NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = H.Esbensen Found 136 matches. Showing 1 to 100. [Next]2018CO08 Phys.Rev. C 97, 044613 (2018) G.Colucci, G.Montagnoli, A.M.Stefanini, H.Esbensen, D.Bourgin, P.Colovic, L.Corradi, M.Faggian, E.Fioretto, F.Galtarossa, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, F.Scarlassara, C.Stefanini, E.Strano, S.Szilner, M.Urbani, G.L.Zhang Isotopic effects in sub-barrier fusion of Si + Si systems NUCLEAR REACTIONS 30Si(30Si, X), E=47-90 MeV; measured fusion evaporation residues (ERs), fusion σ(E) at the XTU tandem accelerator facility of LNL-INFN-Legnaro. Comparison with previous experimental results, 28Si+28Si data, and with theoretical calculations using coupled-channels method with aM3Y+repulsion potential, and including one- and two-phonon excitations and the mutual excitations of the low-lying 2+ and 3- states in projectiles and targets.
doi: 10.1103/PhysRevC.97.044613
2017ST12 Phys.Rev. C 96, 014603 (2017) A.M.Stefanini, G.Montagnoli, H.Esbensen, P.Colovic, L.Corradi, E.Fioretto, F.Galtarossa, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, N.Soic, E.Strano, S.Szilner New results in low-energy fusion of 40Ca + 90, 92Zr NUCLEAR REACTIONS 90,92Zr(40Ca, X), E=128-155 MeV; measured evaporation residues (ER), fusion yields, angular distribution of ERs at XTU Tandem accelerator of the INFN-LNL-Legnaro. 90,94,96Zr(40Ca, X), E(cm)=80-110 MeV; analyzed previous experimental data for fusion σ(E); deduced parameters of the Woods-Saxon ion-ion potential, strength of the pair-transfer coupling, astrophysical S factors, one- and multi-phonon excitations of the low-lying collective modes. Comparison with coupled-channel (CC) calculations.
doi: 10.1103/PhysRevC.96.014603
2016ES01 Phys.Rev. C 93, 034609 (2016) H.Esbensen, G.Montagnoli, A.M.Stefanini Revised analysis of 40Ca + 96Zr fusion reactions NUCLEAR REACTIONS 90,96Zr(40Ca, X), E(cm)=80-115 MeV; analyzed fusion σ(E) data using Ch-1, Ch-27, Ch-28 and Ch-84 potentials. 96Zr(40Ca, X), E(cm)=80-115 MeV; analyzed fusion σ(E), transfer probabilities for one- and two-neutron transfers as functions of distance of closest approach, barrier distributions, S factors for fusion cross sections, scaling factor for the transfer strengths. Coupled-channels calculations based on standard Woods-Saxon potential, including couplings to multiphonon excitations and transfer channels.
doi: 10.1103/PhysRevC.93.034609
2016RE17 Phys.Rev. C 94, 044612 (2016) K.E.Rehm, H.Esbensen, C.L.Jiang, B.B.Back, A.M.Stefanini, G.Montagnoli Moments of fusion-barrier distributions NUCLEAR REACTIONS 40,48Ca, 58,64Ni, 90,96Zr(40Ca, X), 40,48Ca, 90,96Zr(48Ca, X), 48Ca, 58,64Ni, 90,96Zr, 110Pd(32S, X), 48Ca, 64Ni, 90,96Zr, 110Pd(36S, X), 58,64Ni, 132Sn(58Ni, X), 144,148,154Sm, 186W(16O, X), 154Sm(28Si, X), 232Th(15C, X), 209Bi(6He, X), E=85-200 MeV; analyzed fusion radius parameter, moments M1, M2 and M3 of fusion barrier distributions using a new method.
doi: 10.1103/PhysRevC.94.044612
2015JI05 Phys.Rev. C 91, 044602 (2015) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, S.Almaraz-Calderon, M.L.Avila, B.B.Back, D.Bourgin, L.Corradi, S.Courtin, E.Fioretto, F.Galtarossa, A.Goasduff, F.Haas, M.M.Mazzocco, D.Montanari, G.Montagnoli, T.Mijatovic, R.Sagaidak, D.Santiago-Gonzalez, F.Scarlassara, E.E.Strano, S.Szilner Fusion reactions of 58, 64Ni+124Sn NUCLEAR REACTIONS 124Sn(58Ni, X), (64Ni, X), E(cm)=140-165 MeV; measured evaporation residue spectra, fusion σ(E), σ(θ). Coupled-channels calculations to study reaction mechanism. Discussed role of transfer reactions in heavy system, and S-factor maximum. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.044602
2015MO08 Phys.Lett. B 746, 300 (2015) G.Montagnoli, A.M.Stefanini, H.Esbensen, L.Corradi, S.Courtin, E.Fioretto, J.Grebosz, F.Haas, H.M.Jia, C.L.Jiang, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, F.Scarlassara, E.Strano, S.Szilner, D.Torresi Oscillations above the barrier in the fusion of 28Si + 28Si NUCLEAR REACTIONS 28Si(28Si, X), E=62-78 MeV; measured fusion evaporation residues; deduced fusion σ. Comparison with coupled-channel model using the shallow M3Y + repulsion potential.
doi: 10.1016/j.physletb.2015.05.021
2014CA08 Phys.Rev.Lett. 112, 192701 (2014) P.F.F.Carnelli, S.Almaraz-Calderon, K.E.Rehm, M.Albers, M.Alcorta, P.F.Bertone, B.Digiovine, H.Esbensen, J.O.Fernandez Niello, D.Henderson, C.L.Jiang, J.Lai, S.T.Marley, O.Nusair, T.Palchan-Hazan, R.C.Pardo, M.Paul, C.Ugalde Measurements of Fusion Reactions of Low-Intensity Radioactive Carbon Beams on 12C and their Implications for the Understanding of X-Ray Bursts NUCLEAR REACTIONS 12C(10C, X), (12C, X), (13C, X), (14C, X), (15C, X), E=40-50 MeV; measured fusion reaction products; deduced S-factors, σ. Time-dependent HF calculations.
doi: 10.1103/PhysRevLett.112.192701
2014ES01 Phys.Rev. C 89, 044616 (2014) Influence of multiphonon excitations and transfer on the fusion of Ca+Zr NUCLEAR REACTIONS 90,96Zr(40Ca, X), (48Ca, X), E(cm)=85-115 MeV; calculated fusion σ(E), barrier distributions, energy weighted fusion σ(E). Coupled-channel calculations using Woods-Saxon potential, M3Y+repulsion double-folding potential, and nuclear structure input for 40,48Ca, 90,96Zr from ENSDF database. Discussed effects of coupling to multiphonon excitations and transfer channels. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.044616
2014JI02 Phys.Rev. C 89, 051603 (2014) C.L.Jiang, K.E.Rehm, B.B.Back, H.Esbensen, R.V.F.Janssens, A.M.Stefanini, G.Montagnoli Influence of heavy-ion transfer on fusion reactions NUCLEAR REACTIONS 40,48Ca(40Ca, X), 48Ca(48Ca, X), E=45-65 MeV; 58,64Ni(28Si, X), 64Ni(30Si, X), E=42-66 MeV; 40,48Ca(32S, X), 48Ca(36S, X), E=36-56 MeV; 58,64Ni(58Ni, X), 64Ni(64Ni, X), E=85-114 MeV; 124,132Sn(40Ca, X), 132Sn(48Ca, X), E=104-138 MeV; 124,132Sn(58Ni, X), 132Sn(64Ni, X), E=145-200 MeV; analyzed fusion σ(E) using Wong formula; calculated average excitation energies of residual nuclei following neutron pickup reactions; deduced correlation between fusion enhancement and strength of total neutron-transfer cross sections.
doi: 10.1103/PhysRevC.89.051603
2014JI04 Phys.Rev.Lett. 113, 022701 (2014) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, S.Almaraz-Calderon, B.B.Back, L.Corradi, E.Fioretto, G.Montagnoli, F.Scarlassara, D.Montanari, S.Courtin, D.Bourgin, F.Haas, A.Goasduff, S.Szilner, T.Mijatovic Fusion Hindrance for a Positive-Q-Value System 24Mg + 30Si NUCLEAR REACTIONS 30Si(24Mg, X), E<30 MeV; measured fusion reaction products; deduced σ, S-factors.
doi: 10.1103/PhysRevLett.113.022701
2014MO33 Phys.Rev. C 90, 044608 (2014) G.Montagnoli, A.M.Stefanini, H.Esbensen, C.L.Jiang, L.Corradi, S.Courtin, E.Fioretto, J.Grebosz, F.Haas, H.M.Jia, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, F.Scarlassara, E.Strano, S.Szilner, D.Torresi Fusion of 28Si + 28, 30 Different trends at sub-barrier energies NUCLEAR REACTIONS 28,30Si(28Si, X), E=46-86 MeV; measured particle spectra, fusion σ(E), fragment energy and angular distributions using an electrostatic beam separator at INFN-LNL's XTU Tandem accelerator facility; deduced logarithmic derivatives, S-factors, double-phonon excitations, influence of transfer channels and nuclear deformation. Comparison with coupled channel calculations using various potentials.
doi: 10.1103/PhysRevC.90.044608
2014ST02 Phys.Lett. B 728, 639 (2014) A.M.Stefanini, G.Montagnoli, H.Esbensen, L.Corradi, S.Courtin, E.Fioretto, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, G.Pasqualato, C.Parascandolo, F.Scarlassara, E.Strano, S.Szilner, D.Torresi Fusion of 40Ca + 96Zr revisited: Transfer couplings and hindrance far below the barrier NUCLEAR REACTIONS 96Zr(40Ca, X), E=120-152 MeV; measured reaction products, fusion residue; deduced fusion σ, hindrance effect. Coupled-channels analysis, comparison with available data.
doi: 10.1016/j.physletb.2013.12.048
2013JI01 Phys.Rev.Lett. 110, 072701 (2013) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm, R.J.Charity Origin and Consequences of 12C+12C Fusion Resonances at Deep Sub-barrier Energies NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, 13C(13C, X)26Mg, 12C(16O, X)28Si, 16O(16O, X)32S, E(cm)<10 MeV; analyzed available fusion σ, S-factors; deduced resonance behavior of fusion reactions at low energies.
doi: 10.1103/PhysRevLett.110.072701
2013MO01 Phys.Rev. C 87, 014611 (2013) G.Montagnoli, A.M.Stefanini, H.Esbensen, C.L.Jiang, L.Corradi, S.Courtin, E.Fioretto, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, K.E.Rehm, F.Scarlassara, S.Szilner, X.D.Tang, C.A.Ur Effects of transfer channels on near- and sub-barrier fusion of 32S + 48Ca NUCLEAR REACTIONS 48Ca(32S, X), E=60.0-89.4 MeV; measured reaction products, σ(θ, E), fusion σ(E) at Legnaro facility; deduced logarithmic slope. 48Ca(32S, X), (36S, X), E(cm)=35-60 MeV; analyzed fusion σ(E) data, energy-weighted fusion cross sections, astrophysical S factor. Coupled channel analysis with M3Y+repulsion, double-folding potential.
doi: 10.1103/PhysRevC.87.014611
2013ST14 Eur.Phys.J. A 49, 63 (2013) A.M.Stefanini, G.Montagnoli, F.Scarlassara, C.L.Jiang, H.Esbensen, E.Fioretto, L.Corradi, B.B.Back, C.M.Deibel, B.Di Giovine, J.P.Greene, H.D.Henderson, S.T.Marley, M.Notani, N.Patel, K.E.Rehm, D.Sewerinyak, X.D.Tang, C.Ugalde, S.Zhu Fusion of 60Ni + 100Mo near and below the Coulomb barrier - Multi-phonon and transfer couplings down to the hindrance region NUCLEAR REACTIONS 100Mo(60Ni, X), (64Ni, X), E=196-262 MeV; measured particle tracks; deduced fusion σ, logarithmic excitation function slope; calculated fusion σ using CCFULL CC code.
doi: 10.1140/epja/i2013-13063-2
2012CA18 Phys.Rev. C 85, 044604 (2012) P.Capel, H.Esbensen, F.M.Nunes Comparing nonperturbative models of the breakup of neutron-halo nuclei NUCLEAR REACTIONS 208Pb(15C, n14C), E=20, 68 MeV/nucleon; calculated differential σ(E, θ) from breakup modes: continuum discretized coupled channel (CDCC), time-dependent method, semiclassical approximation, and dynamical eikonal approximation. Halo nuclei. Comparison with experimental data. Relevance to 14C(n, γ)15C reaction.
doi: 10.1103/PhysRevC.85.044604
2012ES04 Phys.Rev. C 85, 064611 (2012) Structures in high-energy fusion data NUCLEAR REACTIONS 16O(16O, X), 12C, 16O(12C, X), E(cm)=5-35 MeV; 28Si(28Si, X), E(cm)=25-100 MeV; analyzed fusion σ(E), energy weighted cross section derivatives as function of incident energy. Hill-Wheeler and Wong formulas. Coupled channel calculations based on M3Y+repulsion potential.
doi: 10.1103/PhysRevC.85.064611
2012MO05 Phys.Rev. C 85, 024607 (2012) G.Montagnoli, A.M.Stefanini, C.L.Jiang, H.Esbensen, L.Corradi, S.Courtin, E.Fioretto, A.Goasduff, F.Haas, A.F.Kifle, C.Michelagnoli, D.Montanari, T.Mijatovic, K.E.Rehm, R.Silvestri, PushpendraP.Singh, F.Scarlassara, S.Szilner, X.D.Tang, C.A.Ur Fusion of 40Ca+40Ca and other Ca+Ca systems near and below the barrier NUCLEAR REACTIONS 40Ca(40Ca, X), E=98-130 MeV; measured evaporation residue spectra, σ(E); deduced barrier distribution, astrophysical S factor. 48Ca(48Ca, X), E(cm)=45-70 MeV; analyzed fusion σ(E), barrier distributions. Comparison with previous experimental data and with coupled-channel calculations based on Woods-Saxon (WS), M3Y+repulsion potentials.
doi: 10.1103/PhysRevC.85.024607
2012NO01 Phys.Rev. C 85, 014607 (2012) M.Notani, H.Esbensen, X.Fang, B.Bucher, P.Davies, C.L.Jiang, L.Lamm, C.J.Lin, C.Ma, E.Martin, K.E.Rehm, W.P.Tan, S.Thomas, X.D.Tang, E.Brown Correlation between the 12C+12C, 12C+13C, and 13C+13C fusion cross sections NUCLEAR REACTIONS 12C(13C, p)24Na, 13C(13C, np)24Na, E(cm)=2.6-4.8 MeV; measured Eγ, Iγ, βγ-coin from 24Na decay; deduced thick target yield by activation method, GEANT4 simulation, fusion cross section, S factors. 12C(12C, X), (13C, X), 13C(13C, X), E(cm)=2.5-6.5 MeV; analyzed fusion cross sections, fusion barrier parameters, spectroscopic factors by fitting with Wong formula. Comparison of experimental data with two coupled-channels calculations using ingoing wave boundary condition (IWBC).
doi: 10.1103/PhysRevC.85.014607
2012TA13 J.Phys.:Conf.Ser. 337, 012016 (2012) X.D.Tang, X.Fang, B.Bucher, H.Esbensen, C.L.Jiang, K.E.Rehm, C.J.Lin Upper Limit on the molecular resonance strengths in the 12C+ 12C fusion reaction NUCLEAR REACTIONS 12,13C(12C, X), (13C, X), E(cm)=2-6.5 MeV; analyzed published data on fusion reaction S-factor; deduced average S-factor, resonances, upper limit for molecular resonance strengths, empirical relationship using CRC-AW and EWS (equivalent square well).
doi: 10.1088/1742-6596/337/1/012016
2012TA24 J.Phys.:Conf.Ser. 381, 012120 (2012) X.D.Tang, H.Esbensen, X.Fang, B.Bucher, C.L.Jiang, K.E.Rehm, C.J.Lin, E.Brown Does the 12C+12C fusion reaction trigger superburst? NUCLEAR REACTIONS 12C(12C, X), (13C, X), E(cm)≈2.0-6.5 MeV;13C(13C, X), E(cm)≈2.9-6.5 MeV; calculated fusion reaction rate, modified S-factor using CC with IWBC (incoming wave boundary condition) and different interactions. Discussed role of possible resonance near E(cm)≈1.5 MeV.
doi: 10.1088/1742-6596/381/1/012120
2011AL09 Phys.Rev.Lett. 106, 172701 (2011) M.Alcorta, K.E.Rehm, B.B.Back, S.Bedoor, P.F.Bertone, C.M.Deibel, B.DiGiovine, H.Esbensen, J.P.Greene, C.R.Hoffmann, C.L.Jiang, J.C.Lighthall, S.T.Marley, R.C.Pardo, M.Paul, A.M.Rogers, C.Ugalde, A.H.Wuosmaa Fusion Reactions with the One-Neutron Halo Nucleus 15C NUCLEAR REACTIONS 232Th(13C, X), (14C, X), (15C, X), E(cm)=50-70 MeV; measured fusion fission fragments; deduced yields, σ, 15C+232Th cross section enhancement. Comparison with experimental data, couple-channel calculations.
doi: 10.1103/PhysRevLett.106.172701
2011ES08 Phys.Rev. C 84, 064613 (2011) Effects of mutual excitations in the fusion of carbon isotopes NUCLEAR REACTIONS 13C(13C, X), E(cm)=0-18 MeV; 13C(12C, X), E(cm)=2-7 MeV; 12C(12C, X), E(cm)=1-9 MeV; calculated fusion cross section, S factors. Coupled-channels calculations based on the M3Y+repulsion, double-folding potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064613
2011JI14 J.Phys.:Conf.Ser. 312, 042011 (2011) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm, X.D.Tang Do we understand heavy-ion fusion reactions of importance in stellar evolution? NUCLEAR REACTIONS 10B(10B, X), E≈0.9-3.5 MeV;16O(16O, X), E≈5.5-11.5 MeV;30Si(28Si, X), E≈23-30 MeV;48Ca(36S, X), E≈36-48 MeV;48Ca(40Ca, X), E≈46-56 MeV;48Ca(48Ca, X), E≈46-56 MeV;45Sc(27Al, X), E≈31=39 MeV;64Ni(28Si, X), E≈43-52 MeV;64Ni(64Ni, X), E≈84-100 MeV;92Zr(90Zr, X), E≈165-177 MeV; re-analyzed S-factors in fusion reactions; calculated S-factors, fusion hinderance effect.
doi: 10.1088/1742-6596/312/4/042011
2010ES03 Phys.Rev. C 81, 034606 (2010) Complete fusion of 9Be with spherical targets NUCLEAR REACTIONS 144Sm, 208Pb(9Be, X), E(cm)=25-45 MeV; calculated complete fusion and incomplete fusion cross sections with double-folding potential applied in coupled channels calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.034606
2010ES07 Phys.Rev. C 82, 054621 (2010) H.Esbensen, C.L.Jiang, A.M.Stefanini Hindrance in the fusion of 48Ca+48Ca NUCLEAR REACTIONS 48Ca(48Ca, X), E(cm)=45-60 MeV; analyzed fusion σ, rms radii, and S factors using coupled-channel (CC) method with Woods-Saxon and M3Y+repulsion potentials.
doi: 10.1103/PhysRevC.82.054621
2010JI03 Phys.Rev. C 81, 024611 (2010) C.L.Jiang, K.E.Rehm, H.Esbensen, B.B.Back, R.V.F.Janssens, P.Collon, C.M.Deibel, B.DiGiovine, J.M.Figueira, J.P.Greene, D.J.Henderson, H.Y.Lee, M.Notani, S.T.Marley, R.C.Pardo, N.Patel, D.Seweryniak, X.D.Tang, C.Ugalde, S.Zhu Fusion hindrance for 27Al+45Sc and other systems with a positive Q value NUCLEAR REACTIONS 45Sc(27Al, X), E=51-82 MeV; measured fragment spectra, σ, astrophysical S-factor. Comparison with coupled-channels calculations. 14N(14N, X), E=4-11 MeV; 30Si(28Si, X), E=25-31 MeV; 45Sc(27Al, X), E=32-39 MeV; 64Ni(28Si, X), E=44-51 MeV; 40Ca(40Ca, X), E=49-57 MeV; 48Ca(48Ca, X), E=46-56 MeV; 48Ca(36S, X), E=37-48 MeV; comparison of measured cross sections and astrophysical S-factors with coupled-channel calculations.
doi: 10.1103/PhysRevC.81.024611
2010JI14 Phys.Rev. C 82, 041601 (2010) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, L.Corradi, E.Fioretto, P.Mason, G.Montagnoli, F.Scarlassara, R.Silvestri, P.P.Singh, S.Szilner, X.D.Tang, C.A.Ur Fusion hindrance for Ca+Ca systems: Influence of neutron excess NUCLEAR REACTIONS 48Ca(40Ca, X), E=89.2, 107.7 MeV; measured particle spectra, σ(E, θ); deduced S factors. Comparisons of experimental σ(E) for 40Ca+40Ca, 40Ca+48Ca, 48Ca+48Ca, 40Ca+90Zr, 40Ca+96Zr and 48Ca+96Zr systems with coupled-channel calculations.
doi: 10.1103/PhysRevC.82.041601
2010SI15 Eur.Phys.J. A 44, 63 (2010) C.Signorini, D.Pierroutsakou, B.Martin, M.Mazzocco, T.Glodariu, R.Bonetti, A.Guglielmetti, M.La Commara, M.Romoli, M.Sandoli, E.Vardaci, H.Esbensen, F.Farinon, P.Molini, C.Parascandolo, F.Soramel, S.Sidortchuk, L.Stroe Interaction of 17F with a 208Pb target below the Coulomb barrier NUCLEAR REACTIONS 208Pb(17F, 17F), (17F, 16O), E=86 MeV; measured E(fragment), I(fragment), Ep, Ip, p(fragment)-coin, σ, σ(θ). DWBA analysis. Comparison with optical model, data and systematics. Secondary radioactive beam.
doi: 10.1140/epja/i2010-10934-x
2009ES01 Phys.Rev. C 79, 064619 (2009) Indications of a shallow potential in 48Ca+96Zr fusion reactions NUCLEAR REACTIONS 96Zr(48Ca, X), E=86-115 MeV; 90,94,96Zr(40Ca, X), 90Zr(48Ca, X), E=78-96 MeV; analyzed fusion σ, barrier distributions and astrophysical S factors using coupled-channels calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064619
2009ES02 Phys.Rev. C 80, 024608 (2009); Erratum, Phys.Rev. C 80, 059904 (2009) Coulomb dissociation of 15C and radiative neutron capture on 14C NUCLEAR REACTIONS Pb(15C, X), E=68 MeV/nucleon; analyzed previously measured decay spectra; deduced σ, dipole and quadrupole responses, diffraction dissociation probabilities. 14C(n, γ), E not given; deduced σ for g.s. and first excited state.
doi: 10.1103/PhysRevC.80.024608
2009LI45 Phys.Lett. B 681, 22 (2009) J.F.Liang, J.R.Beene, A.L.Caraley, H.Esbensen, A.Galindo-Uribarri, C.J.Gross, P.E.Mueller, K.T.Schmitt, D.Shapira, D.W.Stracener, R.L.Varner Dynamic polarization in the Coulomb breakup of loosely bound 17F NUCLEAR REACTIONS 58Ni, 208Pb(17F, p), E=10 MeV/nucleon; measured Ep, Ip, (fragment)p-coin, σ(θ) using silicon strip detectors. Comparison with first-order perturbation and dynamical calculations and effect of dynamic polarization discussed.
doi: 10.1016/j.physletb.2009.09.055
2008ES03 Phys.Rev. C 77, 054608 (2008) Coupled-channels calculations of 16O+16O fusion NUCLEAR STRUCTURE 16O(16O, X), E(cm)=2-35 MeV; calculated neutron spectra, fusion σ, spectroscopic factors. Woods Saxon Potential and M3Y+repulsion coupled-channel calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.054608
2008ES04 Phys.Rev. C 78, 024608 (2008) Coulomb excitation at intermediate energies NUCLEAR REACTIONS Au(24Mg, 24Mg'), (32Mg, 32Mg'), (26Si, 26Si'), (38S, 38S'), (40S, 40S'), (42S, 42S'), (44Ar, 44Ar'), (46Ar, 46Ar'), (11Be, 11Be'), E=30-72.3 MeV/nucleon; Bi(26Mg, X), (34Mg, X), E=30-70 MeV/nucleon; calculated σ; 24,2632Mg, 26Si, 38,40,42S, 44,46; calculated B(E2); 11Be; calculated B(E1). Pb(16N, X), (46Ar, X), (54Ni, X), E=10-500 MeV/nucleon; calculated cross sections.
doi: 10.1103/PhysRevC.78.024608
2008JI04 Phys.Rev. C 78, 017601 (2008) C.L.Jiang, B.B.Back, H.Esbensen, J.P.Greene, R.V.F.Janssens, D.J.Henderson, H.Y.Lee, C.J.Lister, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, D.Seweryniak, B.Shumard, X.Wang, S.Zhu, S.Misicu, P.Collon, X.D.Tang Fusion hindrance for a positive Q-value system NUCLEAR REACTIONS 30Si(28Si, X), E=48.5-71 MeV; measured excitation functions, fusion σ. 12C(12C, X); systematics of Q-values. Comparisons with model calculations.
doi: 10.1103/PhysRevC.78.017601
2007ES04 Phys.Rev. C 76, 024302 (2007) H.Esbensen, K.Hagino, P.Mueller, H.Sagawa Charge radius and dipole response of 11Li NUCLEAR STRUCTURE 11Li; calculated dipole response and charge radius. Compared results to available data.
doi: 10.1103/PhysRevC.76.024302
2007ES08 Phys.Rev. C 76, 054609 (2007) Hindrance of 16O+208Pb fusion at extreme sub-barrier energies NUCLEAR REACTIONS 208Pb(16O, X)17O, E(cm)=63-115 MeV; calculated reaction cross sections, S-factors using coupled-channel calculations.
doi: 10.1103/PhysRevC.76.054609
2007MI06 Phys.Rev. C 75, 034606 (2007) Signature of shallow potentials in deep sub-barrier fusion reactions NUCLEAR REACTIONS 58Ni(58Ni, X), 64Ni(64Ni, X), E=85-110 MeV; 100Mo(64Ni, X), E=115-155 MeV; calculated fusion excitation functions, S-factors. Comparison with data.
doi: 10.1103/PhysRevC.75.034606
2006JI01 Phys.Rev. C 73, 014613 (2006) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm Systematics of heavy-ion fusion hindrance at extreme sub-barrier energies NUCLEAR REACTIONS 64Ni(58Ni, X), (64Ni, X), E ≈ 85-105 MeV; 10B(10B, X), 12C(11B, X), (13C, X), 16O(12C, X), (16O, X), E ≈ 2-17 MeV; 64Ni(28Si, X), 48Ca(48Ca, X), E ≈ 45-60 MeV; 89Y(60Ni, X), 92Zr(90Zr, X), E ≈ 120-180 MeV; analyzed fusion σ, sub-barrier hindrance.
doi: 10.1103/PhysRevC.73.014613
2006JI06 Phys.Lett. B 640, 18 (2006) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, S.Misicu, K.E.Rehm, P.Collon, C.N.Davids, J.Greene, D.J.Henderson, L.Jisonna, S.Kurtz, C.J.Lister, M.Notani, M.Paul, R.Pardo, D.Peterson, D.Seweryniak, B.Shumard, X.D.Tang, I.Tanihata, X.Wang, S.Zhu First evidence of fusion hindrance for a small Q-value system NUCLEAR REACTIONS 64Ni(28Si, X), E=63-95 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. Coupled-channels analysis.
doi: 10.1016/j.physletb.2006.07.007
2006MI09 Phys.Rev.Lett. 96, 112701 (2006) Hindrance of Heavy-Ion Fusion due to Nuclear Incompressibility NUCLEAR REACTIONS 64Ni(64Ni, X), E(cm)=85-110 MeV; analyzed fusion σ; deduced role of incompressibility in sub-barrier hindrance. Coupled-channels approach.
doi: 10.1103/PhysRevLett.96.112701
2005ES02 Phys.Rev.Lett. 94, 042502 (2005) H.Esbensen, G.F.Bertsch, K.A.Snover Reconciling Coulomb Dissociation and Radiative Capture Measurements NUCLEAR REACTIONS Pb(8B, p7Be), E=51.9 MeV/nucleon; calculated relative energy spectra, angular distributions. 7Be(p, γ), E=low; analyzed astrophysical S-factor data.
doi: 10.1103/PhysRevLett.94.042502
2005ES12 Phys.Rev. C 72, 054607 (2005) Sensitivity to multi-phonon excitations in heavy-ion fusion reactions NUCLEAR REACTIONS 64Ni, 74Ge, 100Mo(64Ni, X), E(cm)=80-150 MeV; 74Ge(74Ge, X), E(cm)=100-155 MeV; calculated fusion σ, effects of multi-phonon excitation. Comparison with data.
doi: 10.1103/PhysRevC.72.054607
2005JI02 Phys.Rev. C 71, 044613 (2005) C.L.Jiang, K.E.Rehm, H.Esbensen, R.V.F.Janssens, B.B.Back, C.N.Davids, J.P.Greene, D.J.Henderson, C.J.Lister, R.C.Pardo, T.Pennington, D.Peterson, D.Seweryniak, B.Shumard, S.Sinha, X.D.Tang, I.Tanihata, S.Zhu, P.Collon, S.Kurtz, M.Paul Hindrance of heavy-ion fusion at extreme sub-barrier energies in open-shell colliding systems NUCLEAR REACTIONS 100Mo(64Ni, X), E=196-262 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. 58,60,64Ni, 74Ge, 90,91,94Zr, 92,100Mo, 124Sn(58Ni, X), 89Y(60Ni, X), 64Ni, 74Ge, 92,96Zr, 92,100Mo, 124Sn(64Ni, X), E(cm) ≈ 120 MeV; analyzed fusion σ, sub-barrier hindrance.
doi: 10.1103/PhysRevC.71.044613
2004DA10 Phys.Rev. C 69, 034314 (2004) Decay rate of triaxially deformed proton emitters RADIOACTIVITY 141Ho(p); calculated decay rate, branching ratio vs triaxial deformation parameter.
doi: 10.1103/PhysRevC.69.034314
2004ES03 Prog.Theor.Phys.(Kyoto), Suppl. 154, 11 (2004) Challenges in Coupled-Channels Calculations of Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 74Ge(27Al, X), E(cm) ≈ 45-65 MeV; 64Ni(64Ni, X), E(cm) ≈ 85-110 MeV; calculated fusion σ, barrier distributions. Coupled-channels approach, comparison with data.
doi: 10.1143/PTPS.154.11
2004ES05 Phys.Rev. C 70, 047603 (2004) Constraints on the 7Be(p, γ)8B radiative capture rate from charge symmetry NUCLEAR REACTIONS 7Li(n, γ), E < 1000 keV; 7Be(p, γ), E(cm) < 3 MeV; calculated radiative capture σ, astrophysical S-factors. Comparison with data.
doi: 10.1103/PhysRevC.70.047603
2004JI01 Phys.Rev. C 69, 014604 (2004) C.L.Jiang, H.Esbensen, B.B.Back, R.V.F.Janssens, K.E.Rehm Analysis of heavy-ion fusion reactions at extreme sub-barrier energies NUCLEAR REACTIONS 89Y(60Ni, X), E=115-140 MeV; analyzed fusion σ, barrier distribution. 58Ni(58Ni, X), 89Y(60Ni, X), 89Y, 90,92Zr(90Zr, X), 144Sm, 208Pb(16O, X), 208Pb(19F, X), (50Ti, X), 64Ni(64Ni, X), E ≈ 100-300 MeV; analyzed fusion S-factors. Coupled-channels approach.
doi: 10.1103/PhysRevC.69.014604
2004JI05 Phys.Rev.Lett. 93, 012701 (2004) C.L.Jiang, K.E.Rehm, R.V.F.Janssens, H.Esbensen, I.Ahmad, B.B.Back, P.Collon, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, M.Paul, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou Influence of Nuclear Structure on Sub-Barrier Hindrance in Ni + Ni Fusion NUCLEAR REACTIONS 64Ni(64Ni, X), E=171-220 MeV; measured fusion excitation function; deduced structure effects in sub-barrier hindrance. Comparison with similar reactions.
doi: 10.1103/PhysRevLett.93.012701
2004JI07 Prog.Theor.Phys.(Kyoto), Suppl. 154, 61 (2004) C.L.Jiang, H.Esbensen, K.E.Rehm, B.B.Back, R.V.F.Janssens, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou, M.Paul, P.Collon, J.A.Caggiano, A.M.Heinz, I.Nishinaka Systematics of Heavy-Ion Fusion Reactions at Extreme Sub-Barrier Energies NUCLEAR REACTIONS 64Ni(64Ni, X), E=172-212 MeV; measured fusion excitation function; deduced barrier distribution. Fragment mass analyzer, S-factor analysis, fusion reaction systematics discussed.
doi: 10.1143/PTPS.154.61
2003ES07 Phys.Rev. C 68, 034604 (2003) Fusion reactions with germanium isotopes NUCLEAR REACTIONS 70,72,74,76Ge(27Al, X), E(cm) ≈ 48-65 MeV; 70,72,74,76Ge(16O, X), E(cm) ≈ 30-55 MeV; analyzed fusion σ; deduced deformation effects, other reaction mechanism features. Coupled-channels approach.
doi: 10.1103/PhysRevC.68.034604
2003LI14 Phys.Rev. C 67, 044603 (2003) J.F.Liang, J.R.Beene, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, P.A.Hausladen, P.E.Mueller, D.Shapira, D.W.Stracener, R.L.Varner, J.D.Bierman, H.Esbensen, Y.Larochelle Breakup of 17F on 208Pb near the Coulomb barrier NUCLEAR REACTIONS 208Pb(17F, 16OX), E=98, 120 MeV; measured oxygen particles σ(θ); deduced reaction mechanism features. 208Pb(17F, 17F), E=98, 120 MeV; measured σ(θ). 208Pb(17F, X), E(cm) ≈ 70-120 MeV; calculated fusion σ.
doi: 10.1103/PhysRevC.67.044603
2002BF01 Prog.Theor.Phys.(Kyoto), Suppl. 146, 319 (2002) Dynamic Effects in Fragmentation Reactions NUCLEAR REACTIONS 208Pb(17F, X), E=10 MeV/nucleon; calculated breakup probability, role of Barkas effect.
doi: 10.1143/PTPS.146.319
2002DA15 Nucl.Phys. A701, 14c (2002) B.Davids, D.W.Anthony, T.Aumann, S.M.Austin, T.Baumann, D.Bazin, R.R.C.Clement, P.A.Lofy, T.Nakamura, B.M.Sherrill, J.Yurkon, C.N.Davids, H.Esbensen A Kinematically Complete Measurement of the Coulomb Dissociation of 8B NUCLEAR REACTIONS Pb(8B, p7Be), E=83 MeV/nucleon; measured particle spectra; deduced Coulomb dissociation σ. 7Be(p, γ), E=low; deduced astrophysical S-factor. Kinematically complete measurement.
doi: 10.1016/S0375-9474(01)01538-X
2002DA26 Eur.Phys.J. A 15, 65 (2002) B.Davids, S.M.Austin, D.Bazin, H.Esbensen, B.M.Sherrill, I.J.Thompson, J.A.Tostevin Coulomb breakup of 8B and the flux of 8B neutrinos from the Sun NUCLEAR REACTIONS Pb(8B, p7Be), E=83 MeV/nucleon; measured σ. 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled-channels analysis.
doi: 10.1140/epja/i2001-10227-7
2002DA29 Prog.Theor.Phys.(Kyoto), Suppl. 146, 358 (2002) New Theoretical Results on the Proton Decay of Deformed and Near-Spherical Nuclei RADIOACTIVITY 131Eu, 141,141mHo(p); calculated proton decay widths. 144Er, 145Tm, 177Tl(p); analyzed proton decay data; deduced role of particle-vibration coupling.
doi: 10.1143/PTPS.146.358
2002ES01 Phys.Rev. C65, 024605 (2002) Multipole Expansion for Relativistic Coulomb Excitation
doi: 10.1103/PhysRevC.65.024605
2002ES07 Nucl.Phys. A706, 383 (2002) Higher-Order Effects in the Two-Body Breakup of 17F NUCLEAR REACTIONS 58Ni, 208Pb(17F, p16O), E=10, 40 MeV/nucleon; calculated stripping, dissociation probabilities vs impact parameter. Both ground and excited state of projectile considered.
doi: 10.1016/S0375-9474(02)00869-2
2002ES11 Phys.Rev. C66, 044609 (2002) Dynamic polarization in the Coulomb dissociation of 8B NUCLEAR REACTIONS 58Ni(8B, p7Be), E=3-20 MeV/nucleon; calculated σ(θ), dynamic polarization effects. Comparison with data.
doi: 10.1103/PhysRevC.66.044609
2002JI04 Phys.Rev.Lett. 89, 052701 (2002); Comment Phys.Rev.Lett. 91, 229201 (2003) C.L.Jiang, H.Esbensen, K.E.Rehm, B.B.Back, R.V.F.Janssens, J.A.Caggiano, P.Collon, J.Greene, A.M.Heinz, D.J.Henderson, I.Nishinaka, T.O.Pennington, D.Seweryniak Unexpected Behavior of Heavy-Ion Fusion Cross Sections at Extreme Sub-Barrier Energies NUCLEAR REACTIONS 89Y(60Ni, X), E=122-136 MeV; measured fusion-evaporation σ; deduced discrepancy with model prediction at low energy. Comparison with previous results from other systems.
doi: 10.1103/PhysRevLett.89.052701
2002LI34 Phys.Rev. C65, 051603 (2002) J.F.Liang, J.R.Beene, H.Esbensen, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, P.E.Mueller, D.Shapira, D.W.Stracener, I.J.Thompson, R.L.Varner Elastic Scattering and Breakup of 17F at 10 MeV/nucleon NUCLEAR REACTIONS 208Pb(17F, 17F), (17F, 16O), E=170 MeV; measured σ(θ); deduced reaction mechanism features. Comparison with optical model predictions.
doi: 10.1103/PhysRevC.65.051603
2002VO14 Phys.Rev. C66, 044604 (2002) Role of E1-E2 interplay in multiphonon Coulomb excitation
doi: 10.1103/PhysRevC.66.044604
2001DA03 Phys.Rev.Lett. 86, 2750 (2001) B.Davids, D.W.Anthony, T.Aumann, S.M.Austin, T.Baumann, D.Bazin, R.R.C.Clement, C.N.Davids, H.Esbensen, P.A.Lofy, T.Nakamura, B.M.Sherrill, J.Yurkon S17(0) Determined from the Coulomb Breakup of 83 MeV/Nucleon 8B NUCLEAR REACTIONS Pb(8B, p7Be), E=83 MeV/nucleon; measured particle spectra, σ(E, θ). 7Be(p, γ), E=low; deduced astrophysical S-factor. Kinematically complete measurement, first-order perturbation theory analysis.
doi: 10.1103/PhysRevLett.86.2750
2001DA11 Phys.Rev. C63, 065806 (2001) B.Davids, S.M.Austin, D.Bazin, H.Esbensen, B.M.Sherrill, I.J.Thompson, J.A.Tostevin Electromagnetic Dissociation of 8B and the Rate of the 7Be(p, γ)8B Reaction in the Sun NUCLEAR REACTIONS Ag, Pb(8B, p7Be), E=44, 81, 83 MeV/nucleon; measured fragment spectra, longitudinal momentum distributions; deduced Coulomb dissociation σ. 7Be(p, γ), E=low; deduced astrophysical S-factor. Exclusive and inclusive measurements.
doi: 10.1103/PhysRevC.63.065806
2001DA18 Phys.Rev. C64, 034317 (2001) Particle-Vibration Coupling in Proton Decay of Near-Spherical Nuclei NUCLEAR STRUCTURE 145,147,147mTm, 151,151mLu, 161,161mRe, 165,167,167mIr, 171,171mAu, 177,177mTl; calculated proton decay widths, spectroscopic factors; deduced role of particle-vibration coupling.
doi: 10.1103/PhysRevC.64.034317
2001ES01 Phys.Rev. C63, 014315 (2001) Coupled-Channels Treatment of Deformed Proton Emitters RADIOACTIVITY 131Eu, 141Ho(p); calculated proton decay partial widths; deduced role of Coriolis mixing. Coupled-channels approach.
doi: 10.1103/PhysRevC.63.014315
2001ES05 Phys.Rev. C64, 014608 (2001) Eikonal Approximation in Heavy-Ion Fragmentation Reactions NUCLEAR REACTIONS 12C(11Be, X), E=0-100 MeV/nucleon; 208Pb(11Be, X), E=20 MeV/nucleon; calculated breakup probabilities, momentum and angular distributions. Eikonal approximation, comparison with full calculation.
doi: 10.1103/PhysRevC.64.014608
2001SA57 Nucl.Phys. A693, 448 (2001) Giant Resonances in Exotic Nuclei NUCLEAR REACTIONS 8B(208Pb, X)7Be, E=44, 46.5 MeV/nucleon; calculated decay energy spectrum and logitudinal momentum distributions following Coulomb dissociation. Comparison with data. NUCLEAR STRUCTURE 34,40,48,60Ca, 208Pb; calculated quadrupole, isovector and isoscalar strengths distributions, giant resonances. Random Phase Approximation.
doi: 10.1016/S0375-9474(01)00649-2
2000AH03 Phys.Rev. C61, 051304 (2000) I.Ahmad, R.W.Dunford, H.Esbensen, D.S.Gemmell, E.P.Kanter, U.Rutt, S.H.Southworth Nuclear Excitation by Electronic Transition in 189Os NUCLEAR REACTIONS 189Os(X-ray, X), E=69.47-69.97 keV; measured isomer yield; deduced probability for nuclear excitation by electronic transition. RADIOACTIVITY 189mOs(IT); measured T1/2.
doi: 10.1103/PhysRevC.61.051304
2000DA11 Phys.Rev. C61, 054302 (2000) Decay Rates of Spherical and Deformed Proton Emitters RADIOACTIVITY 131Eu, 141Ho, 147mTm, 167,167mIr(p); calculated T1/2. Comparison of direct, distorted wave methods.
doi: 10.1103/PhysRevC.61.054302
2000ES03 Phys.Rev. C61, 054606 (2000) Systematic Study of 8B Breakup Cross Sections NUCLEAR REACTIONS C, 27Al, Si, Sn, Pb(7Be, X), E=20-2000 MeV/nucleon; calculated breakup σ. C, 27Al, Si, Sn, Pb(8B, X), E=20-2000 MeV/nucleon; calculated breakup, one-proton removal σ, fragment momentum distributions. Two-body structure model, comparisons with data.
doi: 10.1103/PhysRevC.61.054606
2000LI38 Phys.Lett. 491B, 23 (2000) J.F.Liang, J.R.Beene, H.Esbensen, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, P.E.Mueller, D.Shapira, D.W.Stracener, R.L.Varner Breakup of Weakly Bound 17F Well Above the Coulomb Barrier NUCLEAR REACTIONS 208Pb(17F, p16O), E=170 MeV; measured σ, fragments angular correlations, proton spectra; deduced breakup mechanism. Comparison with model predictions.
doi: 10.1016/S0370-2693(00)01016-9
1999ES04 Phys.Rev. C59, 3240 (1999) Nuclear Induced Breakup of Halo Nuclei NUCLEAR REACTIONS 58Ni(8B, p7Be), E=26 MeV; calculated σ(θ); deduced role of continuum-continuum coupling.
doi: 10.1103/PhysRevC.59.3240
1999HE43 Nucl.Phys. (Supplement) A654, 669c (1999) K.Hencken, G.Bertsch, H.Esbensen The Nuclear Breakup of Halo Nuclei Through Diffraction and Stripping NUCLEAR REACTIONS C, Pb(6He, X), (11Li, X), E not given; calculated diffraction, 1-neutron and 2-neutron stripping, 2-neutron removal σ. Comparison with data. Serber model.
doi: 10.1016/S0375-9474(00)88523-1
1998BA48 Phys.Rev. C58, 1257 (1998) F.Barranco, R.A.Broglia, H.Esbensen, E.Vigezzi Semiclassical Approximation to Neutron Star Superfluidity Corrected for Proximity Effects
doi: 10.1103/PhysRevC.58.1257
1998BE09 Phys.Rev. C57, 1366 (1998) G.F.Bertsch, K.Hencken, H.Esbensen Nuclear Breakup of Borromean Nuclei NUCLEAR REACTIONS 12C(11Li, X), E=800 MeV/nucleon; 12C(6He, X), E=240, 800 MeV/nucleon; calculated projectile breakup channels σ; deduced neutron halo structure dependence. Eikonal theory. Comparisons with data.
doi: 10.1103/PhysRevC.57.1366
1998DA14 Phys.Rev.Lett. 81, 2209 (1998) B.Davids, D.W.Anthony, S.M.Austin, D.Bazin, B.Blank, J.A.Caggiano, M.Chartier, H.Esbensen, P.Hui, C.F.Powell, H.Scheit, B.M.Sherrill, M.Steiner, P.Thirolf, J.Yurkon, A.Zeller Measurement of E2 Transitions in the Coulomb Dissociation of 8B NUCLEAR REACTIONS 208Pb(8B, p7Be), E=44, 81 MeV/nucleon; measured fragments longitudinal momentum distributions; deduced relative E2 transition strength.
doi: 10.1103/PhysRevLett.81.2209
1998ES04 Phys.Rev. C57, 2401 (1998) H.Esbensen, C.L.Jiang, K.E.Rehm Coupled-Channels Analysis of 58Ni + 124Sn Reactions NUCLEAR REACTIONS 58Ni(124Sn, X)58Ni/59Ni/60Ni/61Ni/62Ni/63Ni/64Ni/65Ni, E(cm)=150-240 MeV; analyzed σ(θ), σ; deduced subbarrier capture enhancement. Coupled channels calculations.
doi: 10.1103/PhysRevC.57.2401
1998JI04 Phys.Rev. C57, 2393 (1998) C.L.Jiang, K.E.Rehm, H.Esbensen, D.J.Blumenthal, B.Crowell, J.Gehring, B.Glagola, J.P.Schiffer, A.H.Wuosmaa Multineutron Transfer in 58Ni + 124Sn Collisions at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 58Ni(124Sn, X)58Ni/59Ni/60Ni/61Ni/62Ni/63Ni/64Ni/65Ni/57Co/56Fe, E=480-512 MeV; measured σ(θ), σ; deduced neutron transfer probabilities, Q-values.
doi: 10.1103/PhysRevC.57.2393
1998RE18 Phys.Rev.Lett. 81, 3341 (1998) K.E.Rehm, H.Esbensen, C.L.Jiang, B.B.Back, F.Borasi, B.Harss, R.V.F.Janssens, V.Nanal, J.Nolen, R.C.Pardo, M.Paul, P.Reiter, R.E.Segel, A.Sonzogni, J.Uusitalo, A.H.Wuosmaa Fusion Cross Sections for the Proton Drip Line Nucleus 17F at Energies Below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(17F, X), E(cm)=80-92 MeV; 208Pb(19F, X), E(cm)=78-100 MeV; measured fusion-fission σ; deduced no enhancement for lighter projectile. Dynamical model calculations.
doi: 10.1103/PhysRevLett.81.3341
1997BA09 Phys.Lett. 390B, 13 (1997) F.Barranco, R.A.Broglia, H.Esbensen, E.Vigezzi Role of Finite Nuclei on the Pairing Gap of the Inner Crust of Neutron Stars
doi: 10.1016/S0370-2693(96)01373-1
1997ES07 Phys.Rev. C56, 3054 (1997) H.Esbensen, G.F.Bertsch, K.Hencken Application of Contact Interactions to Borromean Halos NUCLEAR STRUCTURE 6He, 11Li; calculated two-neutron separation, halo radius. Three-body calculations, density-dependent interaction, comparison with Fadeev approach.
doi: 10.1103/PhysRevC.56.3054
1996ES01 Phys.Rev. C53, 2007 (1996) Momentum Distributions in Stripping Reactions of Single-Nucleon Halo Nuclei NUCLEAR REACTIONS 9Be(11Be, 10Be), E=63 MeV/nucleon. C(8B, 7Be), E=82-91 MeV/nucleon; analyzed ejectile longitudinal momentum distributions. Single-particle approach.
doi: 10.1103/PhysRevC.53.2007
1996ES02 Nucl.Phys. A600, 37 (1996) Effects of E2 Transitions in the Coulomb Dissociation of 8B NUCLEAR REACTIONS, ICPND Pb(8B, X), E=46.5 MeV/nucleon; calculated projectile Coulomb dissociation probabilities vs impact parameter, (7Be+p) system relative kinetic energy, σ(θp) following breakup, fragment momenta. 7Be(p, γ), E not given; calculated astrophysical S-factor vs E(relative); deduced E1, E2 amplitudes interference related asymmetry, constraints determination.
doi: 10.1016/0375-9474(96)00006-1
1996ES07 Phys.Rev. C54, 3109 (1996) Coupled Channels Analysis of High Precision Fusion Data NUCLEAR REACTIONS 144Sm(16O, 16O), (16O, 16O'), E ≈ 55-77.5 MeV; analyzed elastic, quasielastic, inelastic σ(θ); deduced higher-order couplings role. High precision fusion data, coupled-channels treatment.
doi: 10.1103/PhysRevC.54.3109
1996HE23 Phys.Rev. C54, 3043 (1996) K.Hencken, G.Bertsch, H.Esbensen Breakup Reactions of the Halo Nuclei 11Be and 8B NUCLEAR REACTIONS 9Be(11Be, n10Be), E=66 MeV/nucleon; 12C(8B, p7Be), E=1470 MeV/nucleon; analyzed heavier ejectile transverse momentum distribution. Eikonal approximation, realistic optical potential based profile function. NUCLEAR STRUCTURE A ≈ 10-200; calculated breakup σ for 11Be projectile with E=40, 800 MeV/nucleon. Eikonal approximation, realistic optical potential based profile function.
doi: 10.1103/PhysRevC.54.3043
1996KE16 Phys.Rev.Lett. 77, 5020 (1996) J.H.Kelley, S.M.Austin, A.Azhari, D.Bazin, J.A.Brown, H.Esbensen, M.Fauerbach, M.Hellstrom, S.E.Hirzebruch, R.A.Kryger, D.J.Morrissey, R.Pfaff, C.F.Powell, E.Ramakrishnan, B.M.Sherrill, M.Steiner, T.Suomijarvi, M.Thoennessen Study of the Breakup Reaction 8B → 7Be + p: Absorption effects and E2 strength NUCLEAR REACTIONS 9Be, 197Au(8B, p7Be), E=41 MeV/nucleon; measured parallel, transverse momenta. Models comparison.
doi: 10.1103/PhysRevLett.77.5020
1996WA27 Phys.Rev. C54, 1700 (1996) R.E.Warner, R.A.Patty, P.M.Voyles, A.Nadasen, F.D.Becchetti, J.A.Brown, H.Esbensen, A.Galonsky, J.J.Kolata, J.Kruse, M.Y.Lee, R.M.Ronningen, P.Schwandt, J.von Schwarzenberg, B.M.Sherrill, K.Subotic, J.Wang, P.Zecher Total Reaction and 2n-Removal Cross Sections of 20-60A MeV 4,6,8He, 6-9,11Li, and 10Be on Si NUCLEAR REACTIONS, ICPND Si(6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (10Be, X), (α, X), (6He, X), (8He, X), E=20-60 MeV/nucleon; measured reaction σ, 2n-removal σ for some projectiles. 4,6,8He, 6,7,8,9,11Li, 10Be deduced matter distributions. Microscopic, strong absorption optical models.
doi: 10.1103/PhysRevC.54.1700
1995ES01 Nucl.Phys. A581, 107 (1995) H.Esbensen, G.F.Bertsch, C.A.Bertulani Higher-Order Dynamical Effects in Coulomb Dissociation NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; Pb(11Be, X), E=72 MeV/nucleon; calculated projectile dissociation spectra; deduced higher order processes role in Coulomb dissociation. Time-dependent 3D-Schrodinger equation, 9Li+dineutron.
doi: 10.1016/0375-9474(94)00423-K
1995ES02 Phys.Rev. C51, 1274 (1995) H.Esbensen, B.A.Brown, H.Sagawa Positive Parity States in 11Be NUCLEAR STRUCTURE 11Be, 13C; calculated levels. Coupled-channels approach, deformed core+valence nucleon.
doi: 10.1103/PhysRevC.51.1274
1995ES06 Phys.Lett. 359B, 13 (1995) Interference Effects in the Coulomb Dissociation of 8B NUCLEAR STRUCTURE 8B; calculated Coulomb breakup into 7Be+p, E1, E2 interference on σ(θp).
doi: 10.1016/0370-2693(95)01067-Z
1993AN05 Phys.Lett. 304B, 55 (1993) R.Anne, S.E.Arnell, R.Bimbot, S.Dogny, H.Emling, H.Esbensen, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, F.Humbert, B.Jonson, M.Keim, M.Lewitowicz, P.Moller, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, K.Riisager, M.-G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen Rolander, D.Wolski Dissociation Reactions of the 11Be One-Neutron Halo. The Interplay between Structure and Reaction Mechanism NUCLEAR REACTIONS 197Au, Ti, 9Be(11Be, X), E=41 MeV/nucleon; measured exclusive, inclusive σ(θ); deduced structure, reaction mechanism interplay.
doi: 10.1016/0370-2693(93)91399-8
1993ES02 Phys.Rev. C48, 326 (1993) H.Esbensen, G.F.Bertsch, K.Ieki Momentum Distributions for (11Li, 9Li + n + n) Breakup Reactions NUCLEAR REACTIONS Pb(11Li, 9Li), E=28 MeV/nucleon; Ta(11Li, 9Li), E=66 MeV/nucleon; analyzed target Coulomb field induced projectile breakup data. Three-body model for 11Li.
doi: 10.1103/PhysRevC.48.326
1993RE11 Phys.Lett. 317B, 31 (1993) K.E.Rehm, H.Esbensen, J.Gehring, B.Glagola, D.Henderson, W.Kutschera, M.Paul, F.Soramel, A.H.Wuosmaa Sub-Barrier Fusion Cross Sections in 58,62Ni + 92,100Mo Studied with the Gas-Filled Magnet Technique NUCLEAR REACTIONS, ICPND 92,100Mo(58Ni, X), (64Ni, X), E(cm) ≈ 130-160 MeV; measured fusion σ(E), σ(evaporation residue, θ). Gas filled magnet technique for product separation. Coupled-channels model.
doi: 10.1016/0370-2693(93)91565-5
1993SA20 Phys.Lett. 309B, 1 (1993) H.Sagawa, B.A.Brown, H.Esbensen Parity inversion in the N = 7 Isotones and the Pairing Blocking Effect NUCLEAR STRUCTURE 11Be, 13C, 15O; calculated Hartree-Fock single particle energies. 11Be deduced parity inversion possible mechanism. Shell model, Hartree-Fock model.
doi: 10.1016/0370-2693(93)91493-7
1993SA21 Phys.Rev. C48, 118 (1993) D.Sackett, K.Ieki, A.Galonsky, C.A.Bertulani, H.Esbensen, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, H.Schulz, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Electromagnetic Excitation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured 9Li(n)-, γ(9Li)-coin following 11Li Coulomb dissociation; deduced dissociation σ, photonuclear σ(E1), breakup mechanism.
doi: 10.1103/PhysRevC.48.118
1992ES01 Nucl.Phys. A542, 310 (1992) Soft Dipole Excitations in 11Li NUCLEAR STRUCTURE 11Li; calculated valence nucleon dipole response contours. Three-body model. NUCLEAR REACTIONS 197Au(11Li, 9Li), E ≤ 1 GeV/nucleon; calculated Coulomb dissociation σ. 197Au(11Li, 9Li), E=70 MeV/nucleon; calculated ejectile longitudinal recoil momentum distribution. Valence nucleon correlated dipole response.
doi: 10.1016/0375-9474(92)90219-A
1992ES02 Phys.Lett. 287B, 289 (1992) H.Esbensen, D.Kurath, T.-S.H.Lee Correlation Effects in 11B(π-, π+)11Li Reactions NUCLEAR REACTIONS 11B(π-, π+), E=164 MeV; calculated σ(θ); deduced 11Li valence neutrons spatial correlations role.
doi: 10.1016/0370-2693(92)90984-C
1992ES03 Phys.Rev. C46, 1552 (1992) Fragmentation Reactions of 11Li NUCLEAR STRUCTURE A=10-200; calculated (11Li, 9Li) reaction σ, E=800 MeV/nucleon; deduced projectile valence nucleon space correlation role.
doi: 10.1103/PhysRevC.46.1552
1992FR08 Phys.Rev. C45, 2500 (1992) S.H.Fricke, H.Esbensen, S.Landowne Elastic Scattering and Fusion Calculations for 16O + 63,65Cu NUCLEAR REACTIONS, ICPND 63,65Cu(16O, X), E(cm) ≈ 30-70 MeV; calculated fusion σ(E). 63,65Cu(16O, 16O), E=46 MeV; calculated σ(θ). Coupled-channels method.
doi: 10.1103/PhysRevC.45.2500
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