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NSR database version of April 11, 2024.

Search: Author = M.Hjorth-Jensen

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2023FO02      Phys. Rev. Res. 5, 033062 (2023)

B.Fore, J.M.Kim, G.Carleo, M.Hjorth-Jensen, A.Lovato, M.Piarulli

Dilute neutron star matter from neural-network quantum states

doi: 10.1103/PhysRevResearch.5.033062
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2023MR01      Phys.Rev. C 107, 054911 (2023)

D.Mroczek, M.Hjorth-Jensen, J.Noronha-Hostler, P.Parotto, C.Ratti, R.Vilalta

Mapping out the thermodynamic stability of a QCD equation of state with a critical point using active learning

doi: 10.1103/PhysRevC.107.054911
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2022BO15      Rev.Mod.Phys. 94, 031003 (2022)

A.Boehnlein, M.Diefenthaler, N.Sato, M.Schram, V.Ziegler, C.Fanelli, M.Hjorth-Jensen, T.Horn, M.P.Kuchera, D.Lee, W.Nazarewicz, P.Ostroumov, K.Orginos, A.Poon, X.-N.Wang, A.Scheinker, M.S.Smith, L.-G.Pang

Colloquium: Machine learning in nuclear physics

doi: 10.1103/RevModPhys.94.031003
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2021LE13      Phys.Rev.Lett. 127, 062501 (2021)

D.Lee, S.Bogner, B.A.Brown, S.Elhatisari, E.Epelbaum, H.Hergert, M.Hjorth-Jensen, H.Krebs, N.Li, B.-N.Lu, U.-G.Meissner

Hidden Spin-Isospin Exchange Symmetry

doi: 10.1103/PhysRevLett.127.062501
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2021RH01      Phys.Rev. C 103, L051301 (2021)

D.Rhodes, B.A.Brown, J.Henderson, A.Gade, J.Ash, P.C.Bender, R.Elder, B.Elman, M.Grinder, M.Hjorth-Jensen, H.Iwasaki, B.Longfellow, T.Mijatovic, M.Spieker, D.Weisshaar, C.Y.Wu

Exploring the role of high-j configurations in collective observables through the Coulomb excitation of 106Cd

NUCLEAR REACTIONS 208Pb(106Cd, 106Cd'), E=4.03, 4.36 MeV/nucleon; 48Ti(106Cd, 106Cd'), E=3 MeV/nucleon; measured scattered 106Cd and recoil 208Pb, Eγ, Iγ, (particle)γ-coin, angular distributions, γ-ray yields using the JANUS array of two annular Si detectors and SeGA array of sixteen 32-fold segmented HPGe detectors at NSCL-MSU Re-accelerator facility. 106Cd; deduced levels, J, π, E2, M1 and E3 transition matrix elements, B(E2), level half-lives, spectroscopic quadrupole moments, ground-state rotational invariants and quadrupole moments, analysis using GOSIA and GOSIA2 least-squares fitting codes. Comparison with results of previous measurements and with shell-model calculations.

doi: 10.1103/PhysRevC.103.L051301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2019TO10      Eur.Phys.J. A 55, 158 (2019)

D.A.Torres, R.Chapman, V.Kumar, B.Hadinia, A.Hodsdon, M.Labiche, X.Liang, D.O'Donnell, J.Ollier, R.Orlandi, J.F.Smith, K.-M.Spohr, P.Wady, Z.M.Wang, L.Corradi, E.Fioretto, A.Gadea, G.de Angelis, N.Marginean, D.R.Napoli, E.Sahin, A.M.Stefanini, J.J.Valiente-Dobon, F.D.Vedova, M.Axiotis, T.Martinez, S.Szilner, D.Bazzacco, S.Beghini, E.Farnea, R.Marginean, D.Mengoni, G.Montagnoli, F.Recchia, F.Scarlassara, C.A.Ur, S.M.Lenzi, S.Lunardi, T.Kroll, F.Haas, T.Faul, M.Hjorth-Jensen, B.G.Carlsson, S.J.Freeman, A.G.Smith, G.Jones, N.Thompson, G.Pollarolo, G.S.Simpson

Study of medium-spin states of neutron-rich 87, 89, 91Rb isotopes

NUCLEAR REACTIONS 124Sn(96Zr, f), (96Zr, x)87,89,91Rb, E=530 MeV; measured Eγ, Iγ of fission fragments γ-ray decay; 176Yb(36S, x), (36S, f)87,89,91Rb, E=230 MeV; measured thick target Eγ, Iγ of fission fragments γ-ray decay. 87,89,91Rb; deduced γ-ray energy spectrum, new scheme of levels, Jπ, (up to 6423 keV (27/2)+ state), γ-ray transitions; calculated multipolarities, energy differences between (5/2)- and (3/2)- states for odd-A Rb isotopes using spherical shell-model and cranked Nilsson-Strutinsky-Bogoliubov approach.

doi: 10.1140/epja/i2019-12839-6
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2017EL04      Phys.Rev. C 96, 044332 (2017)

B.Elman, A.Gade, D.Weisshaar, D.Barofsky, D.Bazin, P.C.Bender, M.Bowry, M.Hjorth-Jensen, K.W.Kemper, S.Lipschutz, E.Lunderberg, N.Sachmpazidi, N.Terpstra, W.B.Walters, A.Westerberg, S.J.Williams, K.Wimmer

Quadrupole collectivity beyond N = 50 in neutron-rich Se and Kr isotopes

NUCLEAR REACTIONS 209Bi(88Kr, 88Kr'), E=67 MeV/nucleon; 209Bi(90Kr, 90Kr'), E=68 MeV/nucleon; 209Bi(86Se, 86Se'), E=79 MeV/nucleon, [secondary 88,90Kr, 86Se beams from 9Be(96Zr, X), E=120 MeV/nucleon using A1900 fragment separator at the NSCL-MSU Cyclotron Laboratory]; measured reaction products and particle identification plot, Doppler-corrected Eγ, Iγ, (particle)γ-coin, σ, using the CAESAR array of 192 CsI(Na) scintillators. 88,90Kr, 86Se; deduced levels, J, π, Coulomb excitation yields, B(E2) for excited 2+ states. Comparison with shell-model calculations. 88,90Kr, 86Se; calculated shell-model occupations of the proton and neutron orbitals for the observed levels. Systematics of B(E2) values for the first 2+ states in N=36-60 Kr and Se nuclei.

doi: 10.1103/PhysRevC.96.044332
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2017OR02      Phys.Rev. C 96, 024323 (2017)

W.E.Ormand, B.A.Brown, M.Hjorth-Jensen

Realistic calculations for c coefficients of the isobaric mass multiplet equation in 1p0f shell nuclei

NUCLEAR STRUCTURE A=42, 46, 50, 54; calculated c coefficients of the isobaric mass multiplet equation (IMME) for nuclei in A=42 to 54 based on input from three realistic nucleon-nucleon interactions (CD-Bonn, AV18 and N3LO); deduced dependence on the short-range charge-symmetry-breaking (CSB) part of the strong interaction, disagreement in the CSB part between the commonly used CD-Bonn, chiral effective field theory at next-to-next-to-next-to-leading-order, and Argonne V18 nucleon-nucleon interactions, and CSB contribution to the c coefficient from all three interactions too large as compared to the experimental data.

doi: 10.1103/PhysRevC.96.024323
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2017TS01      Phys.Rev. C 95, 021304 (2017)

N.Tsunoda, T.Otsuka, N.Shimizu, M.Hjorth-Jensen, K.Takayanagi, T.Suzuki

Exotic neutron-rich medium-mass nuclei with realistic nuclear forces

NUCLEAR STRUCTURE 20,22,24,26,28,30,32Ne, 24,26,28,30,32,34Mg, 28,30,32,34,36Si; calculated energies of the first 2+ and 4+ states, B(E2), expectation values of the number of the particle-hole excitations in the ground states of Mg isotopes. 31,32Mg; calculated levels, J, π. 28O, 30Ne, 32Mg, 34Si, 36S, 38Ar, 40Ca; calculated effective neutron single-particle energies (ESPEs) of N=20 isotones. Extended Kuo-Krenciglowa (EKK) theory of effective nucleon-nucleon interaction for exotic nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.021304
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2016HA27      Nat.Phys. 12, 186 (2016)

G.Hagen, A.Ekstrom, C.Forssen, G.R.Jansen, W.Nazarewicz, T.Papenbrock, K.A.Wendt, S.Bacca, N.Barnea, B.Carlsson, C.Drischler, K.Hebeler, M.Hjorth-Jensen, M.Miorelli, G.Orlandini, A.Schwenk, J.Simonis

Neutron and weak-charge distributions of the 48Ca nucleus

NUCLEAR STRUCTURE 48Ca; calculated neutron skin parameters, radii. Ab initio calculations.

doi: 10.1038/nphys3529
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2016HA34      Phys.Scr. 91, 063006 (2016)

G.Hagen, M.Hjorth-Jensen, G.R.Jansen, T.Papenbrock

Emergent properties of nuclei from ab initio coupled-cluster calculations

COMPILATION 4,8He, 14C, 16O, 40,48Ca, 56Ni; compiled gs energy, mass excess, difference between theoretical charge radii and data; calculated gs energy, mass excess, charge radii using ab initio approach with chiral NNLOsat interaction.

NUCLEAR STRUCTURE 16,22,24,28O; calculated gs energy, mass excess using two NNLOsat interactions. Compared to available data. 17,23,25O, 53,55,61Ca; calculated low-lying unbound levels, J, π using harmonic oscillator HF basis and Gamow-Hartree-Fock basis. 20Ne, 24Mg; calculated yrast states using CCEI (Coupled Cluster Effective Interaction) and USDB; compared to data.

doi: 10.1088/0031-8949/91/6/063006
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2015EK01      Phys.Rev. C 91, 051301 (2015)

A.Ekstrom, G.R.Jansen, K.A.Wendt, G.Hagen, T.Papenbrock, B.D.Carlsson, C.Forssen, M.Hjorth-Jensen, P.Navratil, W.Nazarewicz

Accurate nuclear radii and binding energies from a chiral interaction

NUCLEAR STRUCTURE 2H, 4,8He, 6,9Li, 14C, 16O, 40Ca; calculated ground-state energies, charge radii, quadrupole moment for deuteron. 6Li, 14C, 16O, 22,24F, 22,24O, 40Ca; calculated levels, J, π, charge density in 16O, scattering lengths, and effective ranges in low-energy proton-proton scattering, scattering phase shifts in low-energy neutron-proton scattering, half-life for the β- decay of 3H; deduced consistently optimized interaction from chiral EFT at NNLO for nuclei and infinite nuclear matter. Coupled-cluster calculations based on chiral effective field theory interaction (NNLOsat). Comparison with experimental data.

doi: 10.1103/PhysRevC.91.051301
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2014EN03      Nucl.Phys. A928, 51 (2014)

T.Engeland, M.Hjorth-Jensen, M.Kartamyshev, E.Osnes

The Kuo-Brown effective interaction: From 18O to the Sn isotopes

NUCLEAR STRUCTURE 102,104,106,108,110,112,114,116Sn; calculated binding energy, mass excess, lowest 2+, 4+-state energy, B(E2). 101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131Sn; calculated single-particle levels, J, π. Large-scale shell model with different nucleon-nucleon potentials and effective interaction from G-matrix and Vlovk interactions. Compared with available data.

doi: 10.1016/j.nuclphysa.2014.03.012
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2014HA01      Phys.Rev. C 89, 014319 (2014)

G.Hagen, T.Papenbrock, A.Ekstrom, K.A.Wendt, G.Baardsen, S.Gandolfi, M.Hjorth-Jensen, C.J.Horowitz

Coupled-cluster calculations of nucleonic matter

NUCLEAR STRUCTURE A=10-1000; N=66, 132; calculated relative finite-size corrections for the kinetic energy in pure neutron matter, E/A of nuclear and neutron matter. Coupled-cluster computations of equation of state (EoS) for symmetric nuclear matter and neutron matter using optimized nucleon-nucleon (NN) potential NNLOopt at next-to-next-to leading order. Comparison with benchmark calculations.

doi: 10.1103/PhysRevC.89.014319
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2014SA46      Phys.Lett. B 736, 137 (2014)

A.Sanetullaev, M.B.Tsang, W.G.Lynch, Jenny Lee, D.Bazin, K.P.Chan, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, A.M.Rogers, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, D.Shapira, W.A.Peters, C.Barbieri, M.Hjorth-Jensen, M.Horoi, T.Otsuka, T.Suzuki, Y.Utsuno

Neutron spectroscopic factors of 55Ni hole-states from image transfer reactions

NUCLEAR REACTIONS 1H(56Ni, d), E=37 MeV/nucleon; measured reaction products; deduced spectroscopic factors, J, π, σ(θ). Comparison with shell model calculations.

doi: 10.1016/j.physletb.2014.07.003
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2132. Data from this article have been entered in the XUNDL database. For more information, click here.


2014TS01      Phys.Rev. C 89, 024313 (2014)

N.Tsunoda, K.Takayanagi, M.Hjorth-Jensen, T.Otsuka

Multi-shell effective interactions

NUCLEAR STRUCTURE 18O, 18F, 42Ca, 42Sc; calculated nucleon-nucleon effective interaction for shell-model calculations for degenerate and nondegenerate model spaces. 42Ca, 42Sc; calculated levels, J, π, two-body matrix elements. Kuo-Krenciglowa (KK) and extended KK (EKK) methods. Comparison with experimental values.

doi: 10.1103/PhysRevC.89.024313
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2014VA02      Phys.Rev. C 89, 054323 (2014)

Zs.Vajta, M.Stanoiu, D.Sohler, G.R.Jansen, F.Azaiez, Zs.Dombradi, O.Sorlin, B.A.Brown, M.Belleguic, C.Borcea, C.Bourgeois, Z.Dlouhy, Z.Elekes, Zs.Fulop, S.Grevy, D.Guillemaud-Mueller, G.Hagen, M.Hjorth-Jensen, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, S.Mandal, P.Mayet, J.Mrazek, F.Negoita, Yu.-E.Penionzhkevich, Zs.Podolyak, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.Timar, C.Timis, A.Yamamoto

Excited states in the neutron-rich nucleus 25F

NUCLEAR REACTIONS C(26Ne, 25F), (27Na, 25F), (28Na, 25F), [secondary 26Ne, 27,28Na beams from C(36S, X), E=77.5 MeV/nucleon primary reaction], E=54-65 MeV/nucleon; measured Eγ, Iγ, γγ-, (25F)γ-coin, time-of-flight using SPEG magnetic spectrometer and an array of 74 BaF2 crystals for γ-rays at GANIL facility, GEANT4 simulations. 25F; deduced levels, J, π. Comparison with shell-model calculations, coupled-cluster theory, and other data.

doi: 10.1103/PhysRevC.89.054323
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013BA57      Phys.Rev. C 88, 051301 (2013)

V.M.Bader, A.Gade, D.Weisshaar, B.A.Brown, T.Baugher, D.Bazin, J.S.Berryman, A.Ekstrom, M.Hjorth-Jensen, S.R.Stroberg, W.B.Walters, K.Wimmer, R.Winkler

Quadrupole collectivity in neutron-deficient Sn nuclei: 104Sn and the role of proton excitations

NUCLEAR REACTIONS 197Au(104Sn, 104Sn'), (102Cd, 102Cd'), [102Cd, 104Sn secondary beams from 9Be(124Xe, X), E=140 MeV/nucleon primary reaction], E=67 MeV/nucleon for 104Sn and 64 MeV/nucleon for 102Cd; measured scattered particle spectra, Eγ, Iγ, (particle)γ-coin using A1900 fragment separator, Si p-i-n detector and TOF for particles and CAESAR array of scintillation detectors for γ rays at NSCL-MSU facility. 104Sn; deduced level, B(E2) for first 2+ state relative to that for 102Cd. Comparison with previous experimental results, and with large-scale shell model calculations. Enhanced quadrupole collectivity. Systematics of B(E2) values for A=104 to 130 even-A Sn nuclei.

doi: 10.1103/PhysRevC.88.051301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013BA58      Phys.Rev. C 88, 054312 (2013)

G.Baardsen, A.Ekstrom, G.Hagen, M.Hjorth-Jensen

Coupled-cluster studies of infinite nuclear matter

doi: 10.1103/PhysRevC.88.054312
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2013DI01      Phys.Rev. C 87, 017301 (2013)

D.D.DiJulio, J.Cederkall, C.Fahlander, A.Ekstrom, M.Hjorth-Jensen, M.Albers, V.Bildstein, A.Blazhev, I.Darby, T.Davinson, H.De Witte, J.Diriken, Ch.Fransen, K.Geibel, R.Gernhauser, A.Gorgen, H.Hess, K.Heyde, J.Iwanicki, R.Lutter, P.Reiter, M.Scheck, M.Seidlitz, S.Siem, J.Taprogge, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, F.Wenander, K.Wimmer

Coulomb excitation of 107In

NUCLEAR REACTIONS 58Ni(107In, 107In'), (107Sn, 107Sn'), [107In and 107Sn secondary beams from LaCx(p, X), E=1.4 GeV primary reaction], E=2.87 MeV/nucleon; measured Eγ, Iγ, scattered particle spectra, (particle)γ-coin, B(E2) using REX-ISOLDE, MINIBALL Ge array facility at CERN. 107In; deduced levels, J, π, B(E2). GOSIA2 analysis for Coulomb excitation. 58Ni; measured Eγ, Iγ, used known B(E2) for first 2+ state for normalization of data for 107In. Comparison with experimental B(E2) values for 113,115In, and with large-scale shell model calculations. 107Sn; observed γ ray spectrum.

doi: 10.1103/PhysRevC.87.017301
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013EK01      Phys.Rev.Lett. 110, 192502 (2013)

A.Ekstrom, G.Baardsen, C.Forssen, G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, W.Nazarewicz, T.Papenbrock, J.Sarich, S.M.Wild

Optimized Chiral Nucleon-Nucleon Interaction at Next-to-Next-to-Leading Order

NUCLEAR STRUCTURE 3H, 3,4He, 10B, 17,22,24O, 40,48,50,52,54,56Ca; calculated energy of the first 2+ state, energy per nucleon for neutron matter, phase shifts. The nucleon-nucleon interaction from chiral effective field theory at next-to-next-to-leading order (NNLO).

doi: 10.1103/PhysRevLett.110.192502
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2013FO06      Phys.Scr. T152, 014022 (2013)

C.Forssen, G.Hagen, M.Hjorth-Jensen, W.Nazarewicz, J.Rotureau

Living on the edge of stability, the limits of the nuclear landscape

doi: 10.1088/0031-8949/2013/T152/014022
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2013LE03      Phys.Rev.Lett. 110, 082502 (2013)

A.Lepailleur, O.Sorlin, L.Caceres, B.Bastin, C.Borcea, R.Borcea, B.A.Brown, L.Gaudefroy, S.Grevy, G.F.Grinyer, G.Hagen, M.Hjorth-Jensen, G.R.Jansen, O.Llidoo, F.Negoita, F.de Oliveira, M.-G.Porquet, F.Rotaru, M.-G.Saint-Laurent, D.Sohler, M.Stanoiu, J.C.Thomas

Spectroscopy of 26F to Probe Proton-Neutron Forces Close to the Drip Line

RADIOACTIVITY 26F(β-), (β-n) [from Be(36S, X)26F, E=77.6 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced decay scheme, J, π, long-lived isomer T1/2. Comparison with available data.

doi: 10.1103/PhysRevLett.110.082502
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013LI04      Phys.Rev. C 87, 014325 (2013)

S.N.Liddick, B.Abromeit, A.Ayres, A.Bey, C.R.Bingham, B.A.Brown, L.Cartegni, H.L.Crawford, I.G.Darby, R.Grzywacz, S.Ilyushkin, M.Hjorth-Jensen, N.Larson, M.Madurga, D.Miller, S.Padgett, S.V.Paulauskas, M.M.Rajabali, K.Rykaczewski, S.Suchyta

Low-energy level schemes of 66, 68Fe and inferred proton and neutron excitations across Z=28 and N=40

RADIOACTIVITY 66,68Mn(β-)[from 9Be(86Kr, X), E=140 MeV/nucleon]; measured Eγ, Iγ, (Mn ions)γ-, γγ-coin, Eβ, Iβ, T1/2 using the BCS system and SeGA array at NSCL facility. 66,68Fe; deduced levels, J, π, β feedings, logft. 66,68Fe, 68Ni; comparison of experimental levels, J, π with shell-model calculations.

doi: 10.1103/PhysRevC.87.014325
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013TA19      J.Phys.:Conf.Ser. 445, 012003 (2013)

K.Takayanagi, N.Tsunoda, M.Hjorth-Jensen, T.Otsuka

Effective Hamiltonian in non-degenerate model space

doi: 10.1088/1742-6596/445/1/012003
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2012DI12      Eur.Phys.J. A 48, 105 (2012)

D.D.DiJulio, J.Cederkall, C.Fahlander, A.Ekstrom, M.Hjorth-Jensen, M.Albers, V.Bildstein, A.Blazhev, I.Darby, T.Davinson, H.De Witte, J.Diriken, Ch.Fransen, K.Geibel, R.Gernhauser, A.Gorgen, H.Hess, J.Iwanicki, R.Lutter, P.Reiter, M.Scheck, M.Seidlitz, S.Siem, J.Taprogge, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, F.Wenander, K.Wimmer

Coulomb excitation of 107Sn

NUCLEAR REACTIONS 58Ni(107Sn, 107Sn'), E=2.87 MeV/nucleon; measured Coulomb excitation Eγ, Iγ using HPGe MINIBALL detector array, particles using DSSSD (double-sided Si strip detector), γ(Ni)-coin. 107,109Sn deduced levels, J, π, γ transitions, B(E2), B(M1) using GOSIA2 code; calculated levels, J, π, γ transitions, B(E2) using shell model.

doi: 10.1140/epja/i2012-12105-7
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Data from this article have been entered in the XUNDL database. For more information, click here.


2012DI13      Phys.Rev. C 86, 031302 (2012)

D.D.DiJulio, J.Cederkall, C.Fahlander, A.Ekstrom, M.Hjorth-Jensen, M.Albers, V.Bildstein, A.Blazhev, I.Darby, T.Davinson, H.De Witte, J.Diriken, Ch.Fransen, K.Geibel, R.Gernhauser, A.Gorgen, H.Hess, J.Iwanicki, R.Lutter, P.Reiter, M.Scheck, M.Seidlitz, S.Siem, J.Taprogge, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, F.Wenander, K.Wimmer

Excitation strengths in 109Sn: Single-neutron and collective excitations near 100Sn

NUCLEAR REACTIONS 58Ni(109Sn, 109Sn'), E=2.87 MeV/nucleon, [109Sn beam from La(p, X), E=1.4 GeV]; measured Eγ, Iγ using the MINIBALL array and REX-ISOLDE facility at CERN. 58Ni, 109Sn; deduced levels, J, π, B(E2). GOSIA2 analysis for Coulomb excitation. Comparison with shell-model calculations. Single neutron excitations relative to 100Sn core.

doi: 10.1103/PhysRevC.86.031302
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Data from this article have been entered in the XUNDL database. For more information, click here.


2012DI15      Phys.Scr. T150, 014012 (2012)

D.D.DiJulio, J.Cederkall, A.Ekstrom, C.Fahlander, M.Hjorth-Jensen

Shell model based Coulomb excitation γ-ray intensity calculations in 107Sn

NUCLEAR STRUCTURE 107,109Sn; calculated γ-ray yields, energy levels, J, π. Comparison with available data.

doi: 10.1088/0031-8949/2012/T150/014012
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2012DI18      J.Phys.:Conf.Ser. 381, 012073 (2012)

D.D.DiJulio, J.Cederkall, A.Ekstrom, C.Fahlander, M.Hjorth-Jensen, for the IS459 collaboration

Sub-barrier Coulomb excitation of 107Sn

NUCLEAR REACTIONS 58Ni(107Sn, 107Sn'), E=2.866 MeV/nucleon[La(p, X)107Sn, E=1.4 GeV]; measured Coulomb excitation scattered Sn, Ni nuclei using DSSSD, Doppler corrected Eγ, Iγ at REX-ISOLDE; calculated γ ray spectra using shell-model with GOSIA; deduced ordering of single-particle orbits.

doi: 10.1088/1742-6596/381/1/012073
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2012HA19      Phys.Rev.Lett. 108, 242501 (2012)

G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, T.Papenbrock

Continuum Effects and Three-Nucleon Forces in Neutron-Rich Oxygen Isotopes

NUCLEAR STRUCTURE 18,22,23,24O; calculated level energies, J, π, point matter and charge radii, 24O long-lived resonances. Chiral effective field interaction, comparison with available data.

doi: 10.1103/PhysRevLett.108.242501
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2012HA26      Phys.Rev.Lett. 109, 032502 (2012)

G.Hagen, M.Hjorth-Jensen, G.R.Jansen, R.Machleidt, T.Papenbrock

Evolution of Shell Structure in Neutron-Rich Calcium Isotopes

NUCLEAR STRUCTURE 42,48,50,52,53,54,55,56,61Ca, 50,54,56Ti; calculated ground state energies, J, π. Chiral effective field theory, comparison with available data.

doi: 10.1103/PhysRevLett.109.032502
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2012TO01      Phys.Rev. C 85, 017305 (2012)

D.A.Torres, G.J.Kumbartzki, Y.Y.Sharon, L.Zamick, B.Manning, N.Benczer-Koller, K.-H.Speidel, T.Ahn, V.Anagnostatou, M.Elvers, P.Goddard, A.Heinz, G.Ilie, D.Radeck, D.Savran, V.Werner, G.Gurdal, M.J.Taylor, P.Maier-Komor, M.Hjorth-Jensen, S.J.Q.Robinson

Measurement of the 96Ru g(41+) factor and its nuclear structure interpretation

NUCLEAR REACTIONS 12C(96Ru, 96Ru'), E=343, 353 MeV; measured 12C spectra, Eγ, Iγ, (12C)g-coin, (12C)γ(θ), precession angle in transient magnetic field, half-life by DSAM. 96Ru; deduced level, half-life of first 2+, g factors of first 2+ and 4+ states, B(E2). Coulomb excitation in inverse kinematics. Comparison with large-scale shell-model calculations.

NUCLEAR MOMENTS 96Ru; measured g factors of first 2+ and 4+ states by transient magnetic field technique in inverse kinematics.

doi: 10.1103/PhysRevC.85.017305
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2011JA06      Phys.Rev. C 83, 054306 (2011)

G.R.Jansen, M.Hjorth-Jensen, G.Hagen, T.Papenbrock

Toward open-shell nuclei with coupled-cluster theory

NUCLEAR STRUCTURE 3,4,5,6He; calculated ground-state energies, first 2+ state energy in 6He, expectation value of total angular Momentum. Method based on equation-of-motion coupled-cluster theory.

doi: 10.1103/PhysRevC.83.054306
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2011JE02      Phys.Rev. C 83, 021305 (2011)

O.Jensen, G.Hagen, M.Hjorth-Jensen, J.S.Vaagen

Closed-shell properties of 24O with ab initio coupled-cluster theory

NUCLEAR STRUCTURE 23O, 23Ne; calculated single-particle levels, J, π. 24O; calculated neutron- and proton-removal spectroscopic factors for hole states in 24O. Coupled-cluster method with chiral nucleon-nucleon N3L interaction including role of continuum states. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.021305
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2011JE03      Phys.Rev.Lett. 107, 032501 (2011)

O.Jensen, G.Hagen, M.Hjorth-Jensen, B.A.Brown, A.Gade

Quenching of Spectroscopic Factors for Proton Removal in Oxygen Isotopes

NUCLEAR STRUCTURE 14,16,22,24,28O; calculated radial overlap functions, spectroscopic factors. Hartree-Fock built from Woods-Saxon single-particle basis.

doi: 10.1103/PhysRevLett.107.032501
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2011SI05      Phys.Rev. C 83, 024315 (2011)

A.Signoracci, B.A.Brown, M.Hjorth-Jensen

Renormalized interactions with a realistic single-particle basis

NUCLEAR STRUCTURE 34Si, 40Ca; calculated single-particle energies, First-order, particle-particle ladder, core-polarization, four-particle two-hole, and total matrix elements using Skxtb interaction and harmonic oscillator basis. 36,38Si; calculated levels, J, π. Shell-model using Harmonic oscillator, core polarization and Skyrme Hartree-Fock calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.024315
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2011TO09      Phys.Rev. C 84, 044327 (2011)

D.A.Torres, G.J.Kumbartzki, Y.Y.Sharon, L.Zamick, B.Manning, N.Benczer-Koller, G.Gurdal, K.-H.Speidel, M.Hjorth-Jensen, P.Maier-Komor, S.J.Q.Robinson, T.Ahn, V.Anagnostatou, M.Elvers, P.Goddard, A.Heinz, G.Ilie, D.Radeck, D.Savran, V.Werner

First g-factor measurements of the 21+ and the 41+ states of radioactive 100Pd

NUCLEAR REACTIONS 12C(96Ru, 8Be), E=350 MeV; measured particle spectra, Eγ, Iγ, αγ-, γγ-coin, γγ(θ), precession angle. 100Pd; deduced levels, J, π, g factors, B(E2) values.

NUCLEAR MOMENTS 100Pd; measured g-factors of first 2+, 4+ states by transient magnetic field technique in inverse kinematics. Comparison with large-scale shell-model calculations and collective-model predictions.

doi: 10.1103/PhysRevC.84.044327
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2011TS07      Phys.Rev. C 84, 044322 (2011)

N.Tsunoda, T.Otsuka, K.Tsukiyama, M.Hjorth-Jensen

Renormalization persistency of the tensor force in nuclei

doi: 10.1103/PhysRevC.84.044322
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2010AT03      Europhys.Lett. 91, 42001 (2010)

L.Atanasova, D.L.Balabanski, S.K.Chamoli, M.Hass, G.S.Simpson, D.Bazzacco, F.Becker, P.Bednarczyk, G.Benzoni, N.Blasi, A.Blazhev, A.Bracco, C.Brandau, L.Caceres, F.Camera, F.C.L.Crespi, P.Detistov, P.Doornenbal, C.Fahlander, E.Farnea, G.Georgiev, J.Gerl, K.A.Gladnishki, M.Gorska, J.Grebosz, R.Hoischen, G.Ilie, M.Ionescu-Bujor, A.Iordachescu, A.Jungclaus, G.Lo Bianco, M.Kmiecik, I.Kojouharov, N.Kurz, S.Lakshmi, R.Lozeva, A.Maj, D.Montanari, G.Neyens, M.Pfutzner, S.Pietri, Zs.Podolyak, W.Prokopowicz, D.Rudolph, G.Rusev, T.R.Saito, A.Saltarelli, H.Schaffner, R.Schwengner, S.Tashenov, J.J.Valiente-Dobon, N.Vermeulen, J.Walker, E.Werner-Malento, O.Wieland, H.J.Wollersheim, H.Grawe, M.Hjorth-Jensen

g-factor measurements at RISING: The cases of 127Sn and 128Sn

NUCLEAR REACTIONS Be(136Xe, X)127Sn/128Sn, E=600 MeV/nucleon; measured reaction products, Larmor precession, Eγ, Iγ; deduced g factors for Sn isomers, J, π. Comparison with shell model calculations.

doi: 10.1209/0295-5075/91/42001
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2010DA17      Phys.Rev.Lett. 105, 162502 (2010)

I.G.Darby, R.K.Grzywacz, J.C.Batchelder, C.R.Bingham, L.Cartegni, C.J.Gross, M.Hjorth-Jensen, D.T.Joss, S.N.Liddick, W.Nazarewicz, S.Padgett, R.D.Page, T.Papenbrock, M.M.Rajabali, J.Rotureau, K.P.Rykaczewski

Orbital Dependent Nucleonic Pairing in the Lightest Known Isotopes of Tin

RADIOACTIVITY 109Xe, 105Te(α); measured Iα, Eα, Iγ, Iγ; deduced J, π for ground and first excited states in 101Sn, ground state spin inversion, strong pairing interaction. Comparison with shell model calculations.

doi: 10.1103/PhysRevLett.105.162502
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2010EK01      Eur.Phys.J. A 44, 355 (2010)

A.Ekstrom, J.Cederkall, C.Fahlander, M.Hjorth-Jensen, T.Engeland, A.Blazhev, P.A.Butler, T.Davinson, J.Eberth, F.Finke, A.Gorgen, M.Gorska, A.M.Hurst, O.Ivanov, J.Iwanicki, U.Koster, B.A.Marsh, J.Mierzejewski, P.Reiter, S.Siem, G.Sletten, I.Stefanescu, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, M.Zielinska

Coulomb excitation of the odd-odd isotopes 106, 108In

NUCLEAR REACTIONS 58Ni(106In, 106In'), (108In, 108In'), E=2.8 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation at the REX-ISOLDE facility. 106,108In; deduced levels, J, π, B(E2); calculated low-lying level properties, E2, M1 matrix elements using shell model plus coupled channels.

doi: 10.1140/epja/i2010-10945-7
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2010HA11      Phys.Rev.Lett. 104, 182501 (2010)

G.Hagen, T.Papenbrock, M.Hjorth-Jensen

Ab Initio Computation of the 17F Proton Halo State and Resonances in A=17 Nuclei

NUCLEAR STRUCTURE 17O, 17F; calculated energies of proton halo states, J, π. deduced continuum effect binding energy yields.

doi: 10.1103/PhysRevLett.104.182501
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2010HA22      Phys.Rev. C 82, 034330 (2010)

G.Hagen, T.Papenbrock, D.J.Dean, M.Hjorth-Jensen

Ab initio coupled-cluster approach to nuclear structure with modern nucleon-nucleon interactions

NUCLEAR STRUCTURE 4He, 16,17,22,24,25,28O, 16,22,24,25,28F, 40,48Ca; calculated ground-state energies, rms radii, single-particle energies, and binding energies. Coupled-cluster model with bare and secondary renormalized nucleon-nucleon interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.034330
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2010HO13      Phys.Rev. C 82, 044305 (2010)

N.Hoteling, C.J.Chiara, R.Broda, W.B.Walters, R.V.F.Janssens, M.Hjorth-Jensen, M.P.Carpenter, B.Fornal, A.A.Hecht, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, X.Wang, A.Wohr, J.Wrzesinski, S.Zhu

Structure of 60, 62Fe and the onset of νg9/2 occupancy

NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), prompt and delayed γ spectra using Gammasphere array. 60,62Fe; deduced levels, J, π, multipolarity, yrast levels. Comparison with shell model calculations. Level systematics of 54,56,58,60,62,64Fe nuclei.

RADIOACTIVITY 60,62Mn(β-)[from 238U(64Ni, X), E=430 MEV]; measured Eγ, Iγ, γγ-coin, γγ(θ) using Gammasphere array. 60,62Fe; deduced levels, J, π, multipolarity.

doi: 10.1103/PhysRevC.82.044305
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2010OT01      Phys.Rev.Lett. 104, 012501 (2010)

T.Otsuka, T.Suzuki, M.Honma, Y.Utsuno, N.Tsunoda, K.Tsukiyama, M.Hjorth-Jensen

Novel Features of Nuclear Forces and Shell Evolution in Exotic Nuclei

NUCLEAR STRUCTURE Z=8-20, 28, 40, N=20, 40-50; 40Ca, 68Ni, 78Ni, 90Zr, 100Sn; calculated monopole matrix elements, single-particle energies for pf and sd-shells; deduced monopole-based universal interaction, shell evolution. Comparison with USD, KB3, GXPF1A interactions.

doi: 10.1103/PhysRevLett.104.012501
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2009BA29      Phys.Rev. C 79, 064313 (2009)

C.Barbieri, M.Hjorth-Jensen

Quasiparticle and quasihole states of nuclei around 56Ni

NUCLEAR STRUCTURE 55,56,57Ni, 57Cu, 55Co; calculated single-particle energies and spectroscopic factors using Faddeev random phase approximation and G matrix technique in the framework of self-consistent Green's function theory with N3LO interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.064313
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2009EK01      Phys.Rev. C 80, 054302 (2009)

A.Ekstrom, J.Cederkall, D.D.DiJulio, C.Fahlander, M.Hjorth-Jensen, A.Blazhev, B.Bruyneel, P.A.Butler, T.Davinson, J.Eberth, C.Fransen, K.Geibel, H.Hess, O.Ivanov, J.Iwanicki, O.Kester, J.Kownacki, U.Koster, B.A.Marsh, P.Reiter, M.Scheck, B.Siebeck, S.Siem, I.Stefanescu, H.K.Toft, G.M.Tveten, J.Van de Walle, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, K.Wrzosek, M.Zielinska

Electric quadrupole moments of the 2+1 states in 100, 102, 104Cd

NUCLEAR REACTIONS 109Ag(100Cd, 100Cd'), E=287.0 MeV; 64Zn, 109Ag(102Cd, 102Cd'), E=292.7 MeV; 64Zn, 109Ag(104Cd, 104Cd'), E=298.7 MeV; measured Eγ, Iγ, γ(particle)-coin, and γ-ray yields using REX-ISOLDE facility. 64Zn, 100,102,104Cd, 109Ag; deduced levels, J, π, E2 matrix elements, electric quadrupole moments. Comparison with shell model calculations.

NUCLEAR MOMENTS 100,102,104Cd; measured electric quadrupole moments of first 2+ states using reorientation method in Coulomb excitation. Comparison with shell model calculations.

doi: 10.1103/PhysRevC.80.054302
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2009HA26      Phys.Rev. C 80, 021306 (2009)

G.Hagen, T.Papenbrock, D.J.Dean, M.Hjorth-Jensen, B.Velamur Asokan

Ab initio computation of neutron-rich oxygen isotopes

NUCLEAR STRUCTURE 16,22,24,28O; calculated ground-state energies, binding energies and rms point matter radii using ab initio calculations with the coupled-cluster model and chiral nucleon-nucleon interaction N3LO. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.021306
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2009HO14      Phys.Rev. C 80, 064323 (2009)

M.Honma, T.Otsuka, T.Mizusaki, M.Hjorth-Jensen

New effective interaction for f5pg9-shell nuclei

NUCLEAR STRUCTURE Z=28-50, N=28-50; calculated two-body matrix elements, monopole matrix elements, single-particle proton and neutron energies, binding energies, magnetic dipole moments, electric quadrupole moments, levels, and B(E2) using shell-model in f5pg9 model space with a new JUN45 effective interaction based on realistic Bonn-C potential. 64,69,70,71,72,73,74,75Ge, 66,82As, 68Se, 70,84Br, 80Ga, 86Rb, 88Y; calculated levels, J, π, and transition matrix elements using shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.064323
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2009TS08      Phys.Rev. C 80, 051301 (2009)

K.Tsukiyama, M.Hjorth-Jensen, G.Hagen

Gamow shell-model calculations of drip-line oxygen isotopes

NUCLEAR STRUCTURE 24,25O; calculated low-lying levels and resonant states using Gamow Shell Model calculations. Discussed nuclear stability. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.051301
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2008EK01      Phys.Rev.Lett. 101, 012502 (2008)

A.Ekstrom, J.Cederkall, C.Fahlander, M.Hjorth-Jensen, F.Ames, P.A.Butler, T.Davinson, J.Eberth, F.Fincke, A.Gorgen, M.Gorska, D.Habs, A.M.Hurst, M.Huyse, O.Ivanov, J.Iwanicki, O.Kester, U.Koster, B.A.Marsh, J.Mierzejewski, P.Reiter, H.Scheit, D.Schwalm, S.Siem, G.Sletten, I.Stefanescu, G.M.Tveten, J.Van de Walle, P.Van Duppen, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, M.Zielinska

0+gs → 2+1 Transition Strengths in 106Sn and 108Sn

NUCLEAR REACTIONS 58Ni(106Sn, X), E=2.83 MeV/nucleon; 58Ni(108Sn, X), E=2.82 MeV/nucleon; measured Eγ, Iγ following coulomb excitations.106,108Sn; deduced B(E2).

doi: 10.1103/PhysRevLett.101.012502
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2008HA30      Phys.Rev.Lett. 101, 092502 (2008)

G.Hagen, T.Papenbrock, D.J.Dean, M.Hjorth-Jensen

Medium-Mass Nuclei from Chiral Nucleon-Nucleon Interactions

NUCLEAR STRUCTURE 4He, 16O, 40Ca, 48Ca, 48Ni; calculated binding energies, radii and densities; spherical coupled-cluster theory; bare chiral NN-interaction;

doi: 10.1103/PhysRevLett.101.092502
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2008HO05      Phys.Rev. C 77, 044314 (2008)

N.Hoteling, W.B.Walters, R.V.F.Janssens, R.Broda, M.P.Carpenter, B.Fornal, A.A.Hecht, M.Hjorth-Jensen, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, J.R.Stone, X.Wang, A.Wohr, J.Wrzesinski, S.Zhu

Rotation-aligned coupling in 61Fe

NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin. 61Fe; deduced levels, J, π. 59Fe; measured Eγ, Iγ. 56,57,58,59,60Fe; systematics. Comparisons with shell model and particle-triaxial rotor model.

doi: 10.1103/PhysRevC.77.044314
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2007AL49      Phys.Atomic Nuclei 70, 1634 (2007)

E.Algin, A.Schiller, A.Voinov, U.Agvaanluvsan, T.Belgya, L.A.Bernstein, C.R.Brune, R.Chankova, P.E.Garrett, S.M.Grimes, M.Guttormsen, M.Hjorth-Jensen, M.J.Hornish, C.W.Johnson, T.Massey, G.E.Mitchell, J.Rekstad, S.Siem, W.Younes

Bulk properties of iron isotopes

NUCLEAR REACTIONS 57Fe(3He, α), (3He, 3He'), E=45 MeV; 56Fe(n, γ), E=thermal; 55Mn(d, n), E=7.0 MeV; measured Eγ, Iγ. Deduced nuclear level densities and radiative strength functions. Compared results to model calculations.

doi: 10.1134/S1063778807090232
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2007CE02      Phys.Rev.Lett. 98, 172501 (2007)

J.Cederkall, A.Ekstrom, C.Fahlander, A.M.Hurst, M.Hjorth-Jensen, F.Ames, A.Banu, P.A.Butler, T.Davinson, U.Datta Pramanik, J.Eberth, S.Franchoo, G.Georgiev, M.Gorska, D.Habs, M.Huyse, O.Ivanov, J.Iwanicki, O.Kester, U.Koster, B.A.Marsh, O.Niedermaier, T.Nilsson, P.Reiter, H.Scheit, D.Schwalm, T.Sieber, G.Sletten, I.Stefanescu, J.Van de Walle, P.Van Duppen, N.Warr, D.Weisshaar, F.Wenander

Sub-Barrier Coulomb Excitation of 110Sn and Its Implications for the 100Sn Shell Closure

NUCLEAR REACTIONS 58Ni(110Sn, 110Sn'), E=2.82 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation. 110Sn deduced B(E2) of the first excited 2+ state. MINIBALL array at REX-ISOLDE.

doi: 10.1103/PhysRevLett.98.172501
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2007HA44      Phys.Rev. C 76, 044305 (2007)

G.Hagen, D.J.Dean, M.Hjorth-Jensen, T.Papenbrock, A.Schwenk

Benchmark calculations for 3H, 4He, 16O, and 40Ca with ab initio coupled-cluster theory

NUCLEAR STRUCTURE 3H, 4He, 16O, 40Ca; calculated CCSD and CCSD(T) energies. Coupled-cluster theory.

doi: 10.1103/PhysRevC.76.044305
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2007KA40      Phys.Rev. C 76, 024313 (2007)

M.P.Kartamyshev, T.Engeland, M.Hjorth-Jensen, E.Osnes

Effective interactions and shell model studies of heavy tin isotopes

NUCLEAR STRUCTURE 134,135,136,137,138,139,140,141,142Sn; calculated binding energies, single and two neutron separation energies, level energies, J, π, B(E2) using the single particle model.

doi: 10.1103/PhysRevC.76.024313
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2007VA22      Phys.Rev.Lett. 99, 162501 (2007)

C.Vaman, C.Andreoiu, D.Bazin, A.Becerril, B.A.Brown, C.M.Campbell, A.Chester, J.M.Cook, D.C.Dinca, A.Gade, D.Galaviz, T.Glasmacher, M.Hjorth-Jensen, M.Horoi, D.Miller, V.Moeller, W.F.Mueller, A.Schiller, K.Starosta, A.Stolz, J.R.Terry, A.Volya, V.Zelevinsky, H.Zwahlen

Z=50 Shell Gap near 100Sn from Intermediate-Energy Coulomb Excitations in Even-Mass 106-112Sn Isotopes

NUCLEAR REACTIONS 197Au(106Sn, 106Sn'), (108Sn, 108Sn'), (110Sn, 110sn'), (112Sn, 112Sn'), E=78-81 MeV; measured Eγ, Iγ, (particle)γ-coinc from projectile coulomb excitation. 106,108,110,112Sn deduced B(E2).

doi: 10.1103/PhysRevLett.99.162501
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2006GO22      Phys.Rev. C 74, 024310 (2006)

J.R.Gour, P.Piecuch, M.Hjorth-Jensen, M.Wloch, D.J.Dean

Coupled-cluster calculations for valence systems around 16O

NUCLEAR STRUCTURE 15N, 15,17O, 17F; calculated excited states energies, configurations. Equation-of-motion coupled-cluster methods, comparison with data.

doi: 10.1103/PhysRevC.74.024310
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2006HA23      Phys.Rev. C 73, 064307 (2006)

G.Hagen, M.Hjorth-Jensen, N.Michel

Gamow shell model and realistic nucleon-nucleon interactions

NUCLEAR STRUCTURE 4He, 16O; calculated single-particle energies. 6He, 18O; calculated level energies, configurations. Gamow shell model.

doi: 10.1103/PhysRevC.73.064307
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2006HO20      Phys.Rev.C 74, 064313 (2006)

N.Hoteling, W.B.Walters, R.V.F.Janssens, R.Broda, M.P.Carpenter, B.Fornal, A.A.Hecht, M.Hjorth-Jensen, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, X.Wang, A.Wohr, J.Wrzesinski, S.Zhu

Yrast structure of 64Fe

NUCLEAR REACTIONS 238U(64Ni, X)64Fe/69Ga, E=430 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 64Fe deduced levels, J, π, configurations. Gammasphere array, comparison with shell model predictions. Level systematics in neighboring nuclides discussed.

doi: 10.1103/PhysRevC.74.064313
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2006LE24      Phys.Rev. C 73, 064305 (2006)

J.Leske, K.-H.Speidel, S.Schielke, J.Gerber, P.Maier-Komor, T.Engeland, M.Hjorth-Jensen

Experimental g factor and B(E2) value of the 41+ state in Coulomb-excited 66Zn compared to shell-model predictions

NUCLEAR REACTIONS C(66Zn, 66Zn'), E=180 MeV; measured Eγ, Iγ(θ, H, t), DSA, (recoil)γ-coin following projectile Coulomb excitation. 66Zn levels deduced T1/2, B(E2), g factors. Comparison with neighboring isotopes, shell-model calculations.

doi: 10.1103/PhysRevC.73.064305
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2005BB09      Phys.Rev. C 72, 061305 (2005)

A.Banu, J.Gerl, C.Fahlander, M.Gorska, H.Grawe, T.R.Saito, H.-J.Wollersheim, E.Caurier, T.Engeland, A.Gniady, M.Hjorth-Jensen, F.Nowacki, T.Beck, F.Becker, P.Bednarczyk, M.A.Bentley, A.Burger, F.Cristancho, G.de Angelis, Zs.Dombradi, P.Doornenbal, H.Geissel, J.Grebosz, G.Hammond, M.Hellstrom, J.Jolie, I.Kojouharov, N.Kurz, R.Lozeva, S.Mandal, N.Marginean, S.Muralithar, J.Nyberg, J.Pochodzalla, W.Prokopowicz, P.Reiter, D.Rudolph, C.Rusu, N.Saito, H.Schaffner, D.Sohler, H.Weick, C.Wheldon, M.Winkler

108Sn studied with intermediate-energy Coulomb excitation

NUCLEAR REACTIONS 197Au(108Sn, 108Sn'), E=142 MeV; 197Au(112Sn, 112Sn'), E=147 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 108,112Sn levels deduced excitation B(E2), core polarization features. Comparison with large-scale shell model predictions.

doi: 10.1103/PhysRevC.72.061305
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2005BR12      Phys.Rev. C 71, 044317 (2005); Erratum Phys.Rev. C 72, 029901 (2005)

B.A.Brown, N.J.Stone, J.R.Stone, I.S.Towner, M.Hjorth-Jensen

Magnetic moments of the 2+1 states around 132Sn

NUCLEAR STRUCTURE 130Sn, 132Sb, 132,134Te; calculated levels, J, π. 124,126,128,130,134Sn, 130,132,134,136Te, 134,136,138Xe, 138Ba; calculated g factors, μ. Shell model, comparisons with data.

doi: 10.1103/PhysRevC.71.044317
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2005DE13      Nucl.Phys. A752, 299c (2005)

D.J.Dean, J.R.Gour, G.Hagen, M.Hjorth-Jensen, K.Kowalski, T.Papenbrock, P.Piecuch, M.Wloch

Nuclear Structure Calculations with Coupled Cluster Methods from Quantum Chemistry

NUCLEAR STRUCTURE 4He, 16O; calculated ground and excited states energies. Coupled cluster approximation.

doi: 10.1016/j.nuclphysa.2005.02.041
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2005EL05      Phys.Rev. C 71, 034301 (2005)

P.J.Ellis, T.Engeland, M.Hjorth-Jensen, M.P.Kartamyshev, E.Osnes

Model calculation of effective three-body forces

doi: 10.1103/PhysRevC.71.034301
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2005HA21      Phys.Rev. C 71, 044314 (2005)

G.Hagen, M.Hjorth-Jensen, J.S.Vaagen

Effective interaction techniques for the Gamow shell model

NUCLEAR STRUCTURE 5,6,7He; calculated level energies, configurations. Gamow shell model, effective interactions compared.

doi: 10.1103/PhysRevC.71.044314
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2005HA41      J.Phys.(London) G31, S1337 (2005)

G.Hagen, M.Hjorth-Jensen, J.S.Vaagen

State-dependent interactions for the Gamow shell model

NUCLEAR STRUCTURE 5,6,7He; calculated resonance energies, configurations. Gamow shell model.

doi: 10.1088/0954-3899/31/8/012
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2005LE38      Phys.Rev. C 72, 044301 (2005)

J.Leske, K.-H.Speidel, S.Schielke, J.Gerber, P.Maier-Komor, T.Engeland, M.Hjorth-Jensen

Dominant (g9/2)2 neutron configuration in the 4+1 state of 68Zn based on new g factor measurements

NUCLEAR REACTIONS C(68Zn, 68Zn'), E=180 MeV; measured Eγ, Iγ(θ, H, t) (particle)γ-coin following projectile Coulomb excitation. 68Zn levels deduced g factors, T1/2, B(E2), configurations. 64Zn levels analyzed g factors, B(E2). Large-scale shell-model calculations.

doi: 10.1103/PhysRevC.72.044301
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2005SO06      Nucl.Phys. A753, 251 (2005)

D.Sohler, M.Palacz, Zs.Dombradi, M.Hjorth-Jensen, C.Fahlander, L.-O.Norlin, J.Nyberg, T.Back, K.Lagergren, D.Rudolph, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, J.Cederkall, B.Cederwall, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, J.Timar, M.Weiszflog, M.Wolinska

Maximally aligned states in the proton drip line nucleus 106Sb

NUCLEAR REACTIONS 54Fe(58Ni, npα), E=240 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, γ-ray polarization. 106Sb deduced high-spin levels, J, π, configurations. Euroball, ISIS arrays.

doi: 10.1016/j.nuclphysa.2005.02.153
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2005WL01      Phys.Rev.Lett. 94, 212501 (2005)

M.Wloch, D.J.Dean, J.R.Gour, M.Hjorth-Jensen, K.Kowalski, T.Papenbrock, P.Piecuch

Ab-Initio Coupled-Cluster Study of 16O

NUCLEAR STRUCTURE 16O; calculated matter density, charge radius, charge form factor, excited states energies. Coupled-cluster singles and doubles approach, comparison with data.

doi: 10.1103/PhysRevLett.94.212501
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2005WL02      J.Phys.(London) G31, S1291 (2005)

M.Wloch, J.R.Gour, P.Piecuch, D.J.Dean, M.Hjorth-Jensen, T.Papenbrock

Coupled-cluster calculations for ground and excited states of closed- and open-shell nuclei using methods of quantum chemistry

NUCLEAR STRUCTURE 15,16,17O; calculated ground and excited states energies, configurations. Coupled-cluster methods.

doi: 10.1088/0954-3899/31/8/007
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2005WL03      Eur.Phys.J. A 25, Supplement 1, 485 (2005)

M.Wloch, D.J.Dean, J.R.Gour, P.Piecuch, M.Hjorth-Jensen, T.Papenbrock, K.Kowalski

Ab initio coupled cluster calculations for nuclei using methods of quantum chemistry

NUCLEAR STRUCTURE 16O; calculated ground and excited states energies. Coupled cluster methods.

doi: 10.1140/epjad/i2005-06-062-8
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2004BE06      Nucl.Phys. A731, 381 (2004)

A.Belic, D.J.Dean, M.Hjorth-Jensen

Pairing correlations and transitions in nuclear systems

doi: 10.1016/j.nuclphysa.2003.11.050
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2004DE21      Phys.Rev. C 69, 054320 (2004)

D.J.Dean, M.Hjorth-Jensen

Coupled-cluster approach to nuclear physics

NUCLEAR STRUCTURE 4He, 16O; calculated ground-state energies. Coupled-cluster approach, no-core G-matrix interaction, many-body perturbation theory.

doi: 10.1103/PhysRevC.69.054320
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2004DE35      Prog.Part.Nucl.Phys. 53, 419 (2004)

D.J.Dean, T.Engeland, M.Hjorth-Jensen, M.P.Kartamyshev, E.Osnes

Effective interactions and the nuclear shell-model

doi: 10.1016/j.ppnp.2004.05.001
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2004GA24      Phys.Rev. C 69, 054307 (2004)

H.Gausemel, B.Fogelberg, T.Engeland, M.Hjorth-Jensen, P.Hoff, H.Mach, K.A.Mezilev, J.P.Omtvedt

Decay of 127In and 129In

RADIOACTIVITY 127,129In(β-) [from 235U(n, F)]; measured Eβ, Eγ, γγ-, βγ-coin following ground-state and isomer decays. 127,129In deduced isomeric states energies, T1/2. 127,129Sn deduced levels, J, π, isomers T1/2. Comparison with shell model predictions.

doi: 10.1103/PhysRevC.69.054307
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2004KO17      Phys.Rev.Lett. 92, 132501 (2004)

K.Kowalski, D.J.Dean, M.Hjorth-Jensen, T.Papenbrock, P.Piecuch

Coupled Cluster Calculations of Ground and Excited States of Nuclei

NUCLEAR STRUCTURE 4He, 16O; calculated ground and excited states energies. Coupled cluster approach.

doi: 10.1103/PhysRevLett.92.132501
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2003BR19      Nucl.Phys. A719, 177c (2003)

B.A.Brown, R.Clement, H.Schatz, J.Giansiracusa, W.A.Richter, M.Hjorth-Jensen, K.-L.Kratz, B.Pfeiffer, W.B.Walters

Nuclear structure theory for the astrophysical rp-process and r-process

NUCLEAR STRUCTURE A=40-80; calculated displacement energies. Z=29-38; calculated one- and two-proton separation energies. 130Cd, 129Ag, 128Pd, 127Rh, 126Ru, 125Tc, 124Mo, 123Nb, 122Zr; calculated level-mixing features, β-decay T1/2.

doi: 10.1016/S0375-9474(03)00914-X
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2003DE13      Rev.Mod.Phys. 75, 607 (2003)

D.J.Dean, M.Hjorth-Jensen

Pairing in nuclear systems: from neutron stars to finite nuclei

doi: 10.1103/RevModPhys.75.607
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2003DI06      Phys.Rev.Lett. 91, 162503 (2003)

I.Dillmann, K.-L.Kratz, A.Wohr, O.Arndt, B.A.Brown, P.Hoff, M.Hjorth-Jensen, U.Koster, A.N.Ostrowski, B.Pfeiffer, D.Seweryniak, J.Shergur, W.B.Walters, and the ISOLDE Collaboration

N = 82 Shell Quenching of the Classical r-Process "Waiting-Point" Nucleus 130Cd

RADIOACTIVITY 130Cd(β-) [from U(n, F)]; measured Eγ, Eβ, γγ-, βγ-coin; deduced Qβ. 130In deduced levels, J, π, configurations, shell quenching. Astrophysical implications discussed. Resonance-ionization laser ion source.

doi: 10.1103/PhysRevLett.91.162503
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2003GU12      Phys.Rev. C 68, 034311 (2003)

M.Guttormsen, R.Chankova, M.Hjorth-Jensen, J.Rekstad, S.Siem, A.Schiller, D.J.Dean

Free energy and criticality in the nucleon pair breaking process

NUCLEAR STRUCTURE 171,172Yb, 166,167Er, 161,162Dy, 148,149Sm; analyzed level densities; deduced Helmholtz free energy, other thermodynamic quantities, continuous nucleon pair breaking.

doi: 10.1103/PhysRevC.68.034311
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2003SC32      Phys.Rev. C 68, 054326 (2003)

A.Schiller, E.Algin, L.A.Bernstein, P.E.Garrett, M.Guttormsen, M.Hjorth-Jensen, C.W.Johnson, G.E.Mitchell, J.Rekstad, S.Siem, A.Voinov, W.Younes

Level densities in 56, 57Fe and 96, 97Mo

NUCLEAR REACTIONS 57Fe, 97Mo(3He, 3He'), (3He, α), E=45 MeV; measured particle spectra, Eγ, Iγ. 56,57Fe, 96,97Mo deduced level densities. Microscopic model, pairing plus random interaction.

doi: 10.1103/PhysRevC.68.054326
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2002EN07      Nucl.Phys. A701, 416c (2002)

T.Engeland, M.Hjorth-Jensen, E.Osnes

Effective Interactions in Medium Heavy Nuclei

NUCLEAR STRUCTURE 116,118,120,122,124,126,128,130Sn, 105,106,107Sb; calculated levels, J, π. Shell model, realistic effective interactions, comparison with data.

doi: 10.1016/S0375-9474(01)01620-7
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2002FO03      Phys.Rev. C65, 044303 (2002)

N.Fotiades, J.A.Cizewski, J.A.Becker, L.A.Bernstein, D.P.McNabb, W.Younes, R.M.Clark, P.Fallon, I.Y.Lee, A.O.Macchiavelli, A.Holt, M.Hjorth-Jensen

High-Spin Excitations in 92, 93, 94, 95Zr

NUCLEAR REACTIONS 173Yb(24Mg, X), E=134.5 MeV; measured Eγ, Iγ, γγ-coin following compound nucleus fission. 92,93,94,95Zr deduced high-spin levels, J, π, configurations. Gammasphere array.

doi: 10.1103/PhysRevC.65.044303
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2002HJ02      Prog.Theor.Phys.(Kyoto), Suppl. 146, 289 (2002)

M.Hjorth-Jensen

Pairing Correlations in Nuclear Systems, from Neutron Stars to Finite Nuclei

doi: 10.1143/PTPS.146.289
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2002LI04      Phys.Rev. C65, 021302 (2002)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu

100Sn Core Excitations in 102In

NUCLEAR REACTIONS 50Cr(58Ni, npα), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 102In deduced levels, possible J, π, configurations. Gammasphere, Microball arrays. Comparison with large-scale shell model calculations.

doi: 10.1103/PhysRevC.65.021302
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2002LI33      Phys.Rev. C65, 051307 (2002)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.H.Yu

Excited States of the Proton Emitter 105Sb

NUCLEAR REACTIONS 50Cr(58Ni, 2np), E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 105Sb deduced levels, possible J, π. Gammasphere, Microball arrays. Comparison with shell model results.

doi: 10.1103/PhysRevC.65.051307
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2002LI45      Phys.Rev. C66, 011302 (2002)

M.Lipoglavsek, C.Baktash, J.Blomqvist, M.P.Carpenter, D.J.Dean, T.Engeland, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, E.Osnes, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.-H.Yu

Breakup of the Doubly Magic 100Sn Core

NUCLEAR REACTIONS 50Cr(58Ni, xnypzα)99Cd/101In, E=225 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin; deduced relative yields. 99Cd, 101In deduced high-spin levels, J, π, configurations, core excitation. Gammasphere, Microball arrays, large-scale shell model calculations.

doi: 10.1103/PhysRevC.66.011302
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2002RE28      Phys.Rev. C66, 024308 (2002)

J.J.Ressler, W.B.Walters, C.N.Davids, D.J.Dean, A.Heinz, M.Hjorth-Jensen, D.Seweryniak, J.Shergur

First observation of 109Te β+ and electron capture decay to levels of 109Sb

RADIOACTIVITY 109Te(β+), (EC) [from 54Fe(58Ni, n2p)]; measured Eγ, Iγ, γγ-coin, T1/2. 109Sb deduced levels, J, π. Comparison with shell model predictions, level systematics in neighboring isotopes.

doi: 10.1103/PhysRevC.66.024308
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2002SC36      Phys.Rev. C66, 024322 (2002)

S.Schiller, M.Guttormsen, M.Hjorth-Jensen, J.Rekstad, S.Siem

Model for pairing phase transition in atomic nuclei

NUCLEAR STRUCTURE 56Mn, 58,59Fe, 104,105,106Pd, 160Tb, 161,162Dy, 234,235U, 238Np; calculated level densities, thermodynamic properties, pairing phase transition features.

doi: 10.1103/PhysRevC.66.024322
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2002SH08      Phys.Rev. C65, 034313 (2002)

J.Shergur, B.A.Brown, V.Fedoseyev, U.Koster, K.L.Kratz, D.Seweryniak, W.B.Walters, A.Wohr, D.Fedorov, M.Hannawald, M.Hjorth-Jensen, V.Mishin, B.Pfeiffer, J.J.Ressler, H.O.U.Fynbo, P.Hoff, H.Mach, T.Nilsson, K.Wilhelmsen-Rolander, H.Simon, A.Bickley, and the ISOLDE Collaboration

β-Decay Studies of 135-137Sn using Selective Resonance Laser Ionization Techniques

RADIOACTIVITY 135,136,137Sn(β-), (β-n) [from U(p, X)]; measured β-delayed neutron spectra, Eγ, Iγ, γγ-coin, T1/2; deduced delayed neutron emission probabilities. 135Sb deduced levels, J, π, β-branching ratio. Resonance laser ionization, mass separator.

RADIOACTIVITY 137Sb(β-), (β-n); estimated T1/2 and %P(n) from extrapolation.

doi: 10.1103/PhysRevC.65.034313
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2001GU11      Phys.Rev. C63, 044301 (2001)

M.Guttormsen, M.Hjorth-Jensen, E.Melby, J.Rekstad, A.Schiller, S.Siem

Entropy of Thermally Excited Particles in Nuclei

NUCLEAR STRUCTURE A=20-250; analyzed level densities; deduced single-particle entropy, related features.

doi: 10.1103/PhysRevC.63.044301
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2001GU23      Phys.Rev. C64, 034319 (2001)

M.Guttormsen, M.Hjorth-Jensen, E.Melby, J.Rekstad, A.Schiller, S.Siem

Heat Capacity and Pairing Transition in Nuclei

NUCLEAR STRUCTURE 162Dy; calculated entropy, heat capacity, other thermodynamic quantities; deduced role of pairing transition. 56Mn, 58,59Fe, 104Rh, 105,106Pd, 160Tb, 161,162Dy, 234Pa, 234,235U; calculated level densities.

doi: 10.1103/PhysRevC.64.034319
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2001LI12      Nucl.Phys. A682, 399c (2001)

M.Lipoglavsek, C.Baktash, M.P.Carpenter, D.J.Dean, C.Fahlander, M.Hjorth-Jensen, R.V.F.Janssens, A.Likar, J.Nyberg, S.D.Paul, A.Piechaczek, D.C.Radford, D.Rudolph, D.Seweryniak, D.G.Sarantites, M.Vencelj, C.H.Yu

First Observation of Excitation Across the 100Sn Core

NUCLEAR REACTIONS 50Cr(58Ni, xnypzα)95Rh/96Pd/97Pd/98Pd/100Pd/98Ag/99Ag/100Ag/101Ag/103Ag/98Cd/99Cd/100Cd/101Cd/102Cd/103Cd/104Cd/101In/102In/103In/104In/105In/102Sn/103Sn/104Sn/105Sn/106Sn/105Sb/106Sb, E=225 MeV; measured γγ-, (charged particle)γ-, (neutron)γ-coin; deduced relative yields. Gammasphere, Microball arrays.

doi: 10.1016/S0375-9474(00)00666-7
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2001SC02      Phys.Rev. C63, 021306 (2001)

A.Schiller, A.Bjerve, M.Guttormsen, M.Hjorth-Jensen, F.Ingebretsen, E.Melby, S.Messelt, J.Rekstad, S.Siem, S.W.Odegard

Critical Temperature for Quenching of Pair Correlations

NUCLEAR REACTIONS 162,163Dy, 172,173Yb(3He, X), E=45 MeV; measured Eα, Eγ, αγ-coin. 161,162Dy, 171,172Yb deduced level density and heat capacity vs excitation energy, critical temperature for phase-transition.

doi: 10.1103/PhysRevC.63.021306
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2001SC36      Yad.Fiz. 64, No 7, 1263 (2001); Phys.Atomic Nuclei 64, 1186 (2001)

A.Schiller, M.Guttormsen, M.Hjorth-Jensen, E.Melby, J.Rekstad, S.Siem

Level Density and Thermal Properties in Rare Earth Nuclei

NUCLEAR REACTIONS 162Dy(3He, 3He'), E=45 MeV; 162,163Dy, 172,173Yb(3He, α), E=45 MeV; measured Eγ, Iγ. 161,162Dy, 171,172Yb deduced level densities, thermodynamic quantities, pygmy resonance strength.

doi: 10.1134/1.1389540
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2001SI21      Phys.Rev. C63, 055501 (2001)

T.Siiskonen, M.Hjorth-Jensen, J.Suhonen

Renormalization of the Weak Hadronic Current in the Nuclear Medium

NUCLEAR STRUCTURE 16O, 40Ca, 56Ni, 100Sn; calculated weak charge-changing hadronic current renormalization.

doi: 10.1103/PhysRevC.63.055501
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2001VI12      Nucl.Phys. A691, 443c (2001)

I.Vidana, A.Polls, A.Ramos, L.Engvik, M.Hjorth-Jensen

Hyperon Effects on the Properties of β-Stable Neutron Star Matter

doi: 10.1016/S0375-9474(01)01071-5
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2000EN02      Phys.Rev. C61, 021302 (2000)

T.Engeland, M.Hjorth-Jensen, E.Osnes

Shell-Model Studies of the Proton Drip Line Nucleus 106Sb

NUCLEAR STRUCTURE 106Sb; calculated levels, J, π, B(E2). Shell model, comparison with data.

doi: 10.1103/PhysRevC.61.021302
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