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NSR database version of March 21, 2024.

Search: Author = H.Esbensen

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0904.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0848.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0774.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0772.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2117.


2014ES01      Phys.Rev. C 89, 044616 (2014)

H.Esbensen, A.M.Stefanini

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0741.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0750.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0801.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0719.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2044.


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
Citations: PlumX Metrics


2012ES04      Phys.Rev. C 85, 064611 (2012)

H.Esbensen

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0758.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1785.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1785.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1831.


2011ES08      Phys.Rev. C 84, 064613 (2011)

H.Esbensen, X.Tang, C.L.Jiang

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010ES03      Phys.Rev. C 81, 034606 (2010)

H.Esbensen

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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1781.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0759.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1704.


2009ES01      Phys.Rev. C 79, 064619 (2009)

H.Esbensen, C.L.Jiang

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
Citations: PlumX Metrics


2009ES02      Phys.Rev. C 80, 024608 (2009); Erratum, Phys.Rev. C 80, 059904 (2009)

H.Esbensen

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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1803.


2008ES03      Phys.Rev. C 77, 054608 (2008)

H.Esbensen

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
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2008ES04      Phys.Rev. C 78, 024608 (2008)

H.Esbensen

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
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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
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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
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2007ES08      Phys.Rev. C 76, 054609 (2007)

H.Esbensen, S.Misicu

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
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2007MI06      Phys.Rev. C 75, 034606 (2007)

S.Misicu, H.Esbensen

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
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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
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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
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2006MI09      Phys.Rev.Lett. 96, 112701 (2006)

S.Misicu, H.Esbensen

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
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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
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2005ES12      Phys.Rev. C 72, 054607 (2005)

H.Esbensen

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
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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
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2004DA10      Phys.Rev. C 69, 034314 (2004)

C.N.Davids, H.Esbensen

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
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2004ES03      Prog.Theor.Phys.(Kyoto), Suppl. 154, 11 (2004)

H.Esbensen

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
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2004ES05      Phys.Rev. C 70, 047603 (2004)

H.Esbensen

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
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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
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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
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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
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2003ES07      Phys.Rev. C 68, 034604 (2003)

H.Esbensen

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1484.


2002BF01      Prog.Theor.Phys.(Kyoto), Suppl. 146, 319 (2002)

G.F.Bertsch, H.Esbensen

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
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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
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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
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2002DA29      Prog.Theor.Phys.(Kyoto), Suppl. 146, 358 (2002)

C.N.Davids, H.Esbensen

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
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2002ES01      Phys.Rev. C65, 024605 (2002)

H.Esbensen, C.A.Bertulani

Multipole Expansion for Relativistic Coulomb Excitation

doi: 10.1103/PhysRevC.65.024605
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2002ES07      Nucl.Phys. A706, 383 (2002)

H.Esbensen, G.F.Bertsch

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
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2002ES11      Phys.Rev. C66, 044609 (2002)

H.Esbensen, G.F.Bertsch

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0889.


2002VO14      Phys.Rev. C66, 044604 (2002)

A.Volya, H.Esbensen

Role of E1-E2 interplay in multiphonon Coulomb excitation

doi: 10.1103/PhysRevC.66.044604
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0820.


2001DA18      Phys.Rev. C64, 034317 (2001)

C.N.Davids, H.Esbensen

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
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2001ES01      Phys.Rev. C63, 014315 (2001)

H.Esbensen, C.N.Davids

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
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2001ES05      Phys.Rev. C64, 014608 (2001)

H.Esbensen, G.F.Bertsch

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
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2001SA57      Nucl.Phys. A693, 448 (2001)

H.Sagawa, H.Esbensen

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
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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
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2000DA11      Phys.Rev. C61, 054302 (2000)

C.N.Davids, H.Esbensen

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
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2000ES03      Phys.Rev. C61, 054606 (2000)

H.Esbensen, K.Hencken

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
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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
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1999ES04      Phys.Rev. C59, 3240 (1999)

H.Esbensen, G.F.Bertsch

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1996ES01      Phys.Rev. C53, 2007 (1996)

H.Esbensen

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
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1996ES02      Nucl.Phys. A600, 37 (1996)

H.Esbensen, G.F.Bertsch

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
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1996ES07      Phys.Rev. C54, 3109 (1996)

H.Esbensen, B.B.Back

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0919.


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
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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
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1995ES06      Phys.Lett. 359B, 13 (1995)

H.Esbensen, G.F.Bertsch

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1327.


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
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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
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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
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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
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1992ES01      Nucl.Phys. A542, 310 (1992)

H.Esbensen, G.F.Bertsch

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
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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
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1992ES03      Phys.Rev. C46, 1552 (1992)

H.Esbensen, G.F.Bertsch

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
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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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