NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = A.T.Kruppa Found 48 matches. 2022KR03 Phys.Rev. C 106, 024303 (2022) A.T.Kruppa, J.Kovacs, P.Salamon, O.Legeza, G.Zarand Entanglement and seniority NUCLEAR STRUCTURE 42,44,46Ca; calculated squared overlap of the configuration interaction (CI) and seniority (SEN) model wave functions as a function of total angular momentum, total correlations and one-body entanglement entropies as a function of total angular momentum for the ground and yrast states. 42,43Ca, 94Ru; calculated mode entropies in the ground and yrast states; analyzed entanglement structure of the open shells of certain semimagic nuclei, and compared with predictions of a single-j shell SEN model. Numerical shell model calculations using an inert core using realistic effective interactions from the G-matrix formalism, and with the density matrix renormalization group method.
doi: 10.1103/PhysRevC.106.024303
2018ID02 Phys.Rev. C 97, 024307 (2018) R.M.Id Betan, A.T.Kruppa, T.Vertse Shadow poles in coupled-channel problems calculated with the Berggren basis NUCLEAR STRUCTURE 5He; calculated locations of the poles of the S matrix for the Cox potential for 3/2+ resonant state of 5He formed in t+d -> α+n fusion reaction using phenomenological two-channel model and Berggren basis for expanding the coupled-channels solutions; deduced shadow pole of 5He migrates between Riemann sheets when the coupling strength is varied.
doi: 10.1103/PhysRevC.97.024307
2017HO27 Phys.Rev. C 96, 064603 (2017) J.Hong, C.A.Bertulani, A.T.Kruppa Neutron removal from the deformed halo nucleus 31Ne NUCLEAR REACTIONS 12C(31Ne, 30Ne), E=230 MeV/nucleon; calculated neutron knockout cross sections and longitudinal momentum distributions as function of deformation using a model to include deformed wave functions and a dynamical knockout formalism that includes the dependence on the nuclear orientation to study the neutron removal. Comparison with experimental data. 31Ne; deduced 3/2- for the deformed halo nucleus.
doi: 10.1103/PhysRevC.96.064603
2014KR01 Phys.Rev. C 89, 014330 (2014) A.T.Kruppa, G.Papadimitriou, W.Nazarewicz, N.Michel Nuclear three-body problem in the complex energy plane: Complex-scaling Slater method NUCLEAR STRUCTURE 6He; calculated total energy, one and two neutron radial and angular densities of ground state and first 2+ resonance. Complex-scaling (CS) approach in the Slater basis, and benchmarking with the complex-energy Gamow shell model (GSM) for bound and unbound states of two-neutron halo nucleus 6He treated as α+n+n cluster system using Minnesota force for two-body interaction, and Tikhonov regularization procedure.
doi: 10.1103/PhysRevC.89.014330
2011PA35 Phys.Rev. C 84, 051304 (2011) G.Papadimitriou, A.T.Kruppa, N.Michel, W.Nazarewicz, M.Ploszajczak, J.Rotureau Charge radii and neutron correlations in helium halo nuclei NUCLEAR STRUCTURE 6,8He; calculated two-neutron GSM density, ground state configurations, rms charge and neutron radii, S(2n) versus rms neutron radius. The Gamow shell model (GSM) with a finite-range modified MN interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.051304
2011PE18 Phys.Rev. C 84, 024311 (2011) J.C.Pei, A.T.Kruppa, W.Nazarewicz Quasiparticle continuum and resonances in the Hartree-Fock-Bogoliubov theory NUCLEAR STRUCTURE 70Zn; calculated continuum contributions, binding energy as a function of low-energy quasiparticle neutron cutoff, Occupation numbers of the discretized neutron quasiparticle continuum states, phase shifts of neutron 1s1/2 state, deep-hole HFB resonance widths and energies. 90Ni; HFB neutron resonance energies and widths, phase shift of the neutron 1p3/2 resonance. 84,86,88,90Ni; calculated continuum contributions. Hartree-Fock-Bogoliubov (HFB) equations, Thomas-Fermi approximation for quasiparticle continuum, HFB resonances and deep-hole states.
doi: 10.1103/PhysRevC.84.024311
2010SA13 Phys.Rev. C 81, 064322 (2010) P.Salamon, A.T.Kruppa, T.Vertse New method for calculating shell correction NUCLEAR STRUCTURE 16,18,20,22,24O, 20Ne, 40,48Ca, 68,78Ni, 90,122,124Zr, 100,132Sn, 146Gd, 180,208Pb; calculated neutron shell corrections using the smoothed finite-range weight function and the generalized Strutinski procedure. Comparison with the semiclassical shell correction.
doi: 10.1103/PhysRevC.81.064322
2010SA20 J.Phys.(London) G37, 105106 (2010) Curvature correction in Strutinsky's method
doi: 10.1088/0954-3899/37/10/105106
2008ID01 Phys.Rev. C 78, 044308 (2008) R.Id Betan, A.T.Kruppa, T.Vertse Complex energy approaches for calculating isobaric analogue states
doi: 10.1103/PhysRevC.78.044308
2008KA16 Phys.Lett. B 664, 52 (2008) M.Karny, K.P.Rykaczewski, R.K.Grzywacz, J.C.Batchelder, C.R.Bingham, C.Goodin, C.J.Gross, J.H.Hamilton, A.Korgul, W.Krolas, S.N.Liddick, K.Li, K.H.Maier, C.Mazzocchi, A.Piechaczek, K.Rykaczewski, D.Schapira, D.Simpson, M.N.Tantawy, J.A.Winger, C.H.Yu, E.F.Zganjar, N.Nikolov, J.Dobaczewski, A.T.Kruppa, W.Nazarewicz, M.V.Stoitsov Shell structure beyond the proton drip line studied via proton emission from deformed 141Ho RADIOACTIVITY 141Ho(p) [from 92Mo(54Fe, X), E=290, 300 MeV]; measured Ep, Ip, T1/2.
doi: 10.1016/j.physletb.2008.04.056
2007KR08 Phys.Rev. C 75, 044602 (2007) Scattering amplitude without an explicit enforcement of boundary conditions NUCLEAR REACTIONS 3H(p, n), E ≈ 1-5 MeV; calculated phase shifts. Standard uniform complex scaling.
doi: 10.1103/PhysRevC.75.044602
2004KR09 Phys.Rev. C 69, 054311 (2004) Gamow and R-matrix approach to proton emitting nuclei NUCLEAR STRUCTURE 141Ho; calculated resonance parameters, level energies and configurations, proton decay T1/2. Triaxial nonadiabatic weak coupling model.
doi: 10.1103/PhysRevC.69.054311
2003KR22 Acta Phys.Pol. B34, 2315 (2003) W.Krolas, R.Grzywacz, K.P.Rykaczewski, J.C.Batchelder, C.R.Bingham, C.J.Gross, D.Fong, J.H.Hamilton, D.J.Hartley, J.K.Hwang, Y.Larochelle, T.A.Lewis, K.H.Maier, J.W.McConnell, A.Piechaczek, A.V.Ramayya, K.Rykaczewski, D.Shapira, M.N.Tantawy, J.A.Winger, C.-H.Yu, E.F.Zganjar, A.T.Kruppa, W.Nazarewicz, T.Vertse First observation of excited states in 140Dy NUCLEAR REACTIONS 92Mo(54Fe, 4n2p), E=315 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin; deduced σ. 140Dy deduced levels, J, π, isomer T1/2. Level systematics in neighboring nuclides discussed.
2002KR04 Phys.Rev. C65, 031303 (2002) W.Krolas, R.Grzywacz, K.P.Rykaczewski, J.C.Batchelder, C.R.Bingham, C.J.Gross, D.Fong, J.H.Hamilton, D.J.Hartley, J.K.Hwang, Y.Larochelle, T.A.Lewis, K.H.Maier, J.W.McConnell, A.Piechaczek, A.V.Ramayya, K.Rykaczewski, D.Shapira, M.N.Tantawy, J.A.Winger, C.-H.Yu, E.F.Zganjar, A.T.Kruppa, W.Nazarewicz, T.Vertse First Observation of the Drip Line Nucleus 140Dy: Identification of a 7 μs K Isomer Populating the Ground State Band NUCLEAR REACTIONS 92Mo(54Fe, 2nα), E=315 MeV; measured delayed Eγ, Iγ, γγ-, (X-ray)γ-, (recoil)γ-coin. 140Dy deduced isomer J, π, T1/2, configuration. Mass separator, comparisons with model predictions. Level systematics in neighboring nuclides discussed. RADIOACTIVITY 141Ho(p); calculated proton decay branching ratios, fine structure features.
doi: 10.1103/PhysRevC.65.031303
2002NA18 Nucl.Phys. A701, 165c (2002) W.Nazarewicz, M.Bender, S.Cwiok, P.H.Heenen, A.T.Kruppa, P.-G.Reinhard, T.Vertse Theoretical Description of Superheavy Nuclei NUCLEAR STRUCTURE 257No, 261Rf, 265Sg, 269Hs, 271Ds, 277Cn; calculated levels, J, π, Qα. Z=120; calculated neutron shell correction energies. Skyrme-Hartree-Fock and relativistic mean-field calculations.
doi: 10.1016/S0375-9474(01)01567-6
2001BA26 Nucl.Phys. A682, 256c (2001) B.Barmore, A.T.Kruppa, W.Nazarewicz, T.Vertse A New Approach to Deformed Proton Emitters: Non-adiabatic coupled-channels
doi: 10.1016/S0375-9474(00)00648-5
2001KR06 Phys.Rev. C63, 044324 (2001) A.T.Kruppa, P.H.Heenen, R.J.Liotta Resonances in the Hartree-Fock BCS Theory NUCLEAR STRUCTURE 42,44Ti, 44,46Cr, 46,48Fe; calculated binding energies, radii. 40Ca, 48Ni; calculated single-particle resonance energies, widths. Hartree-Fock BCS theory.
doi: 10.1103/PhysRevC.63.044324
2001KR10 Phys.Rev. C63, 064301 (2001) Local Realizations of Contact Interactions in Two- and Three-Body Problems NUCLEAR STRUCTURE 2H; calculated binding energy. 11Li; calculated two-neutron separation energy. Two-body contact interactions.
doi: 10.1103/PhysRevC.63.064301
2001SH35 Nucl.Phys. A694, 233 (2001) J.A.Sheikh, A.T.Kruppa, N.Rowley Chaos and Isospin Symmetry Breaking in Rotational Nuclei
doi: 10.1016/S0375-9474(01)00982-4
2000BB02 Phys.Rev. C62, 054315 (2000) B.Barmore, A.T.Kruppa, W.Nazarewicz, T.Vertse Theoretical Description of Deformed Proton Emitters: Nonadiabatic coupled-channel method RADIOACTIVITY 109I, 113Cs, 117La, 131Eu, 141,141mHo(p); calculated proton decay T1/2, branching ratios. Nonadiabatic coupled-channels method, comparison with data.
doi: 10.1103/PhysRevC.62.054315
2000KR03 Phys.Rev. C61, 034313 (2000) A.T.Kruppa, M.Bender, W.Nazarewicz, P.-G.Reinhard, T.Vertse, S.Cwiok Shell Corrections of Superheavy Nuclei in Self-Consistent Calculations NUCLEAR STRUCTURE Z=120; calculated neutron single-particle levels, shell corrections. Z=110-130; calculated proton shell corrections, macroscopic energies. Self-consistent Skyrme-Hartree-Fock and relativistic mean field calculations.
doi: 10.1103/PhysRevC.61.034313
2000KR07 Phys.Rev.Lett. 84, 4549 (2000) A.T.Kruppa, B.Barmore, W.Nazarewicz, T.Vertse Fine Structure in the Decay of Deformed Proton Emitters: Nonadiabatic approach RADIOACTIVITY 131Eu, 141Ho, 141mHo(p); calculated T1/2, ground and first excited state branching ratios. Comparison with data, solution of Schroedinger equation in complex energy plane.
doi: 10.1103/PhysRevLett.84.4549
2000VE03 Phys.Rev. C61, 064317 (2000) T.Vertse, A.T.Kruppa, W.Nazarewicz Shell Corrections for Finite-Depth Deformed Potentials: Green's function oscillator expansion method NUCLEAR STRUCTURE 298Fl, 132,154Sn, 100,110,120Zr; calculated shell corrections, related quantities. Green's function oscillator expansion method, Woods-Saxon potential, generalized Strutinsky smoothing procedure.
doi: 10.1103/PhysRevC.61.064317
1999AR23 Phys.Rev. C60, 064315 (1999) Continuum Level Density in a Microscopic Cluster Model: Parameters of resonances NUCLEAR STRUCTURE 5He, 5Li, 8Be; calculated resonances energies, widths. Cluster model, continuum level density method.
doi: 10.1103/PhysRevC.60.064315
1999HA58 Comput.Phys.Commun. 123, 143 (1999) K.Hagino, N.Rowley, A.T.Kruppa A Program for Coupled-Channel Calculations with All Order Couplings for Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 144Sm(16O, X), E(cm)=55-72 MeV; calculated fusion σ, compound nucleus mean angular momentum. Coupled-channels approach.
doi: 10.1016/S0010-4655(99)00243-X
1999RY04 Phys.Rev. C60, 011301 (1999) K.Rykaczewski, J.C.Batchelder, C.R.Bingham, T.Davinson, T.N.Ginter, C.J.Gross, R.Grzywacz, M.Karny, B.D.MacDonald, J.F.Mas, J.W.McConnell, A.Piechaczek, R.C.Slinger, K.S.Toth, W.B.Walters, P.J.Woods, E.F.Zganjar, B.Barmore, L.Gr.Ixaru, A.T.Kruppa, W.Nazarewicz, M.Rizea, T.Vertse Proton Emitters 140Ho and 141Ho: Probing the structure of unbound Nilsson orbitals NUCLEAR REACTIONS 92Mo(54Fe, xnp)140Ho/141Ho/141mHo, E=315 MeV; measured proton spectra following residual nucleus decay, (recoil)(decay)-coin; deduced production σ. RADIOACTIVITY 140,141mHo(p) [from 92Mo(54Fe, xnp)]; measured Ep, T1/2. 140,141Ho deduced proton resonance features, configurations, deformation effects. Coupled-channels analysis.
doi: 10.1103/PhysRevC.60.011301
1998KR11 Phys.Lett. 431B, 237 (1998) Calculation of the Continuum Level Density
doi: 10.1016/S0370-2693(98)00573-5
1998VE02 Phys.Rev. C57, 3089 (1998) T.Vertse, A.T.Kruppa, R.J.Liotta, W.Nazarewicz, N.Sandulescu, T.R.Werner Shell Corrections for Finite Depth Potentials: Particle continuum effects NUCLEAR STRUCTURE 78Ni, 90,96,104,106,108,110,122Zr, 124Zr, 132Sn, 146Gd, 208Pb, 298Fl; calculated neutron shell correction energies. 48Ni, 90Zr, 100,132Sn, 146Gd, 180,208Pb; calculated proton shell correction energies. 146Gd, 208Pb calculated smoothed level densities. Smoothing procedure with particle continuum contribution.
doi: 10.1103/PhysRevC.57.3089
1997KR10 Phys.Rev.Lett. 79, 2217 (1997) A.T.Kruppa, P.-H.Heenen, H.Flocard, R.J.Liotta Particle-Unstable Nuclei in the Hartree-Fock Theory NUCLEAR STRUCTURE 6,8,10He, 10C, 12,14,16,22,24,26,28O; calculated binding energies. 10He, 12,26,28O; calculated ground state decay widths. Complex scaled Hartree-Fock procedure, Skyrme effective interactions, several parametrizations compared.
doi: 10.1103/PhysRevLett.79.2217
1996ST14 Phys.Rev.Lett. 77, 36 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α Decay of Deformed Actinide Nuclei RADIOACTIVITY 221Fr, 227Pa, 241Am, 253Es(α); calculated α-decay associated anisotropies. Branching ratios data input.
doi: 10.1103/PhysRevLett.77.36
1996ST28 Nucl.Phys. A611, 332 (1996) T.L.Stewart, M.W.Kermode, D.J.Beachey, N.Rowley, I.S.Grant, A.T.Kruppa α-Particle Decay Through a Deformed Barrier RADIOACTIVITY A=220-248; Z=88-96; calculated α-decay associated amplitudes vs phases. 233,229U, 247,257Es, 237Np, 241Pu, 243,245Cm, 249Bk, 249Cf(α); calculated α-decay associated anisotropies, branching ratios in some cases. Eigenchannel formalism, sub-barrier fusion.
doi: 10.1016/S0375-9474(96)00404-6
1995HI05 Nucl.Phys. A583, 135c (1995); Erratum Nucl.Phys. A587, 853 (1995) D.J.Hinde, C.R.Morton, M.Dasgupta, J.R.Leigh, J.P.Lestone, R.C.Lemmon, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa Fusion Barrier Distributions and Fission Anisotropies NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E(cm) ≈ 55-70 MeV; analyzed fusion σ(E). 208Pb(16O, F), (16O, X), E(cm) ≈ 70-85 MeV; measured fission anisotropies, fusion barrier distribution.
doi: 10.1016/0375-9474(94)00647-6
1995KR13 Phys.Rev. C52, 1818 (1995) Chaotic Behavior in the Cranking and Particles-Rotor Models
doi: 10.1103/PhysRevC.52.1818
1994MO24 Phys.Rev.Lett. 72, 4074 (1994) C.R.Morton, M.Dasgupta, D.J.Hinde, J.R.Leigh, R.C.Lemmon, J.P.Lestone, J.C.Mein, J.O.Newton, H.Timmers, N.Rowley, A.T.Kruppa Clear Signatures of Specific Inelastic and Transfer Channels in the Distribution of Fusion Barriers NUCLEAR REACTIONS, ICPND 144Sm(16O, X), (17O, X), E=61-100 MeV; measured fusion σ(E); deduced fusion barrier distribution structure, specific transfer channels signature.
doi: 10.1103/PhysRevLett.72.4074
1993CS02 Phys.Rev.Lett. 70, 1389 (1993) A.Csoto, R.G.Lovas, A.T.Kruppa Two-Pole Structure of the (3/2)+ Resonance of 5He in a Dynamical Microscopic Model NUCLEAR REACTIONS 3H(d, d), E ≤ 150 keV; 4He(n, n), ≤ 6 MeV; analyzed phase shifts. 5He, 5Li deduced 3/2 resonance characteristics. Dynamical microscopic model.
doi: 10.1103/PhysRevLett.70.1389
1993KR01 Phys.Rev. C47, R451 (1993) A.T.Kruppa, M.A.Nagarajan, J.P.Vary Charge Exchange Effects in Elastic Scattering with Radioactive Beams NUCLEAR REACTIONS 13N, 13C(13C, 13C), E(cm)=7.5-10 MeV; calculated σ(θ); deduced effective neutron-proton interaction extraction possibility. Four-body model.
doi: 10.1103/PhysRevC.47.R451
1993KR14 Nucl.Phys. A560, 845 (1993) A.T.Kruppa, P.Romain, M.A.Nagarajan, N.Rowley Effect of Multiphonon Coupling on Heavy-Ion Fusion NUCLEAR REACTIONS 92Zr(32S, 32S), (32S, 32S'), E(cm) ≈ 70-90 MeV; calculated elastic, quasielastic σ(E); deduced multi-phonon channels effect on barrier distribution. Fusion reactions, vibrational coupling effects.
doi: 10.1016/0375-9474(93)90174-V
1993LE01 Phys.Rev. C47, R437 (1993) J.R.Leigh, N.Rowley, R.C.Lemmon, D.J.Hinde, J.O.Newton, J.X.Wei, J.C.Mein, C.R.Morton, S.Kuyucak, A.T.Kruppa Reconciling Deformation Parameters from Fusion with Those from Coulomb Excitation NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-68 MeV; analyzed fusion data. 154Sm deduced deformation parameters consistency with Coulomb excitation fits.
doi: 10.1103/PhysRevC.47.R437
1991KR13 J.Phys.(London) G17, L209 (1991) A.T.Kruppa, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Magnetic Substate Population in Heavy-Ion Inelastic Scattering at Energies Near the Coulomb Barrier NUCLEAR REACTIONS 92Zr(16O, 16O'), E=56 MeV; calculated magnetic substate population probability vs θ, σ(θ); deduced nuclear reorientation coupling role. Coupled-channels method.
doi: 10.1088/0954-3899/17/11/007
1990KR16 Prog.Theor.Phys.(Kyoto) 84, 1145 (1990) Resonances in Complex-Scaled Orthogonality Condition Model of Nuclear Cluster System NUCLEAR REACTIONS 16O(α, α), E not given; calculated potential, resonances, widths. Orthogonality condition model.
doi: 10.1143/ptp/84.6.1145
1990LO14 Nucl.Phys. A516, 325 (1990) R.G.Lovas, A.T.Kruppa, J.B.J.M.Lanen Cluster-Model Interpretation of the 6Li(e, e'p) Reaction NUCLEAR REACTIONS 6Li(e, e'p), E not given; calculated missing energy, momentum distributions. Cluster model.
doi: 10.1016/0375-9474(90)90312-A
1989LA22 Phys.Rev.Lett. 63, 2793 (1989) J.B.J.M.Lanen, R.G.Lovas, A.T.Kruppa, H.P.Blok, J.F.J.van den Brand, R.Ent, E.Jans, G.J.Kramer, L.Lapikas, E.N.M.Quint, G.van der Steenhoven, P.C.Tiemeijer, P.K.A.de Witt Huberts (e, e'p) Study of Triton + Deuteron + Proton Clustering in 6Li NUCLEAR REACTIONS 6Li(e, e'p), E not given; measured momentum distribution, spectral function missing energy dependences. 6Li deduced clustering effects.
doi: 10.1103/PhysRevLett.63.2793
1988KR01 Phys.Rev. C37, 383 (1988) A.T.Kruppa, R.G.Lovas, B.Gyarmati Complex Scaling in the Cluster Model: Resonances in 8Be NUCLEAR STRUCTURE 8Be; calculated resonances, Γ. Resonating group model.
doi: 10.1103/PhysRevC.37.383
1987KR07 Phys.Rev. C36, 327 (1987) A.T.Kruppa, R.Beck, F.Dickmann Electromagnetic Properties of 6Li in a Cluster Model with Breathing Clusters NUCLEAR STRUCTURE 2H; calculated structure function, rms radius, binding energy. 4He; calculated binding energy, rms radius, charge form factor. 6Li; calculated binding energy, rms radius, B(E2), level < E >. Generator coordinate method. NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated charge, magnetic form factors. Microscopic α+d cluster model.
doi: 10.1103/PhysRevC.36.327
1987LO16 Nucl.Phys. A474, 451 (1987) R.G.Lovas, A.T.Kruppa, R.Beck, F.Dickmann Fragmentation Properties of 6Li NUCLEAR REACTIONS 6Li(p, pd), E=670, 590 MeV; 6Li(α, 2α), E=700 MeV; 6Li(p, p3He), E not given; calculated fragmentation strengths. NUCLEAR STRUCTURE 6Li; calculated α+d, t+3He cluster fragmentation amplitudes. 3,2H, 3,4He; calculated rms charge radii, binding energies.
doi: 10.1016/0375-9474(87)90626-9
1986KR12 Phys.Lett. 179B, 317 (1986) A.T.Kruppa, R.G.Lovas, R.Beck, F.Dickmann Breathing Cluster Model for Nuclei of Two s-Wave Clusters NUCLEAR STRUCTURE 5He, 6,7Li, 7,8Be; calculated binding energies. 6Li; calculated charge form factor square, α-d fragmentation strength. Breathing model, two s-wave clusters.
doi: 10.1016/0370-2693(86)90484-3
1984BE37 Phys.Rev. C30, 1044 (1984) R.Beck, F.Dickmann, A.T.Kruppa Cluster Model with Breathing Clusters: Dynamical distortion effects in 6Li NUCLEAR STRUCTURE 6Li; calculated ground state energy, deuteron cluster size. Generator coordinate method.
doi: 10.1103/PhysRevC.30.1044
1984GY01 Nucl.Phys. A417, 393 (1984) B.Gyarmati, A.T.Kruppa, Z.Papp, G.Wolf Single-Particle Resonant States in Deformed Potentials NUCLEAR STRUCTURE 239U; calculated single particle resonances, widths. Deformed potentials, separable expansion method.
doi: 10.1016/0375-9474(84)90404-4
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