, 049904 (2012)

A.Adeluyi, C.A.Bertulani

Constraining gluon shadowing using photoproduction in ultraperipheral pA and AA collisions

doi: 10.1103/PhysRevC.85.044904
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2012AD17      Phys.Rev. C 86, 047901 (2012)

A.Adeluyi, C.A.Bertulani, M.J.Murray

Nuclear effects in photoproduction of heavy quarks and vector mesons in ultraperipheral PbPb and pPB collisions at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.86.047901
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2012BE02      Phys.Rev. C 85, 014321 (2012)

C.A.Bertulani, H.Liu, H.Sagawa

Global investigation of odd-even mass differences and radii with isospin-dependent pairing interactions

NUCLEAR STRUCTURE Z=8-102, N=8-156; calculated binding energies, S(n), S(p), neutron and proton odd-even staggering (OES), neutron and proton radii, neutron skin. Hartree-Fock HF+BCS model with SLy4 interactions, and isospin-dependent pairing (IS+IV) and Isoscalar (IS) pairing interactions using EV8odd computer code. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.014321
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2012BE30      J.Phys.:Conf.Ser. 337, 012007 (2012)

C.A.Bertulani, M.Karakoc

Medium Effects in Reactions with Rare Isotopes

NUCLEAR REACTIONS 9Be(15C, 14C), E=10-500 MeV/nucleon; analyzed data; deduced σ, dσ data of halo neutron knockout. 9Be(14O, 13O), (14O, 13N), E≈50, 300 MeV/nucleon; 9Be(36Ca, 35Ca), (36Ca, 35K), E=70.5, 300 MeV/nucleon; calculated spectroscopic factors using NuShell code, σ using modified MOMDIS code to solve Bethe-Goldstone equation considering medium effects via effective interaction.

doi: 10.1088/1742-6596/337/1/012007
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2012PO07      Phys.Rev. C 85, 041304 (2012)

I.Poltoratska, P.von Neumann-Cosel, A.Tamii, T.Adachi, C.A.Bertulani, J.Carter, M.Dozono, H.Fujita, K.Fujita, Y.Fujita, K.Hatanaka, M.Itoh, T.Kawabata, Y.Kalmykov, A.M.Krumbholz, E.Litvinova, H.Matsubara, K.Nakanishi, R.Neveling, H.Okamura, H.J.Ong, B.Ozel-Tashenov, V.Yu.Ponomarev, A.Richter, B.Rubio, H.Sakaguchi, Y.Sakemi, Y.Sasamoto, Y.Shimbara, Y.Shimizu, F.D.Smit, T.Suzuki, Y.Tameshige, J.Wambach, M.Yosoi, J.Zenihiro

Pygmy dipole resonance in 208Pb

NUCLEAR REACTIONS 208Pb(p, p'), E=295 MeV; measured Ep, Ip, σ(θ). 208Pb; deduced levels, J, π, PDR, σ(E1), σ(M1), B(E1). Multipole decomposition analysis based on DWBA calculations. Comparison with quasiparticle-phonon model (QPM), relativistic time-blocking approximation (RTBA), and shell model calculations. Separation of PDR and GDR strength with Coulomb-nuclear interference.

doi: 10.1103/PhysRevC.85.041304
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2011AD03      Rev.Mod.Phys. 83, 195 (2011)

E.G.Adelberger, A.Garcia, R.G.H.Robertson, K.A.Snover, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, A.B.Balantekin, K.Heeger, M.J.Ramsey-Musolf, D.Bemmerer, A.Junghans, D.Bemmerer, A.Junghans, C.A.Bertulani, K.-W.Chen, H.Costantini, P.Prati, M.Couder, E.Uberseder, M.Wiescher, R.Cyburt, B.Davids, S.J.Freedman, M.Gai, D.Gazit, L.Gialanella, G.Imbriani, U.Greife, M.Hass, W.C.Haxton, T.Itahashi, K.Kubodera, K.Langanke, D.Leitner, M.Leitner, P.Vetter, L.Winslow, L.E.Marcucci, T.Motobayashi, A.Mukhamedzhanov, R.E.Tribble, F.M.Nunes, T.-S.Park, R.Schiavilla, E.C.Simpson, C.Spitaleri, F.Strieder, H.-P.Trautvetter, K.Suemmerer, S.Typel

Solar fusion cross sections. II. The pp chain and CNO cycles

NUCLEAR REACTIONS 2H(p, γ), 3He(3He, 2p), (α, γ), (p, e), 7Be, 12C, 14N, 15N, 17O(p, γ), 15N, 16,17,18O(p, α), E<3 MeV; analyzed and evaluated experimental data; deduced recommended values and uncertainties.

doi: 10.1103/RevModPhys.83.195
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2011AD17      Phys.Rev. C 84, 024916 (2011)

A.Adeluyi, C.A.Bertulani

Gluon distributions in nuclei probed at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.84.024916
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2011HE24      J.Phys.:Conf.Ser. 312, 092029 (2011)

A.M.Heilmann, P.von Neumann-Cosel, A.Tamil, T.Adachi, C.Bertulani, J.Carter, H.Fujuita, Y.Fujita, K.Hatanaka, K.Hirota, On.H.Jin, T.Kawabata, A.Krugmann, H.Matsubara, E.Litvinova, R.Neveling, H.Okamura, B.Ozel-Tashenov, I.Poltoratska, V.Yu.Ponomarev, A.Richter, H.Sakaguchi, Y.Sakemi, Y.Sasamoto, Y.Shimizu, Y.Shimbara, F.D.Smit, T.Suzuki, Y.Tameshige, Y.Yasuda, M.Yosoi, J.Zenihiro

Electric dipole response in 120Sn

NUCLEAR REACTIONS 120Sn(polarized p, p'), E=295 MeV; measured Ep, Ip(θ=forward), proton polarization using high-resolution Grand Raiden magnetic spectrometer; deduced B(E1) strength distribution. Data of published DALINAC-S experiment with (γ, γ') used to extract B(E1) strengths.

doi: 10.1088/1742-6596/312/9/092029
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2011LI04      Phys.Rev. C 83, 011303 (2011)

H.L.Liu, F.R.Xu, P.M.Walker, C.A.Bertulani

Effects of high-order deformation on high-K isomers in superheavy nuclei

NUCLEAR STRUCTURE 254No; calculated potential energy surfaces, multi-quasiparticle states, levels, J, π, high-K isomers, neutron and proton single particle levels using the Woods-Saxon potential, β2, β4, β6 deformations. Configuration-constrained potential-energy-surface (PES) calculations. Effects of the β6 deformation on the high-K isomers. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.011303
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2011LI26      Phys.Rev. C 83, 067303 (2011)

H.L.Liu, F.R.Xu, P.M.Walker, C.A.Bertulani

Deformation and its influence on K isomerism in neutron-rich Hf nuclei

NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192Hf; calculated excitation energies, β2, β4 deformations for multi-qp isomeric states, configurations of K isomers, potential energy curves as function of γ deformation parameter. Configuration-constrained calculations of potential-energy surfaces. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.067303
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2011LO04      Phys.Rev. C 83, 024907 (2011)

W.H.Long, C.A.Bertulani

Nucleus-nucleus interaction between boosted nuclei

doi: 10.1103/PhysRevC.83.024907
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2011OG12      J.Phys.:Conf.Ser. 312, 082008 (2011)

K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro

Status of breakup reaction theory

NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.

doi: 10.1088/1742-6596/312/4/082008
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2011PI04      Phys.Rev. C 83, 045801 (2011)

R.G.Pizzone, C.Spitaleri, L.Lamia, C.Bertulani, A.Mukhamedzhanov, L.Blokhintsev, V.Burjan, S.Cherubini, Z.Hons, G.G.Kiss, V.Kroha, M.La Cognata, C.Li, J.Mrazek, S.Piskor, S.M.R.Puglia, G.G.Rapisarda, S.Romano, M.L.Sergi, A.Tumino

Trojan horse particle invariance studied with the 6Li(d, α)4He and 7Li( p, α)4He reactions

NUCLEAR REACTIONS 6Li(3He, 2α), E=17.5 MeV; measured Eα, Iα, angular distribution; deduced momentum distribution, Q value, quasifree (QF) contribution. 6Li(d, α), E(cm)=0-5 MeV; 7Li(p, α), E(cm)=0-7 MeV; 7Li(3He, 2α), E not given; analyzed excitation functions, σ, differential σ. Trojan horse method (THM) in the framework of the plane wave approximation.

doi: 10.1103/PhysRevC.83.045801
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0649. Data from this article have been entered in the XUNDL database. For more information, click here.


2011SA04      Phys.Rev. C 83, 024303 (2011)

A.R.Samana, F.Krmpotic, N.Paar, C.A.Bertulani

Neutrino and antineutrino charge-exchange reactions on 12C

NUCLEAR STRUCTURE 12B, 12N; calculated ground state energies, GT-B values, weak-interaction properties of ground states. QRPA and Projected quasiparticle random phase approximation (QRPA).

NUCLEAR REACTIONS 12C(ν, e-)12N, E=0-600 MeV; 12C(ν-bar, e+)12B, E=0-600 MeV; calculated exclusive and inclusive cross sections, sum rule, muon capture transition rates. Astrophysical significance to supernova neutrino spectra. QRPA and PQRPA models. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.024303
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2011TA18      Phys.Rev.Lett. 107, 062502 (2011)

A.Tamii, I.Poltoratska, P.von Neumann-Cosel, Y.Fujita, T.Adachi, C.A.Bertulani, J.Carter, M.Dozono, H.Fujita, K.Fujita, K.Hatanaka, D.Ishikawa, M.Itoh, T.Kawabata, Y.Kalmykov, A.M.Krumbholz, E.Litvinova, H.Matsubara, K.Nakanishi, R.Neveling, H.Okamura, H.J.Ong, B.Ozel-Tashenov, B.Rubio, H.Sakaguchi, Y.Sakemi, Y.Sasamoto, Y.Shimbara, Y.Shimizu, V.Yu.Ponomarev, A.Richter, F.D.Smit, T.Suzuki, Y.Tameshige, J.Wambach, R.Yamada, M.Yosoi, J.Zenihiro

Complete Electric Dipole Response and the Neutron Skin in 208Pb

NUCLEAR REACTIONS 208Pb(p, p'), E<20 MeV; measured reaction products, proton spectra; deduced electric dipole (E1) and spin magnetic dipole (M1) modes, E1 strength distribution, neutron skin thickness. Comparison with experimental data.

doi: 10.1103/PhysRevLett.107.062502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2355.


2011WA02      Phys.Rev. C 83, 018801 (2011)

B.Wang, C.A.Bertulani, A.B.Balantekin

Electron screening and its effects on big-bang nucleosynthesis

doi: 10.1103/PhysRevC.83.018801
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2010BE09      Phys.Rev. C 81, 044910 (2010)

C.A.Bertulani, M.Ellermann

Production of exotic atoms at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.81.044910
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2010BE17      Phys.Rev. C 81, 064603 (2010)

C.A.Bertulani, C.De Conti

Pauli blocking and medium effects in nucleon knockout reactions

NUCLEAR REACTIONS 9Be(11Be, 10Be), (15C, 14C), (34Ar, 33Ar), E=10-500 MeV/nucleon; calculated σ and transverse and longitudinal momentum distribution for one-nucleon knockout reactions. Free nucleon-nucleon cross sections obtained using eikonal approximation compared with geometrical treatment of Pauli blocking and with Dirac-Brueckner methods.

doi: 10.1103/PhysRevC.81.064603
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2010BE25      Nucl.Phys. A834, 643c (2010)

C.A.Bertulani

Nuclear Astrophysics in Rare Isotope Facilities

doi: 10.1016/j.nuclphysa.2010.01.112
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2010HU11      At.Data Nucl.Data Tables 96, 824 (2010)

J.T.Huang, C.A.Bertulani, V.Guimaraes

Radiative capture of nucleons at astrophysical energies with single-particle states

NUCLEAR REACTIONS 2H, 6,7Li, 7,9Be, 8B, 11,12,13C, 13,14,15N, 16O, 20Ne(p, γ), E(cm) < 3 MeV; 2H, 7,8Li, 11B, 12,14C, 15N, 16,18O(n, γ), E(cm) < 2 MeV; calculated binding energies, σ, S-factors, spectroscopic factors. Single-particle potential model.

doi: 10.1016/j.adt.2010.06.004
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2010LO03      Phys.Rev. C 81, 031302 (2010)

W.-H.Long, P.Ring, J.Meng, N.Van Giai, C.A.Bertulani

Nuclear halo structure and pseudospin symmetry

NUCLEAR STRUCTURE 40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74Ca, 56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94Ni, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Zr, 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174Sn, 122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Ce; calculated neutron skin thickness (rn-rp) using RHFB with PKA1 plus the D1S pairing force. 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198Ce; calculated neutron and proton densities, neutron single particle energies, Two-body interaction matrix elements Vab, neutron shell gap, halo structure near neutron drip line, and conservation of pseudospin symmetry using relativistic Hartree-Fock-Bogoliubov calculations.

doi: 10.1103/PhysRevC.81.031302
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2010OG02      Prog.Theor.Phys.(Kyoto) 123, 701 (2010)

K.Ogata, C.A.Bertulani

Dynamical Relativistic Effects in Breakup Processes of Halo Nuclei

NUCLEAR REACTIONS 208Pb(8B, X), (11Be, X), E=250 MeV/nucleon; 8B, 11Be; calculated dynamical relativistic effects on breakup σ(θ), σ(E, θ) in halo nuclei. Continuum-Discretized Coupled-Channels method (CDCC).

doi: 10.1143/PTP.123.701
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2009BE10      Phys.Rev. C 79, 034306 (2009)

G.F.Bertsch, C.A.Bertulani, W.Nazarewicz, N.Schunck, M.V.Stoitsov

Odd-even mass differences from self-consistent mean field theory

NUCLEAR STRUCTURE A=50-250, N=10-150, Z=10-102; calculated odd-even staggering in nuclear binding energies using density functional theory and and multiple treatments of pairing interactions; Sn, N=55-85, Dy, N=79-101, Pb, N=99-131, Z=65-81, N=98, 102; calculated binding energy differences. 25Ne, 39P, 52Ti, 61Cu, 87Kr, 111Ag, 147Gd, 173Tm, 203Tl, 207Pb; calculated deformation parameters. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.034306
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