NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.Lenske Found 171 matches. Showing 1 to 100. [Next]2024AD01 Phys.Rev. C 109, 014602 (2024) G.G.Adamian, N.V.Antonenko, H.Lenske, V.V.Sargsyan Application of a universal reaction function to the description of heavy-ion reaction cross sections
doi: 10.1103/PhysRevC.109.014602
2023CA02 Prog.Part.Nucl.Phys. 128, 103999 (2023) F.Cappuzzello, H.Lenske, M.Cavallaro, C.Agodi, N.Auerbach, J.I.Bellone, R.Bijker, S.Burrello, S.Calabrese, D.Carbone, M.Colonna, G.De Gregorio, J.L.Ferreira, D.Gambacurta, H.Garcia-Tecocoatzi, A.Gargano, J.A.Lay, R.Linares, J.Lubian, E.Santopinto, O.Sgouros, V.Soukeras, A.Spatafora Shedding light on nuclear aspects of neutrinoless double beta decay by heavy-ion double charge exchange reactions
doi: 10.1016/j.ppnp.2022.103999
2023IS05 Phys.Rev. C 108, L051301 (2023) J.Isaak, D.Savran, N.Pietralla, N.Tsoneva, A.Zilges, K.Eberhardt, C.Geppert, C.Gorges, H.Lenske, D.Renisch Direct demonstration of the two-phonon structure of the Jnullp = 1-4742keV
doi: 10.1103/PhysRevC.108.L051301
2023LE16 Eur.Phys.J. A 59, 222 (2023) Interactions of ω mesons in nuclear matter and with nuclei
doi: 10.1140/epja/s10050-023-01129-x
2022AN23 Eur.Phys.J. A 58, 211 (2022) N.V.Antonenko, G.G.Adamian, V.V.Sargsyan, H.Lenske Double-folding nucleus-nucleus interaction potential based on the self-consistent calculations NUCLEAR STRUCTURE 16O, 40,48Ca; calculated self-consistent HFB nucleon-density distributions. NUCLEAR REACTIONS 12C, 16O, 30Si(12C, X), 16O(16O, X), 28Si, 30Si(28Si, X), 30Si, 24Mg(30Si, X), 40Ca(40Ca, X), 48Ca, 36S(48Ca, X), 36S(64Ni, X), E not given; analyzed available data; deduced the centroids of the experimental barrier distributions for self-consistently defined nucleus–nucleus potentials.
doi: 10.1140/epja/s10050-022-00865-w
2022RO11 Phys.Rev. C 106, 014618 (2022) J.L.Rodriguez-Sanchez, J.Benlliure, I.Vidana, H.Lenske, J.Vargas, C.Scheidenberger, H.Alvarez-Pol, J.Atkinson, T.Aumann, Y.Ayyad, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, P.Diaz Fernandez, A.Estrade, H.Geissel, E.Haettner, A.Kelic-Heil, Yu.A.Litvinov, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, Y.K.Tanaka, H.Weick, J.S.Winfield Systematic study of Δ(1232) resonance excitations using single isobaric charge-exchange reactions induced by medium-mass projectiles of Sn NUCLEAR REACTIONS 1H, 12C, Cu, Pb(112Sn, 112In), (112Sn, 112Sb), 1H, C(124Sn, 124Sb), E=1 GeV/nucleon; measured reaction products; deduced total σ, quasielastic and inelastic σ; missing energy spectra. Observed energy shift for the Δ-resonance peak of about 63 ± 5 MeV and quenching of the quasielastic component. Comparison to theoretical predictions using random phase approximation (RPA) with Giessen energy density functional (GiEDF). FRS spectrometer with SIS-18 synchrotron beam (GSI).
doi: 10.1103/PhysRevC.106.014618
2022SA02 Phys.Lett. B 824, 136792 (2022) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, H.Lenske Constraints on the appearance of a maximum in astrophysical S-factor NUCLEAR REACTIONS 12C, 16O, 30Si(12C, X), 16O(16O, X), 28,30Si(28Si, X), (30Si, X), 30Si(24Mg, X), 40Ca(40Ca, X), 48Ca(48Ca, X), (36S, X), 64Ni(36S, X), E not given; analyzed available data; deduced σ, S-factors.
doi: 10.1016/j.physletb.2021.136792
2021AD07 Eur.Phys.J. A 57, 89 (2021) G.G.Adamian, N.V.Antonenko, H.Lenske, L.A.Malov, S.-G.Zhou Self-consistent methods for structure and production of heavy and superheavy nuclei RADIOACTIVITY 295119, 295,297120(α); calculated Q-values, T1/2. Compared with available experimental data.
doi: 10.1140/epja/s10050-021-00375-1
2021LE24 Int.J.Mod.Phys. E30, 2130010 (2021) Theory and applications of nuclear direct reactions
doi: 10.1142/S0218301321300101
2021LE28 Universe 7, 98 (2021) H.Lenske, J.Bellone, M.Colonna, D.Gambacurta Nuclear Matrix Elements for Heavy Ion Sequential Double Charge Exchange Reactions
doi: 10.3390/universe7040098
2021MA47 Phys.Rev. C 104, L011304 (2021) L.A.Malov, G.G.Adamian, N.V.Antonenko, H.Lenske Shaping the archipelago of stability by the competition of proton and neutron shell closures NUCLEAR STRUCTURE Z=112-126, N=170-190; calculated ground-state shell correction energies. 298,300,302,304120; calculated ground-state shell correction energies in the nuclei of α-decay chains. 288Fl, 304120; predicted as doubly-magic nuclei after 208Pb. Self-consistent energy-density functional (EDF) theory plus-HFB theory in the framework of microscopic-macroscopic method. Comparison to other theoretical approaches.
doi: 10.1103/PhysRevC.104.L011304
2021MA82 Phys.Rev. C 104, 064303 (2021) L.A.Malov, G.G.Adamian, N.V.Antonenko, H.Lenske Landscape of the island of stability with self-consistent mean-field potentials NUCLEAR STRUCTURE 272Ds; calculated ratio of density-dependent mass and mass of nucleus for proton and neutrons of the spherical nucleus 272Ds. 288Fl, 292Lv, 300120; calculated energy dependencies of the ground-state level-density parameters using mean-field potentials. 243Cm, 251Cf; calculated energies of low-lying one-quasineutron states using phenomenological Woods-Saxon (WS) potentials. 247Bk, 251Es; calculated energies of low-lying one-quasiproton states using phenomenological Woods-Saxon (WS) potentials. 295119, 291Ts, 287Mc, 283Nh, 279Rg; 297120, 293Og, 289Lv, 285Fl, 281Cn; 295120, 291Og, 287Lv, 283Fl, 279Cn; 299120, 295Og, 291Lv, 287Fl, 283Cn; calculated energies, J, π of low-lying one-quasiproton states for α decay chains of 295119 and 295,297,299120. 295119, 291Ts, 287Mc, 283Nh, 279Rg; 296120, 292Og, 288Lv, 284Fl, 280Cn; 297120, 293Og, 289Lv, 285Fl, 281Cn; 295120, 291Og, 287Lv, 283Fl, 279Cn; 299120, 295Og, 291Lv, 287Fl, 283Cn; 301120, 297Og, 293Lv, 289Fl, 285Cn; 304120, 300Og, 296Lv, 292Fl, 288Cn; calculated ground-state shell correction energies for α decay chains of 295119 and 295,296,297,299,301,304120. 286,290Fl, 296,300120; calculated potential energy surfaces in (β2, β4) planes. Microscopic-macroscopic method to calculate the ground-state shell corrections in superheavy nuclei, incorporating effective nucleon mass from the noncovariant energy-density functionals, with Schrodinger-equivalent central and spin-orbit mean-field potentials. Relevance to island of stability of superheavy nuclei and shape coexistence in superheavy nuclei and effect on spectrum of α decay. Comparison with available experimental data.
doi: 10.1103/PhysRevC.104.064303
2020AD06 Phys.Rev. C 101, 034301 (2020) G.G.Adamian, N.V.Antonenko, H.Lenske, L.A.Malov Predictions of identification and production of new superheavy nuclei with Z=119 and 120 ATOMIC MASSES 275,276,277,278,279,280,281,282Ds, 279,280,281,282,283,284,285,286Cn, 281,282,283,284,285,286,287,288,289,290,291,292Fl, 287,288,289,290,291,292,293,294,295,296Lv, 291,292,293,294,295,296,297,298,299,300,301,302Og, 293,294,295,296,297,298,299,300,301,302120, 279,280,281,282,283Rg, 283,284,285,286,287Nh, 287,288,289,290,291Mc, 291,292,293,294,295Ts, 295,296,297,298,299,300,301119; calculated atomic masses, Q(α). Microscopic-macroscopic method with Woods-Saxon potential extracted from the HFB self-consistent consideration. Comparison with other theoretical calculations. NUCLEAR STRUCTURE 279Rg, 283Nh, 287Mc, 291Ts, 295119, 275,277Ds, 279,281Cn, 283,285Fl, 287,289Lv, 291,293Og, 295,297120; calculated low-lying levels, J, π, ground-state shell corrections, Q(α) for the nuclei of α-decay chains of 295119, 295120, and 297120. Microscopic-macroscopic method with Woods-Saxon potential extracted from the HFB self-consistent consideration. Comparison with experimental values, and with other theoretical calculations. NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 249Cf(48Ca, X), (50Ti, X), 238U, 244Pu, 248Cm, (54Cr, X), 238U, 244Pu(58Fe, X), 238U(64Ni, X), 248,249,250,251Cf(48Ti, X), (50Ti, X), 244,245,246,247,248Cm(54Cr, X), 235,236,237,238U, 247,248,249Bk(50Ti, X), E not given; calculated Q-values, evaporation residue production cross sections of superheavy elements. DNS fusion model.
doi: 10.1103/PhysRevC.101.034301
2020RO12 Phys.Lett. B 807, 135565 (2020) J.L.Rodriguez-Sanchez, J.Benlliure, I.Vidana, H.Lenske, C.Scheidenberger, J.Vargas, H.Alvarez-Pol, J.Atkinson, T.Aumann, Y.Ayyad, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, P.Diaz Fernandez, A.Estrade, H.Geissel, E.Haettner, A.Kelic-Heil, Yu.A.Litvinov, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, Y.K.Tanaka, H.Weick, J.S.Winfield Study of Δ excitations in medium-mass nuclei with peripheral heavy ion charge-exchange reactions NUCLEAR REACTIONS C(112Sn, 112In), E=1 GeV/nucleon; analyzed available data; deduced missing spectra, change in the relative magnitude between the contribution of the excitation of the resonance in the target and in the projectile.
doi: 10.1016/j.physletb.2020.135565
2020RO13 Nucl.Phys. A1002, 121995 (2020) I.S.Rogov, G.G.Adamian, N.V.Antonenko, T.M.Shneidman, H.Lenske Nucleon density distribution in description of nuclear decays NUCLEAR STRUCTURE 44Ti; analyzed available data; calculated spectroscopic factors. RADIOACTIVITY 236,238U(α), (SF); analyzed self-consistently calculated nucleon density distributions; deduced T1/2.
doi: 10.1016/j.nuclphysa.2020.121995
2020SA05 Eur.Phys.J. A 56, 19 (2020) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, H.Lenske Extended quantum diffusion approach to reactions of astrophysical interests
doi: 10.1140/epja/s10050-019-00009-7
2020SO26 Commun. Phys. 11, 3242 (2020) P.-A.Soderstrom, L.Capponi, E.Aciksoz, T.Otsuka, N.Tsoneva, Y.Tsunoda, D.L.Balabanski, N.Pietralla, G.L.Guardo, D.Lattuada, H.Lenske, C.Matei, D.Nichita, A.Pappalardo, T.Petruse Electromagnetic character of the competitive γγ/γ-decay from 137mBa RADIOACTIVITY 137Cs(β-), 137Ba(IT); measured decay products, Eγ, Iγ, γ-γ-coin.; deduced γ-ray energies, widths and nuclear static dipole polarisabilities, angular correlation of the two photons emitted in the double-γ decay, Energy-sharing distribution for the two photons in the double-γ decay, an improved value on the double-photon versus single-photon branching ratio. Comparison with calculations. CeBr3 detectors from ELIGANT, the ELI Gamma Above Neutron Threshold (ELIGANT) detector system.
doi: 10.1038/s41467-020-16787-4
2019LE16 Prog.Part.Nucl.Phys. 109, 103716 (2019) H.Lenske, F.Cappuzzello, M.Cavallaro, M.Colonna Heavy ion charge exchange reactions as probes for nuclear β-decay NUCLEAR REACTIONS 42Ca(48Ti, 49Ti), (48Ti, 49V), (48Ti, 47Ti), (48Ti, 47Sc), E=385 MeV; calculated σ(θ, E). Comparison with experimental data.
doi: 10.1016/j.ppnp.2019.103716
2019LE20 Eur.Phys.J. A 55, 238 (2019) Dissolution of shell structures and the polarizability of dripline nuclei
doi: 10.1140/epja/i2019-12811-6
2019SA65 Acta Phys.Pol. B50, 507 (2019) V.V.Sargsyan, H.Lenske, G.G.Adamian, N.V.Antonenko From Dinuclear Systems to Close Binary Stars: Application to Mass Transfer
doi: 10.5506/aphyspolb.50.507
2019TS06 Nucl.Phys. A990, 183 (2019) N.Tsoneva, M.Spieker, H.Lenske, A.Zilges Fine structure of the pygmy quadrupole resonance in 112, 114Sn
doi: 10.1016/j.nuclphysa.2019.07.008
2018AD02 Nucl.Phys. A970, 22 (2018) G.G.Adamian, N.V.Antonenko, H.Lenske Estimates of production and structure of nuclei with Z = 119 NUCLEAR REACTIONS 246,247,248Cm(51V, γ), (51V, xn), E not given;247,248,249Bk(50Ti, γ), (50Ti, xn), E not given; calculated 295119 hot fusion Q, Qα, evaporation residue σ using TCSM (Two-Center Shell Model), α-decay chain.
doi: 10.1016/j.nuclphysa.2017.11.001
2018AD21 Eur.Phys.J. A 54, 170 (2018) G.G.Adamian, L.A.Malov, N.V.Antonenko, H.Lenske, K.Wang, S.-G.Zhou Incorporating self-consistent single-particle potentials into the microscopic-macroscopic method
doi: 10.1140/epja/i2018-12603-6
2018CA16 Eur.Phys.J. A 54, 72 (2018) F.Cappuzzello, C.Agodi, M.Cavallaro, D.Carbone, S.Tudisco, D.Lo Presti, J.R.B.Oliveira, P.Finocchiaro, M.Colonna, D.Rifuggiato, L.Calabretta, D.Calvo, L.Pandola, L.Acosta, N.Auerbach, J.Bellone, R.Bijker, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, O.Brunasso, S.Burrello, S.Calabrese, A.Calanna, E.R.Chavez-Lomeli, G.D'Agostino, P.N.De Faria, G.De Geronimo, F.Delaunay, N.Deshmukh, J.L.Ferreira, M.Fisichella, A.Foti, G.Gallo, H.Garcia-Tecocoatzi, V.Greco, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, J.A.Lay, F.La Via, H.Lenske, R.Linares, G.Litrico, F.Longhitano, J.Lubian, N.H.Medina, D.R.Mendes, M.Moralles, A.Muoio, A.Pakou, H.Petrascu, F.Pinna, S.Reito, A.D.Russo, G.Russo, G.Santagati, E.Santopinto, R.B.B.Santos, O.Sgouros, M.A.G.da Silveira, S.O.Solakci, G.Souliotis, V.Soukeras, A.Spatafora, D.Torresi, R.Magana Vsevolodovna, A.Yildirim, V.A.B.Zagatto The NUMEN project: NUclear Matrix Elements for Neutrinoless double beta decay
doi: 10.1140/epja/i2018-12509-3
2018LE14 Phys.Rev. C 98, 044620 (2018) H.Lenske, J.I.Bellone, M.Colonna, J.-A.Lay, for the NUMEN Collaboration Theory of single-charge exchange heavy-ion reactions NUCLEAR REACTIONS 40Ca, 116Sn(18O, 18O), (18O, 18F), (18O, X), E=25-950 MeV; calculated total reaction σ(E), elastic scattering differential σ(E, θ), single charge exchange DWBA differential σ(θ, E), differential σ(E), and distortion factors using DWBA calculations; deduced transition form factors for Fermi type non-spin-flip and Gamow-Teller-type spin-flip transitions using a revised approach to the theoretical modeling of nuclear single-charge exchange (SCE) heavy-ion reactions in the framework of DWBA theory. 18O, 40Ca; calculated proton and neutron HFB ground-state densities, QRPA response functions for 18O to 18F and 40Ca to 40K transitions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.044620
2017AD13 Acta Phys.Pol. B48, 441 (2017) G.G.Adamian, N.V.Antonenko, A.N.Bezbakh, R.V.Jolos, L.A.Malov, K.Wang, S.-G.Zhou, H.Lenske Influence of Properties of Superheavy Nuclei on Their α Decays RADIOACTIVITY 288Mc, 291,293Ts(α); calculated α-decay chains, Qα, mass excess, levels, J, π, T1/2 using microscopic-macroscopic approach based on TCSM (Two-Center Shell Model). NUCLEAR STRUCTURE 291Ts, 287Mc, 283Nh, 279Rg, 275Mt, 271Bh, 267Db, 253Lr, 259Md, 293Ts, 289Mc, 285Nh, 281Rg, 277Mt, 273Bh, 269Db, 265Lr, 261Md, 288Mc, 284Nh, 280Rg, 276Mt, 272Bh, 268Db; calculated low-lying one-quasiparticle levels, J, π, Qα, mass excess.284Nh, 288Mc(α); calculated α-decay scheme (288Mc to 284Nh, 284Nh to 280Rg) using TCSM (Two-Center Shell Model).
doi: 10.5506/APhysPolB.48.441
2017AD29 Phys.Rev. C 96, 044310 (2017) G.G.Adamian, N.V.Antonenko, L.A.Malov, H.Lenske Examination of production and properties of 268-271Hs NUCLEAR REACTIONS 249Cf(22Ne, 3n)268Hs, ECN=35.2 MeV; 249Cf(22Ne, 4n)267Hs, ECN=46 MeV; 248Cm(26Mg, 3n)271Hs, ECN=33.4 MeV; 248Cm(26Mg, 4n)270Hs, ECN=44.8 MeV; 248Cm(26Mg, 5n)269Hs, ECN=50.8 MeV; 244Pu(30Si, 3n)271Hs, ECN=33.4 MeV; 244Pu(30Si, 4n)270Hs, ECN=46 MeV; 244Pu(30Si, 5n)269Hs, ECN=51.4 MeV; 238U(36S, 3n)271Hs, ECN=34.6 MeV; 238U(36S, 4n), 270Hs, ECN=43.6 MeV; 238U(36S, 3n)269Hs, ECN=49.6 MeV; 226Ra(48Ca, 3n)271Hs, ECN=32.8 MeV; 226Ra(48Ca, 4n)270Hs, ECN=38.8 MeV; calculated production σ using dinuclear system model (DNS), and compared with available experimental data. NUCLEAR STRUCTURE 245Pu, 249,252,253Fm, 256,257,259No, 260,261,262,263Rf, 264,265,266,267Sg, 268,269,270,271Hs, 272,273Ds, 277Cn; calculated levels, K- and shape isomers, J, π using microscopic-macroscopic model, and compared with experimental values. 248Fm; calculated quadrupole and hexadecapole deformation parameters as function of elongation parameter in the two-center shell model. 269,270,271Hs, 265,266,267Sg, 261,263Rf; calculated potential energy surfaces in the plane of elongation and deformation parameters. RADIOACTIVITY 277Cn, 273Ds, 269,271Hs, 265,267Sg, 261,263Rf, 257No(α); calculated Q(α), T1/2. Comparison with available experimental values.
doi: 10.1103/PhysRevC.96.044310
2017CA01 Phys.Rev.Lett. 118, 012701 (2017) M.Cavallaro, M.De Napoli, F.Cappuzzello, S.E.A.Orrigo, C.Agodi, M.Bondi, D.Carbone, A.Cunsolo, B.Davids, T.Davinson, A.Foti, N.Galinski, R.Kanungo, H.Lenske, C.Ruiz, A.Sanetullaev Investigation of the 10Li shell inversion by neutron continuum transfer reaction NUCLEAR REACTIONS 2H(9Li, p), E=100 MeV; measured reaction products, Ep, Ip; deduced σ(θ), energy levels, J, π, resonance, shell inversion features.
doi: 10.1103/PhysRevLett.118.012701
2017LA01 Nucl.Phys. A957, 450 (2017) Elastic scattering, polarization and absorption of relativistic antiprotons on nuclei NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E at 608 MeV/c; calculated σ(θ). 12C(p-bar, p-bar), E at 608, 800, 1100 MeV/c; calculated polarization, double scattering polarization vs θ. 1H(p-bar, p-bar), E at 679, 1089 MeV/c; calculated polarization vs θ. 12C, 63Cu, 208Pb(p, p), E at 9.92, 18.85 MeV/c;20Ne(p, p), (p-bar, p-bar), E at 10 GeV/c; calculated σ(θ). 12C, 27Al, 63Cu(p-bar, p-bar'), E at 0.1-1000 MeV/c; calculated σ. Glauber model; calculations compared with available data.
doi: 10.1016/j.nuclphysa.2016.10.006
2017LA18 Phys.Lett. B 773, 470 (2017) Distillation of scalar exchange by coherent hypernucleus production in antiproton-nucleus collisions NUCLEAR REACTIONS H(p-bar, X), 40Ar(p-bar, Λ)40Cl E=1.5-20 GeV; analyzed available data; deduced σ and σ(θ) for hypernuclei production.
doi: 10.1016/j.physletb.2017.09.007
2017TO16 Phys.Lett. B 773, 20 (2017) A.P.Tonchev, N.Tsoneva, C.Bhatia, C.W.Arnold, S.Goriely, S.L.Hammond, J.H.Kelley, E.Kwan, H.Lenske, J.Piekarewicz, R.Raut, G.Rusev, T.Shizuma, W.Tornow Pygmy and core polarization dipole modes in 206Pb: Connecting nuclear structure to stellar nucleosynthesis NUCLEAR REACTIONS 208Pb(γ, γ'), E=4.9-8.1 MeV; analyzed available data; deduced a range for the neutron-skin thickness of and a corresponding range for the slope of the symmetry energy, Maxwellian-averaged radiative σ.
doi: 10.1016/j.physletb.2017.07.062
2016AD37 Phys.Rev. C 94, 054309 (2016) G.G.Adamian, N.V.Antonenko, H.Lenske, S.V.Tolokonnikov, E.E.Saperstein Isotopic trends of nuclear surface properties of spherical nuclei NUCLEAR STRUCTURE 48,50,52,54,56,58,60,64,68,72,76,78,80,82,84,86,88Ni; calculated binding energies per nucleon. 58,64Ni; calculated radial distributions of the proton density. 64Ni, 122Sn, 196Pb, 272Ds; calculated nucleon-density distributions. Z=28, N=20-50; Z=82, N=98-126; Z=12, N=11-32; Z=50, N=50-85; Z=110, N=154-190; calculated isotopic dependencies of proton and neutron radii and diffuseness. Partially ab initio method, and the Fayans energy density functional (EDF) method used in calculations. Comparison with available experimental data. NUCLEAR REACTIONS 208Pb(64Ni, X), (32Si, X), (α, X); 58Ni(58Ni, X); calculated nucleus-nucleus potentials defined by the density-dependent NN interaction and nucleon density profiles.
doi: 10.1103/PhysRevC.94.054309
2016DE05 Phys.Rev. C 93, 034311 (2016) V.Derya, N.Tsoneva, T.Aumann, M.Bhike, J.Endres, M.Gooden, A.Hennig, J.Isaak, H.Lenske, B.Loher, N.Pietralla, D.Savran, W.Tornow, V.Werner, A.Zilges Decay of quadrupole-octupole 1- states in 40Ca and 140Ce NUCLEAR REACTIONS 40Ca, 140Ce(polarized γ, γ'), E=3.6, 5.9 MeV; measured Eγ, Iγ, γγ-coin, polarization asymmetry and analyzing powers using high intensity γ-ray Source (HIγS) facility at (TUNL); deduced levels, J, π, B(E1), B(E2). Comparisons with energy density functional (EDF) and quasiparticle-phonon model (QPM) calculations. B(E1) and B(E2) systematics for N=82 isotones of 138Ba, 140Ce, 142Nd, 144Sm.
doi: 10.1103/PhysRevC.93.034311
2016GA26 Nucl.Phys. A954, 308 (2016) T.Gaitanos, Ch.Moustakidis, G.A.Lalazissis, H.Lenske Multi-strangeness production in hadron induced reactions
doi: 10.1016/j.nuclphysa.2016.04.011
2016SA23 Phys.Rev. C 93, 054613 (2016) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, A.Diaz-Torres, P.R.S.Gomes, H.Lenske Experimental elastic and quasi-elastic angular distributions provide transfer probabilities NUCLEAR REACTIONS 206Pb(18O, 16O), E=79 MeV; calculated two-neutron transfer probabilities using experimental data for elastic and quasielastic probabilities in 18O+206Pb and 16O+208Pb reactions. Comparison with experimental data for two-neutron transfer reaction.
doi: 10.1103/PhysRevC.93.054613
2016SH14 Phys.Rev. C 93, 045206 (2016) 2π production in the Giessen coupled-channels model
doi: 10.1103/PhysRevC.93.045206
2016SP01 Phys.Lett. B 752, 102 (2016) M.Spieker, N.Tsoneva, V.Derya, J.Endres, D.Savran, M.N.Harakeh, S.Harissopulos, R.-D.Herzberg, A.Lagoyannis, H.Lenske, N.Pietralla, L.Popescu, M.Scheck, F.Schluter, K.Sonnabend, V.I.Stoica, H.J.Wortche, A.Zilges The pygmy quadrupole resonance and neutron-skin modes in 124Sn NUCLEAR REACTIONS 124Sn(α, α'), E=34 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), B(E2), pygmy quadrupole resonance. Comparison with quasiparticle random-phase approximation calculations.
doi: 10.1016/j.physletb.2015.11.004
2015AD11 Phys.Rev. C 91, 054602 (2015) G.G.Adamian, N.V.Antonenko, H.Lenske Role of the neck degree of freedom in cold fusion reactions NUCLEAR REACTIONS 48Ca, 50Ti, 54Cr, 58Fe, 64,72,78Ni, 70Zn(208Pb, X), E not given; calculated mass parameter and potential energy surface contours, time-dependence of the neck parameter in cold fusion reactions. Two-center shell model. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.054602
2015AD26 Phys.Rev. C 92, 054319 (2015) G.G.Adamian, N.V.Antonenko, H.Lenske Origin of termination of negative-parity bands NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar, 40,42Ca, 44Ti, 54Cr, 62Zn, 74Kr; calculated termination of negative-parity rotational bands built on ground states, lifetimes of E2 transitions and α-cluster decay using α-cluster interpretation. Predicted terminating states.
doi: 10.1103/PhysRevC.92.054319
2015FE03 Phys.Rev. C 91, 034307 (2015) Thermal properties of asymmetric nuclear matter
doi: 10.1103/PhysRevC.91.034307
2015KR04 Phys.Rev. C 91, 044328 (2015) Krishichayan, M.Bhike, W.Tornow, G.Rusev, A.P.Tonchev, N.Tsoneva, H.Lenske Polarized photon scattering off 52Cr Determining the parity of J=1 states NUCLEAR REACTIONS 52Cr(polarized γ, γ'), E=5.21, 5.56, 6.40, 6.50, 7.00, 7.08, 7.19, 7.40, 7.51, 7.74, 7.89, 8.02, 8.11, 8.20, 8.75, 8.95, 9.15, 9.25, 9.36, 9.45 MeV; measured Eγ, Iγ, linear polarization using High Intensity γ-Ray Source (HIγS) facility of TUNL. 52Cr; deduced levels, J, π, B(M1), B(E1), E1 and M1 strength functions, spin-flip M1 resonance structure around 9.1 MeV, fragmentation pattern of the dipole strength below and around the neutron emission threshold, new mode of excitation related to pygmy dipole resonance (PDR). Comparison with calculations using three-phonon quasiparticle phonon model (QPM) with self-consistent energy-density functional theory.
doi: 10.1103/PhysRevC.91.044328
2015PE08 Phys.Rev. C 92, 014330 (2015) L.Pellegri, A.Bracco, N.Tsoneva, R.Avigo, G.Benzoni, N.Blasi, S.Bottoni, F.Camera, S.Ceruti, F.C.L.Crespi, A.Giaz, S.Leoni, H.Lenske, B.Million, A.I.Morales, R.Nicolini, O.Wieland, D.Bazzacco, P.Bednarczyk, B.Birkenbach, M.Ciemala, G.de Angelis, E.Farnea, A.Gadea, A.Gorgen, A.Gottardo, J.Grebosz, R.Isocrate, M.Kmiecik, M.Krzysiek, S.Lunardi, A.Maj, K.Mazurek, D.Mengoni, C.Michelagnoli, D.R.Napoli, F.Recchia, B.Siebeck, S.Siem, C.Ur, J.J.Valiente-Dobon Multitude of 2+ discrete states in 124Sn observed via the (17O, 17O' γ) reaction: Evidence for pygmy quadrupole states NUCLEAR REACTIONS 124Sn(17O, 17O'), E=340 MeV; measured Eγ, Iγ, γ(θ), particle spectra, (17O)γ-coin, inelastic scattering σ using the AGATA array at Tandem-ALPI accelerator complex of INFN-LNL facility. 124Sn; deduced levels, J, π, multipolarity, B(E2) for 2+ states, sum rule strength for the ISGQR. DWBA analysis. Comparison with self-consistent density functional theory and extended QRPA approach describing 2+ states as pygmy quadrupole resonances.
doi: 10.1103/PhysRevC.92.014330
2015SA46 Phys.Rev. C 92, 054620 (2015) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, A.Diaz-Torres, P.R.S.Gomes, H.Lenske Derivation of breakup probabilities of weakly bound nuclei from experimental elastic and quasi-elastic scattering angular distributions NUCLEAR REACTIONS 206Pb(6He, 6He), (6He, 6He'), E=16 MeV; 210Pb(α, α), (α, α'), E=17.71 MeV; devised a simple method and a formula relating the breakup and elastic (quasi-elastic) scattering probabilities; calculated breakup probability for 6He+206Pb reaction, and compared with continuum-discretized coupled-channels (CDCC) calculations.
doi: 10.1103/PhysRevC.92.054620
2015TS01 Phys.Rev. C 91, 044318 (2015) N.Tsoneva, S.Goriely, H.Lenske, R.Schwengner Pygmy resonances and radiative nucleon captures for stellar nucleosynthesis NUCLEAR REACTIONS 86Kr, 88Sr, 90Zr, 92Mo(γ, X), E=4-11 MeV; calculated dipole photoabsorption σ(E), B(E1); 85Kr, 87Sr, 89Y, 91Mo(n, γ), E=0.001-10 MeV; calculated capture σ(E), partial capture σ(E) to a compound nuclear state, Maxwellian-averaged cross sections. 89Zr, 91Mo(n, γ), E=0.001-10 MeV; 89Y(p, γ), E=1.6-6 MeV; predicted theoretical σ(E). Self-consistent energy density functional (EDF)+quasiparticle-random phase-approximation (QRPA) with and without pygmy dipole resonances (PDR), three-phonon EDF+quasiparticle-phonon-model (QPM), Hartree Fock Bogoliubov (HFB)+QRPA calculations based on BSk7 force and implemented in statistical reaction model TALYS code to assess contribution of PDR to radiative capture cross sections. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.044318
2014FE05 Phys.Rev. C 89, 044617 (2014) Particle production in antiproton-induced nuclear reactions
doi: 10.1103/PhysRevC.89.044617
2014OZ03 Phys.Rev. C 90, 024304 (2014) B.Ozel-Tashenov, J.Enders, H.Lenske, A.M.Krumbholz, E.Litvinova, P.von Neumann-Cosel, I.Poltoratska, A.Richter, G.Rusev, D.Savran, N.Tsoneva Low-energy dipole strength in 112, 120Sn NUCLEAR REACTIONS 112Sn(γ, γ'), E(endpoint)=5.5, 7.5, 9.5 MeV bremsstrahlung; 120Sn(γ, γ'), E(endpoint)=7.5, 9.1 MeV bremsstrahlung; measured Eγ, Iγ, γ(θ) using S-DALINAC NRF facility at the TU Darmstadt. 112,120Sn; deduced levels, Γ02/Γ, B(E1), summed B(E1) strengths. Fluctuation analysis of γ spectra for unresolved strength. Comparison with quasiparticle-phonon model, and relativistic time blocking approximations (RQTBA), and previous experimental results.
doi: 10.1103/PhysRevC.90.024304
2014SA70 Phys.Rev. C 90, 064601 (2014) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, A.Diaz-Torres, P.R.S.Gomes, H.Lenske Deriving capture and reaction cross sections from observed quasi-elastic and elastic backscattering NUCLEAR REACTIONS 58Ni(58Ni, 58Ni), (58Ni, 58Ni'), E=86-118 MeV; 74Ge(64Ni, 64Ni), (64Ni, 64Ni'), E=96-120 MeV; 92Mo(α, α), (α, α'), E=13.20, 18.70 MeV; 106,110Cd(α, α), (α, α'), E=15.55, 18.8 MeV; 112Sn(α, α), (α, α'), E=13.90, 18.84 MeV; 120Sn(16O, 16O), (16O, 16O'), E=Vb, Vb+5 MeV, Vb+10 MeV; 144,154Sm(16O, 16O), (16O, 16O'), E=55-80 MeV; 152Sm(16O, 16O), (16O, 16O'), E=58.8, 63.3, 72.4 MeV; 208Pb(6Li, 6Li), (6Li, 6Li'), (7Li, 7Li), (7Li, 7Li'), E=Vb+5 MeV, Vb+10 MeV; 208Pb(16O, 16O), (16O, 16O'), E=65-95 MeV; 208Pb(20Ne, 20Ne), (20Ne, 20Ne'), E=Vb, Vb+5 MeV, Vb+10 MeV; analyzed and proposed methods for extracting differential and integral reaction and capture σ(E, J) from the experimental elastic and quasi-elastic backscattering measurements. Coupled-channels approach.
doi: 10.1103/PhysRevC.90.064601
2014SA75 Eur.Phys.J. A 50, 168 (2014) V.V.Sargsyan, G.G.Adamian, N.V.Antonenko, A.Diaz-Torres, P.R.S.Gomes, H.Lenske Extracting integrated and differential cross sections in low-energy heavy-ion reactions from backscattering measurements NUCLEAR REACTIONS 110Cd, 120Sn(α, x), E=9.5-20 MeV; calculated coupled-reaction channels σ, reaction σ, elastic scattering σ(θ) using backscattering data. 92Mo(α, x), E=10-20 MeV;120Sn(α, x), E=11-30 MeV;208Pb(16O, x), E=67-80 MeV; calculated reaction σ (in the case of 16O also capture σ). Compared with data and other calculations.
doi: 10.1140/epja/i2014-14168-8
2013CA26 Phys.Rev. C 88, 055204 (2013) Coupled-channel analysis of KΣ production on the nucleon up to 2.0 GeV
doi: 10.1103/PhysRevC.88.055204
2013GA37 Nucl.Phys. A914, 405c (2013) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel, A.Obermann In-medium effects on hypernuclear formation NUCLEAR REACTIONS 1H(Λ, Λ), E at 0.1-0.5 GeV/c;1H(Λ, Σ0), E at 0.5-2 GeV/c;1H(Σ-, Σ-), E at 0.12-0.18 GeV/c;1H(Σ-, Λ), (Σ-, Σ0), E at 0.1-0.8 GeV/c;1H(p(bar), Λ), (p-bar, Ξ-bar), E at 2.2-3.2 GeV/c; calculated σ using parameterization. 1n(Σ+, Σ+), E=0-400 MeV;1H(Λ, Λ), E=0-400 MeV; calculated σ using GiBUU (Giessen BUU).
doi: 10.1016/j.nuclphysa.2012.12.124
2013MI27 Phys.Rev. C 88, 064310 (2013) N.Minkov, S.Drenska, K.Drumev, M.Strecker, H.Lenske, W.Scheid Non-yrast spectra of odd-A nuclei in a model of coherent quadrupole-octupole motion NUCLEAR STRUCTURE 151Pm, 157Gd, 223Ra, 239Np, 243Am; calculated levels, J, π, B(E1), B(E2), non-yrast and yrast quasi-parity-doublet bands. Coherent quadrupole and octupole motion (CQOM) reflection-asymmetric model. discussed role of reflection-asymmetric deformed shell model to describe single-particle motion and Coriolis interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.064310
2013RU01 Phys.Rev.Lett. 110, 022503 (2013) G.Rusev, N.Tsoneva, F.Donau, S.Frauendorf, R.Schwengner, A.P.Tonchev, A.S.Adekola, S.L.Hammond, J.H.Kelley, E.Kwan, H.Lenske, W.Tornow, A.Wagner Fine Structure of the Giant M1 Resonance in 90Zr NUCLEAR REACTIONS 90Zr(γ, γ'), E=7-11 MeV; measured reaction products, Eγ, Iγ; deduced dipole excitations, 1+ states, fine structure of the giant M1 resonance, B(M1). Comparison with three-phonon QPM calculations.
doi: 10.1103/PhysRevLett.110.022503
2013SC03 Phys.Rev. C 87, 024306 (2013) R.Schwengner, R.Massarczyk, G.Rusev, N.Tsoneva, D.Bemmerer, R.Beyer, R.Hannaske, A.R.Junghans, J.H.Kelley, E.Kwan, H.Lenske, M.Marta, R.Raut, K.D.Schilling, A.Tonchev, W.Tornow, A.Wagner Pygmy dipole strength in 86Kr and systematics of N=50 isotones NUCLEAR REACTIONS 86Kr(γ, γ'), (polarized γ, γ'), E<11.2 MeV; measured Eγ, Iγ, γγ(θ), widths, azimuthal asymmetry, integrated σ. ELBE accelerator facility at HZDR, and HIγS facility at TUNL. 86Kr; deduced levels, PDR, J, π, branching ratios, photoabsorption σ(E), energy-weighted sums of photoabsorption σ. Comparison of photoabsorption σ with that from (γ, n) reaction. NUCLEAR STRUCTURE 86Kr, 88Sr, 90Zr, 92Mo; calculated neutron skin thickness, B(E1), proton and neutron transition densities using QRPA calculations. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.87.024306
2013SH03 Phys.Rev. C 87, 015201 (2013) η-meson production in the resonance-energy region
doi: 10.1103/PhysRevC.87.015201
2012GA19 Nucl.Phys. A881, 240 (2012) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel Formation of double-Λ hypernuclei at PANDA NUCLEAR REACTIONS 12C, Cu, 165Ho, 197Au, 238U(p-bar, X), E-1.22 GeV; calculated σ, dσ. 64Cu(p-bar, X), (p, X), E=5 GeV; calculated fragment multiplicity, yields, fragment E*, Λ, 2Λ, Ξ- rapidity distribution, dσ, σ.
doi: 10.1016/j.nuclphysa.2011.12.010
2012MI08 Phys.Rev. C 85, 034306 (2012) N.Minkov, S.Drenska, M.Strecker, W.Scheid, H.Lenske Non-yrast nuclear spectra in a model of coherent quadrupole-octupole motion NUCLEAR STRUCTURE 152,154Sm, 154,156,158Gd, 236U, 100Mo; calculated levels, J, π, yrast and non-yrast sequences with alternating parity, B(E1), B(E2), B(E3), density distribution contours, Coherent quadrupole-octupole vibrations and rotations model (CQOM). Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034306
2012NO05 Phys.Rev. C 85, 044312 (2012) C.Nociforo, A.Prochazka, R.Kanungo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, N.Kurz, M.Lantz, H.Lenske, Yu.A.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, I.Szarka, I.Tanihata, H.Weick, M.Winkler One-neutron removal reactions on Al isotopes around the N=20 shell closure NUCLEAR REACTIONS C(33Al, 32Al), (34Al, 33Al), (35Al, 34Al), (36Al, 35Al), [secondary 33,34,35,36Al beams from 9Be(48Ca, X), E=1 GeV/nucleon primary reaction], E=900 MeV/nucleon; measured time of flight, energy loss, longitudinal momentum distribution, one-neutron removal cross sections using FRS at GSI; deduced spectroscopic factors, occupation probabilities, theoretical single-particle cross sections. Momentum analysis within the eikonal model approach. Shell structure, magic numbers. Comparison with USDB, SDPF-M shell model calculations.
doi: 10.1103/PhysRevC.85.044312
2012TS07 J.Phys.:Conf.Ser. 366, 012043 (2012) Investigations of Skin Nuclei in a Density Functional Approach NUCLEAR STRUCTURE 112,120Sn; calculated B(E1) vs E* using QRPA and two- and three-phonon QPM. 104,108,112,116,120,124,132,134Sn; calculated main proton and main neutron 2QP components of the 2+2 states vs mass, sum of B(E2) vs mass using QRPA. Some calculations compared to data.
doi: 10.1088/1742-6596/366/1/012043
2011KA01 Phys.Rev. C 83, 021302 (2011) R.Kanungo, A.Prochazka, W.Horiuchi, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, Y.Utsuno, H.Weick, M.Winkler Matter radii of 32-35Mg NUCLEAR REACTIONS C, H(32Mg, X), (33Mg, X)(34Mg, X)(35Mg, X), E=900 MeV/nucleon, [secondary Mg beams from Be(48Ca, X) primary reaction]; measured interaction cross sections by detecting unreacted Mg particles by Bρ-ΔE-TOF method. 32,33,34,35Mg; deduced matter radii by Glauber model analysis. Comparison with HF and RMF predictions. Neutron skin thickness.
doi: 10.1103/PhysRevC.83.021302
2011KA36 Phys.Rev. C 84, 061304 (2011) R.Kanungo, A.Prochazka, M.Uchida, W.Horiuchi, G.Hagen, T.Papenbrock, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, O.Jensen, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, H.Weick, M.Winkler Exploring the anomaly in the interaction cross section and matter radius of 23O NUCLEAR REACTIONS C(22O, X), (23O, X), [22O, 23O secondary beams from 9Be(48Ca, X), E=1 GeV/nucleon primary reaction], E=900 MeV/nucleon; measured energy loss, time of flight, magnetic rigidity. 22,23O; deduced interaction cross section, matter radii, neutron skin thickness. Glauber model analysis. Comparison with ab initio coupled-cluster theory.
doi: 10.1103/PhysRevC.84.061304
2011LE06 Prog.Part.Nucl.Phys. 66, 368 (2011) H.Lenske, S.E.A.Orrigo, N.Tsoneva Density functional theory for reactions of astrophysical interest NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated electric dipole strength distributions, B(E1), nuclear skin thickness. QRPA results. NUCLEAR REACTIONS 138Ba(γ, X), E<9 mEV; calculated photo-absorption σ. QRPA results.
doi: 10.1016/j.ppnp.2011.01.036
2011TO17 J.Phys.:Conf.Ser. 312, 092058 (2011) A.P.Tonchev, S.L.Hammond, J.H.Kelley, E.Kwan, H.Lenske, R.Raut, G.Rusev, W.Tornow, N.Tsoneva Coarse and Fine Structure of the Pygmy Dipole Resonance NUCLEAR REACTIONS 138Ba(polarized γ, γ), (polarized γ, γ'), E=5.4, 7.2, 8.5 MeV; measured Eγ, Iγ(θ) using HPGe with nuclear resonance fluorescence; deduced σ, M1, E1 asymmetry, GDR, PDR photoabsorption σ, E1 ground-state γ transition strength, resonant-shape; calculated E1, M1 γ transition strength distribution using QPM.
doi: 10.1088/1742-6596/312/9/092058
2010BE27 Nucl.Phys. A839, 51 (2010) A relativistic description of the A(π+, K+)ΛA reaction
doi: 10.1016/j.nuclphysa.2010.03.006
2010GA08 Phys.Rev. C 81, 054316 (2010) T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel Breathing mode in an improved transport approach NUCLEAR STRUCTURE 12C, 100Sn; calculated rms radii, binding energies, neutron and proton density profiles, proton mean-field potentials. 12C, 56Ni, 96Ru, 124,136Sn, 208Pb; calculated rms radii. A=10-210; calculated excitation energies and widths of giant-monopole resonances (GMR).Improved relativistic Boltzmann-Uehling-Uhlenbeck (BUU) transport approach.
doi: 10.1103/PhysRevC.81.054316
2010KA05 Phys.Lett. B 685, 253 (2010) R.Kanungo, C.Nociforo, A.Prochazka, Y.Utsuno, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, T.Otsuka, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, I.Szarka, I.Tanihata, H.Weick, M.Winkler Structure of 33Mg sheds new light on the N=20 island of inversion NUCLEAR REACTIONS C(33Mg, 32Mg), E=898 MeV/nucleon; measured 32Mg fragments using MUSIC setup at GSI, σ, longitudinal momentum distribution. 33Mg; deduced ground state configuration, relevance to 'Island of Inversion'. Monte Carlo shell model (MCSM) calculation with the SDPF-M interaction. 33Mg beam produced in Be(48Ca, X) at 1 GeV/nucleon.
doi: 10.1016/j.physletb.2010.02.008
2010SH04 Phys.Rev. C 81, 015204 (2010) Associated photoproduction of K+ mesons off protons within a coupled-channels K-matrix approach
doi: 10.1103/PhysRevC.81.015204
2010SH14 Phys.Rev. C 82, 015203 (2010) Spin-5/2 fields in hadron physics
doi: 10.1103/PhysRevC.82.015203
2010TO01 Phys.Rev.Lett. 104, 072501 (2010) A.P.Tonchev, S.L.Hammond, J.H.Kelley, E.Kwan, H.Lenske, G.Rusev, W.Tornow, N.Tsoneva Spectral Structure of the Pygmy Dipole Resonance NUCLEAR REACTIONS 138Ba(γ, γ), (γ, γ'), E ≈ below one-neutron separation energy; measured Eγ, Iγ; deduced σ, energy levels, B(E1), B(M1). Comparison with QPM calculations.
doi: 10.1103/PhysRevLett.104.072501
2009GA10 Phys.Lett. B 675, 297 (2009) Formation of hypernuclei in high energy reactions within a covariant transport model
doi: 10.1016/j.physletb.2009.04.038
2009KA14 Phys.Rev.Lett. 102, 152501 (2009) R.Kanungo, C.Nociforo, A.Prochazka, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, T.Otsuka, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, I.Szarka, I.Tanihata, Y.Utsuno, H.Weick, M.Winkler One-Neutron Removal Measurement Reveals 24O as a New Doubly Magic Nucleus NUCLEAR REACTIONS 12C(24O, 23O), E=920 MeV/nucleon; measured fragment spectra. 24O; deduced one neutron removal spectroscopic factor. 23O; deduced level energies.
doi: 10.1103/PhysRevLett.102.152501
2009LE25 Hyperfine Interactions 194, 277 (2009) Antiprotons for nuclear structure research
doi: 10.1007/s10751-009-0079-5
2009OR03 Phys.Lett. B 677, 214 (2009) Pairing resonances and the continuum spectroscopy of 10Li NUCLEAR REACTIONS 9Li(n, n), E=0-5 MeV; calculated σ(E). HFB Gorkov model, pairing correlations in the continuum. NUCLEAR REACTIONS 2H(9Li, 10Li), E=2.36, 20 MeV/nucleon; calculated σ(θ), σ(E). 10Li; deduced resonance energies. DWBA model, transfer to the continuum. Comparison to experimental data.
doi: 10.1016/j.physletb.2009.05.024
2009SH46 Phys.Rev. C 80, 058201 (2009) Gauge-invariant interaction of spin-3/2 resonances
doi: 10.1103/PhysRevC.80.058201
2008SC20 Phys.Rev. C 78, 064314 (2008) R.Schwengner, G.Rusev, N.Tsoneva, N.Benouaret, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, J.Klug, K.Kosev, H.Lenske, C.Nair, K.D.Schilling, A.Wagner Pygmy dipole strength in 90Zr NUCLEAR REACTIONS 90Zr(γ, γ'), E=7.9, 9.0, 13.2 MeV; measured Eγ, Iγ.σ, angular distributions, widths; deduced levels, J, π. Comparisons with calculations for 88Sr, 90Zr.
doi: 10.1103/PhysRevC.78.064314
2008SH13 Phys.Rev. C 77, 052201 (2008) Hypernuclear production by the (γ, K+) reaction within a relativistic model NUCLEAR REACTIONS 16O(γ, K+)16N, E<2 GeV; calculated momentum distributions, σ, levels, J, π for hypernuclei.
doi: 10.1103/PhysRevC.77.052201
2008TS01 Phys.Rev. C 77, 024321 (2008) Pygmy dipole resonances in the tin region NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated nucleon densities, B(E1), energy of first 1- state, configurations, pygmy-dipole resonance strengths, dipole transition densities, dipole energies, cross sections.
doi: 10.1103/PhysRevC.77.024321
2008TS02 J.Phys.(London) G35, 014047 (2008) Low-energy dipole excitations in nuclei at the N = 50, 82 and Z = 50 shell closures as signatures for a neutron skin NUCLEAR STRUCTURE 88Sr, 90Zr, 100,102,106,108,110,112,122,132Sn, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm; Z=50; N=50, 82; calculated one-phonon dipole transition densities, total PDR strength. Hartree-Fock-Bogoljubov (HFB) and quasiparticle-phonon model (QPM).
doi: 10.1088/0954-3899/35/1/014047
2007KO65 Eur.Phys.J. A 33, 291 (2007) Correlations in hypernuclear matter
doi: 10.1140/epja/i2007-10475-5
2007LE07 Phys.Lett. B 647, 82 (2007) Probing matter radii of neutron-rich nuclei by antiproton scattering NUCLEAR REACTIONS 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88Ni(p-bar, X), E=50, 100, 200, 300, 400 MeV; calculated absorption σ. Microscopic optical potential. NUCLEAR STRUCTURE 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88Ni; calculated radii. Microscopic optical potential.
doi: 10.1016/j.physletb.2007.02.009
2007LE13 Prog.Part.Nucl.Phys. 59, 114 (2007) H.Lenske, U.Badarch, P.Konrad, S.E.A.Orrigo, N.Tsoneva Density functional theory for nuclei and hypernuclei
doi: 10.1016/j.ppnp.2006.12.004
2007TS06 Prog.Part.Nucl.Phys. 59, 317 (2007) Pygmy dipole resonance in exotic nuclei NUCLEAR STRUCTURE Sn;N=82; calculated one-phonon dipole transition densities and total PDR strength using a method incorporating both HFB and multi-phonon QPM theory.
doi: 10.1016/j.ppnp.2006.12.030
2006JE02 Phys.Lett. B 635, 17 (2006) H.B.Jeppesen, A.M.Moro, T.Nilsson, F.Ames, P.van den Bergh, U.C.Bergmann, G.Bollen, M.J.G.Borge, J.Cederkall, P.Van Duppen, S.Emhofer, O.Forstner, L.M.Fraile, H.O.U.Fynbo, J.Gomez-Camacho, D.Habs, R.von Hahn, G.Huber, M.Huyse, H.T.Johansson, B.Jonson, O.Kester, H.Lenske, L.Liljeby, M.Meister, G.Nyman, M.Oinonen, M.Pantea, H.Podlech, U.Ratzinger, K.Reisinger, K.G.Rensfelt, R.Repnow, K.Riisager, A.Richter, K.Rudolph, H.Scheit, A.Schempp, P.Schmidt, G.Schrieder, D.Schwalm, T.Sieber, H.Simon, O.Tengblad, E.Tengborn, M.Turrion, L.Weissman, F.Wenander, B.Wolf Investigation of the 9Li + 2H → 8Li + t reaction at REX-ISOLDE NUCLEAR REACTIONS 2H(9Li, 8Li), E=2.36 MeV/nucleon; measured particle spectra, σ(θ). 8Li levels deduced energies, spectroscopic factors. Comparison with optical model calculations, post-accelerated radioactive beam.
doi: 10.1016/j.physletb.2006.02.034
2006NO11 Eur.Phys.J. A 27, Supplement 1, 283 (2006) C.Nociforo, F.Cappuzzello, A.Cunsolo, A.Foti, S.E.A.Orrigo, J.S.Winfield, M.Cavallaro, S.Fortier, D.Beaumel, H.Lenske Exploring the Nα + 3n light nuclei via the (7Li, 7Be) reaction NUCLEAR REACTIONS 11B, 15N, 19F(7Li, 7Be), E ≈ 8 MeV/nucleon; measured excitation energy spectra. 7He, 11Be, 15C, 19O deduced excited states features.
doi: 10.1140/epja/i2006-08-043-4
2006OR02 Phys.Lett. B 633, 469 (2006) S.E.A.Orrigo, H.Lenske, F.Cappuzzello, A.Cunsolo, A.Foti, A.Lazzaro, C.Nociforo, J.S.Winfield Core excited Fano-resonances in exotic nuclei NUCLEAR REACTIONS 14C(n, n), E*=5-12 MeV; calculated σ. 15N(7Li, 7Be), E=55 MeV; analyzed particle spectra, σ(E, θ=14°). 15C deduced resonance energies, widths. Quasiparticle-core coupled model.
doi: 10.1016/j.physletb.2005.12.046
2006SH03 Nucl.Phys. A764, 313 (2006) A relativistic two-nucleon model for A(p, K+ΛB reaction NUCLEAR REACTIONS 1H, 4He, 12C, 40Ca(p, K+), E=0.5-3.0 GeV; calculated hypernucleus production σ(E, θ), intermediate states contributions. Fully covariant two-nucleon model.
doi: 10.1016/j.nuclphysa.2005.09.015
2006VO11 Nucl.Phys. A779, 1 (2006) S.Volz, N.Tsoneva, M.Babilon, M.Elvers, J.Hasper, R.-D.Herzberg, H.Lenske, K.Lindenberg, D.Savran, A.Zilges The photoresponse of stable N = 82 nuclei below 10 MeV NUCLEAR REACTIONS 138Ba(γ, γ'), E=9.2 MeV bremsstrahlung; 140Ce, 142Nd, 144Sm(γ, γ'), E=7.6, 9.9 MeV bremsstrahlung; measured Eγ, Iγ. 138Ba, 140Ce, 142Nd, 144Sm deduced dipole transition energies, B(E1). Comparison with quasiparticle-phonon model predictions.
doi: 10.1016/j.nuclphysa.2006.08.012
2005KO19 Nucl.Phys. A756, 192 (2005) Short range correlations and spectral functions in asymmetric nuclear matter
doi: 10.1016/j.nuclphysa.2005.03.083
2005NO01 Phys.Lett. B 605, 79 (2005) C.Nociforo, K.L.Jones, L.H.Khiem, P.Adrich, T.Aumann, B.V.Carlson, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, J.V.Kratz, R.Kulessa, T.Lange, Y.Leifels, H.Lenske, E.Lubkiewicz, G.Munzenberg, R.Palit, H.Scheit, H.Simon, K.Summerer, S.Typel, E.Wajda, W.Walus, H.Weick, and the LAND-FRS Collaboration Coulomb breakup of 23O NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; measured En, Eγ, Iγ, (fragment)γ-, nγ-coin, σ(E); deduced final-state interaction effects. 23O deduced ground state J, π, configuration, spectroscopic factor.
doi: 10.1016/j.physletb.2004.11.014
2005SH20 Phys.Rev. C 71, 055206 (2005); Erratum Phys.Rev. C 72, 019903 (2005) V.Shklyar, H.Lenske, U.Mosel, G.Penner Coupled-channel analysis of ω-meson production in πN and γN reactions for c.m. energies up to 2 GeV NUCLEAR REACTIONS 1H(π-, X), (γ, X), E(cm) ≈ 1.7-2.1 GeV; analyzed ω-meson production σ, σ(θ); deduced resonance contributions. Coupled-channels effective Lagrangian approach.
doi: 10.1103/PhysRevC.71.055206
2005SH30 Phys.Rev. C 72, 015210 (2005) Coupled-channel analysis of KΛ production in the nucleon resonance region NUCLEAR REACTIONS 1H(π-, K0X), (γ, K+X), E(cm) ≈ 1.6-2 GeV; analyzed hyperon production associated σ, σ(θ), polarization observables, related data; deduced final state resonance couplings. Unitary coupled-channels effective Lagrangian model.
doi: 10.1103/PhysRevC.72.015210
2004CA20 Europhys.Lett. 65, 766 (2004) F.Cappuzzello, S.E.A.Orrigo, A.Cunsolo, H.Lenske, M.C.Allia, D.Beaumel, S.Fortier, A.Foti, A.Lazzaro, C.Nociforo, J.S.Winfield Excited states of 15C NUCLEAR REACTIONS 15N(7Li, 7Be), E=55 MeV; measured σ(E, θ). 15C deduced levels, J, π. Comparison with quasiparticle RPA predictions.
doi: 10.1209/epl/i2003-10197-8
2004CA29 Nucl.Phys. A739, 30 (2004) F.Cappuzzello, H.Lenske, A.Cunsolo, D.Beaumel, S.Fortier, A.Foti, A.Lazzaro, C.Nociforo, S.E.A.Orrigo, J.S.Winfield Analysis of the 11B(7Li, 7Be)11Be reaction at 57 MeV in a microscopic approach NUCLEAR REACTIONS 11B(7Li, 7Be), E=57 MeV; measured particle spectra, σ(E, θ). 11Be deduced levels, configurations. Quasiparticle RPA analysis.
doi: 10.1016/j.nuclphysa.2004.03.221
2004LE17 Prog.Part.Nucl.Phys. 53, 153 (2004) Correlation dynamics in dripline nuclei
doi: 10.1016/j.ppnp.2004.02.020
2004RA21 Nucl.Phys. A744, 108 (2004) E.Ramstrom, H.Lenske, H.H.Wolter A multistep direct reaction approach for neutron-induced reactions at intermediate energy NUCLEAR REACTIONS 56Fe(n, p), E=28-97 MeV; 208Pb(n, p), E=62.7, 96 MeV; calculated response functions, σ(E, θ). Multistep direct reaction approach, comparison with data.
doi: 10.1016/j.nuclphysa.2004.08.021
2004SH23 Phys.Rev. C 69, 065205 (2004) Exclusive K+ production in proton-nucleus collisions NUCLEAR REACTIONS 40Ca(p, K+), E=2.0 GeV; calculated hypernucleus production σ(E, θ), intermediate states contributions. Fully covariant two-nucleon model.
doi: 10.1103/PhysRevC.69.065205
2004TS02 Nucl.Phys. A731, 273 (2004) N.Tsoneva, H.Lenske, Ch.Stoyanov Pygmy Dipole Resonances as a Manifestation of the Structure of the Neutron-Rich Nuclei NUCLEAR STRUCTURE 120,122,124,126,128,130Sn; calculated level energies, B(E1), B(E2), B(E3), pygmy dipole resonance features.
doi: 10.1016/j.nuclphysa.2003.11.038
2004TS03 Phys.Lett. B 586, 213 (2004) N.Tsoneva, H.Lenske, Ch.Stoyanov Probing the nuclear neutron skin by low-energy dipole modes NUCLEAR STRUCTURE 120,122,124,126,128,130,132Sn; calculated level energies, transitions B(Eλ), pygmy dipole resonance features; deduced dependence on neutron skin thickness.
doi: 10.1016/j.physletb.2004.02.024
2003BO38 Nucl.Phys. A722, 3c (2003) H.G.Bohlen, R.Kalpakchieva, W.von Oertzen, T.N.Massey, B.Gebauer, S.M.Grimes, T.Kokalova, H.Lenske, A.Lenz, M.Milin, Ch.Schulz, S.Thummerer, S.Torilov, A.Tumino Structure studies of neutron-rich Beryllium and Carbon isotopes NUCLEAR REACTIONS 9Be(14N, 13N), E=217.9 MeV; 9Be(15N, 12N), E=240 MeV; 9Be(13C, 11C), E=379 MeV; 13C(12C, 9C), E=230.7 MeV; measured particle spectra, σ(E, θ). 10,11,12Be, 16C; deduced levels, J, π.
doi: 10.1016/S0375-9474(03)01327-7
2003BO41 Phys.Rev. C 68, 054606 (2003) H.G.Bohlen, R.Kalpakchieva, B.Gebauer, S.M.Grimes, H.Lenske, K.P.Lieb, T.N.Massey, M.Milin, W.von Oertzen, Ch.Schulz, T.Kokalova, S.Torilov, S.Thummerer Spectroscopy of particle-hole states of 16C NUCLEAR REACTIONS 12,13C(12C, 9C), E=230.7 MeV; measured particle spectra, σ(θ). 15,16C deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.68.054606
2003BO50 Acta Phys.Hung.N.S. 18, 179 (2003) H.G.Bohlen, W.von Oertzen, R.Kalpakchieva, B.Gebauer, S.M.Grimes, T.N.Massey, H.Lenske, A.Lenz, M.Milin, Ch.Schulz, T.Kokalova, S.Torilov, S.Thummerer Structure Studies of Neutron-Rich Beryllium and Carbon Isotopes NUCLEAR REACTIONS 9Be(13C, 11C), E=379 MeV; 9Be(14N, 13N), E=217.9 MeV; 9Be(15N, 12N), E=240 MeV; measured particle spectra. 10,11,12Be deduced rotational bands. 9Be(16O, 14O), E=233.5 MeV; 13C(12C, 14O), E=230.7 MeV; measured σ(E, θ). 11Be deduced levels, J, π. 13C(12C, 9C), E=230.7 MeV; measured particle spectra. 16C deduced levels. Quasiparticle RPA calculations.
doi: 10.1556/APH.18.2003.2-4.10
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