NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = A.Zuker Found 86 matches. 2021ZU02 Phys.Rev. C 103, 024322 (2021) Quadrupole dominance in the light Sn and in the Cd isotopes NUCLEAR STRUCTURE 104,106,108,110,112,114,116,118,120,122,124,126,128,130Sn, 102,104,106,108,110,112,114,116,118,120,122,124,126Cd; calculated B(E2) for the first 2+ state using shell-model with a minimally renormalized realistic interaction, supplemented by quasi- and pseudo-SU3 symmetries and Nilsson-SU3 self-consistent calculations, with general monopole Hamiltonian GEMO. Comparison with experimental and evaluated data. Discussed B(E2)(first 4+ to first 2+)/B(E2)(first 2+ to g.s.).
doi: 10.1103/PhysRevC.103.024322
2020SI10 Phys.Lett. B 806, 135474 (2020) M.Siciliano, J.J.Valiente-Dobon, A.Goasduff, F.Nowacki, A.P.Zuker, D.Bazzacco, A.Lopez-Martens, E.Clement, G.Benzoni, T.Braunroth, F.C.L.Crespi, N.Cieplicka-Orynczak, M.Doncel, S.Erturk, G.de France, C.Fransen, A.Gadea, G.Georgiev, A.Goldkuhle, U.Jakobsson, G.Jaworski, P.R.John, I.Kuti, A.Lemasson, T.Marchi, D.Mengoni, C.Michelagnoli, T.Mijatovic, C.Muller-Gatermann, D.R.Napoli, J.Nyberg, M.Palacz, R.M.Perez-Vidal, B.Saygi, D.Sohler, S.Szilner, D.Testov, M.Zielinska, D.Barrientos, B.Birkenbach, H.C.Boston, A.J.Boston, B.Cederwall, J.Collado, D.M.Cullen, P.Desesquelles, C.Domingo-Pardo, J.Dudouet, J.Eberth, F.J.Egea Canet, V.Gonzalez, L.J.Harkness-Brennan, H.Hess, D.S.Judson, A.Jungclaus, W.Korten, M.Labiche, A.Lefevre, S.Leoni, H.Li, A.Maj, R.Menegazzo, B.Million, A.Pullia, F.Recchia, P.Reiter, M.D.Salsac, E.Sanchis, O.Stezowski, Ch.Theisen Pairing-quadrupole interplay in the neutron-deficient tin nuclei: First lifetime measurements of low-lying states in 106, 108Sn NUCLEAR REACTIONS 92Mo(106Cd, X)106Sn/108Sn, E=770 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, lifetimes, B(E2), B(E4). Differential plunger device.
doi: 10.1016/j.physletb.2020.135474
2018BO17 Phys.Rev.Lett. 121, 032502 (2018) A.Boso, S.M.Lenzi, F.Recchia, J.Bonnard, A.P.Zuker, S.Aydin, M.A.Bentley, B.Cederwall, E.Clement, G.de France, A.Di Nitto, A.Dijon, M.Doncel, F.Ghazi Moradi, A.Gadea, A.Gottardo, T.Henry, T.Huyuk, G.Jaworski, P.R.John, K.Juhasz, I.Kuti, B.Melon, D.Mengoni, C.Michelagnoli, V.Modamio, D.R.Napoli, B.M.Nyako, J.Nyberg, M.Palacz, J.Timar, J.J.Valiente-Dobon Neutron Skin Effects in Mirror Energy Differences: The Case of 23Mg-23Na NUCLEAR REACTIONS 12C(16O, nα), (16O, pα), E=60-70 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, mirror energy differences, high-spin states. Comparison with available data.
doi: 10.1103/PhysRevLett.121.032502
2016BO14 Phys.Rev.Lett. 116, 212501 (2016) J.Bonnard, S.M.Lenzi, A.P.Zuker Neutron Skins and Halo Orbits in the sd and pf Shells NUCLEAR STRUCTURE 48Ca, 68Ni, 120Sn, 208Pb; calculated nuclear radii, neutron skin, halo orbits.
doi: 10.1103/PhysRevLett.116.212501
2015ZU02 Phys.Rev. C 92, 024320 (2015) A.P.Zuker, A.Poves, F.Nowacki, S.M.Lenzi Nilsson-SU3 self-consistency in heavy N=Z nuclei NUCLEAR STRUCTURE 28Si, 60Zn, 64Ge, 68Se, 72Kr, 80Zr, 84Mo, 88Ru, 92Pd, 96Cd; calculated energies, B(E2), intrinsic quadrupole moments of low-lying positive-parity states up to 8+ for N=Z nuclei using shell model. Nilsson-SU3 self-consistency, quasi and pseudo-SU3 quadrupole moments. Coexistence of prolate and oblate deformations in 72Kr and 84Mo.
doi: 10.1103/PhysRevC.92.024320
2012GO19 Phys.Rev.Lett. 109, 162502 (2012) A.Gottardo, J.J.Valiente-Dobon, G.Benzoni, R.Nicolini, A.Gadea, S.Lunardi, P.Boutachkov, A.M.Bruce, M.Gorska, J.Grebosz, S.Pietri, Zs.Podolyak, M.Pfutzner, P.H.Regan, H.Weick, J.Alcantara Nunez, A.Algora, N.Al-Dahan, G.de Angelis, Y.Ayyad, N.Alkhomashi, P.R.P.Allegro, D.Bazzacco, J.Benlliure, M.Bowry, A.Bracco, M.Bunce, F.Camera, E.Casarejos, M.L.Cortes, F.C.L.Crespi, A.Corsi, A.M.D.Bacelar, A.Y.Deo, C.Domingo-Pardo, M.Doncel, Zs.Dombradi, T.Engert, K.Eppinger, G.F.Farrelly, F.Farinon, E.Farnea, H.Geissel, J.Gerl, N.Goel, E.Gregor, T.Habermann, R.Hoischen, R.Janik, S.Klupp, I.Kojouharov, N.Kurz, S.M.Lenzi, S.Leoni, Mandal, R.Menegazzo, D.Mengoni, B.Million, A.I.Morales, D.R.Napoli, F.Naqvi, C.Nociforo, A.Prochazka, W.Prokopowicz, F.Recchia, R.V.Ribas, M.W.Reed, D.Rudolph, E.Sahin, H.Schaffner, A.Sharma, B.Sitar, D.Siwal, K.Steiger, P.Strmen, T.P.D.Swan, I.Szarka, C.A.Ur, P.M.Walker, O.Wieland, H-J.Wollersheim, F.Nowacki, E.Maglione, A.P.Zuker New Isomers in the Full Seniority Scheme of Neutron-Rich Lead Isotopes: The Role of Effective Three-Body Forces NUCLEAR REACTIONS Be(238U, X)210Pb/212Pb/214Pb/216Pb, E=1 GeV/nucleon; measured reaction products, Eγ, Iγ; deduced level schemes, J, π, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.109.162502
2010ME12 Nucl.Phys. A843, 14 (2010) J.Mendoza-Temis, J.G.Hirsch, A.P.Zuker The anatomy of the simplest Duflo-Zuker mass formula ATOMIC MASSES Z=8-108; A=16-256; analyzed masses using DZ10 model. Comparison with other models and data.
doi: 10.1016/j.nuclphysa.2010.05.055
2007DE14 Phys.Rev. C 75, 034317 (2007) F.Della Vedova, S.M.Lenzi, M.Ionescu-Bujor, N.Marginean, M.Axiotis, D.Bazzacco, A.M.Bizzeti-Sona, P.G.Bizzeti, A.Bracco, F.Brandolini, D.Bucurescu, E.Farnea, A.Iordachescu, S.Lunardi, T.Martinez, P.Mason, R.Menegazzo, B.Million, D.R.Napoli, M.Nespolo, P.Pavan, C.Rossi Alvarez, C.A.Ur, R.Venturelli, A.P.Zuker Isospin symmetry breaking at high spin in the mirror nuclei 35Ar and 35Cl NUCLEAR REACTIONS 24Mg(16O, nα), (16O, pα), E=70 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 35Ar, 35Cl deduced high-spin levels, J, π, configurations, analog states, spin-orbit interaction effects, isospin symmetry features. GASP, ISIS arrays.
doi: 10.1103/PhysRevC.75.034317
2006GA33 Phys.Rev.Lett. 97, 152501 (2006) A.Gadea, S.M.Lenzi, S.Lunardi, N.Marginean, A.P.Zuker, G.de Angelis, M.Axiotis, T.Martinez, D.R.Napoli, E.Farnea, R.Menegazzo, P.Pavan, C.A.Ur, D.Bazzacco, R.Venturelli, P.Kleinheinz, P.Bednarczyk, D.Curien, O.Dorvaux, J.Nyberg, H.Grawe, M.Gorska, M.Palacz, K.Lagergren, L.Milechina, J.Ekman, D.Rudolph, C.Andreoiu, M.A.Bentley, W.Gelletly, B.Rubio, A.Algora, E.Nacher, L.Caballero, M.Trotta, M.Moszynski Observation of 54Ni: Cross-Conjugate Symmetry in f7/2 Mirror Energy Differences NUCLEAR REACTIONS 24Mg(32S, 2n), E=75 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 54Ni deduced levels, J, π. Euroball IV, Euclides arrays. Level systematics in neighboring isobars discussed.
doi: 10.1103/PhysRevLett.97.152501
2006HI14 Phys.Scr. T125, 158 (2006) J.G.Hirsch, V.Velazquez, A.Frank, J.Barea, P.Van Isacker, A.P.Zuker An upper limit of ground-state energy fluctuations in nuclear masses
doi: 10.1088/0031-8949/2006/T125/036
2006SC29 Phys.Rev.C 74, 061302 (2006) Shell-model phenomenology of low-momentum interactions NUCLEAR STRUCTURE 39,41,47,49Ca, 49Sc, 57Ni; calculated single-particle level energies. Low-momentum interactions, G matrices.
doi: 10.1103/PhysRevC.74.061302
2005CA39 Rev.Mod.Phys. 77, 427 (2005) E.Caurier, G.Martinez-Pinedo, F.Nowacki, A.Poves, A.P.Zuker The shell model as a unified view of nuclear structure
doi: 10.1103/RevModPhys.77.427
2005MO19 Phys.Rev. C 71, 064317 (2005) R.A.Molina, A.P.Zuker, A.Relano, J.Retamosa Spectral statistics of Hamiltonian matrices in tridiagonal form
doi: 10.1103/PhysRevC.71.064317
2004EK01 Phys.Rev.Lett. 92, 132502 (2004) J.Ekman, D.Rudolph, C.Fahlander, A.P.Zuker, M.A.Bentley, S.M.Lenzi, C.Andreoiu, M.Axiotis, G.de Angelis, E.Farnea, A.Gadea, Th.Kroll, N.Marginean, T.Martinez, M.N.Mineva, C.Rossi-Alvarez, C.A.Ur Unusual Isospin-Breaking and Isospin-Mixing Effects in the A = 35 Mirror Nuclei NUCLEAR REACTIONS 16O(24Mg, nα), (24Mg, pα), E=60 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 35Ar deduced levels, J, π, isospin mixing. GASP, ISIS arrays.
doi: 10.1103/PhysRevLett.92.132502
2004PO09 Eur.Phys.J. A 20, 119 (2004) A.Poves, E.Caurier, F.Nowacki, A.Zuker Spherical shell model description of deformation and superdeformation NUCLEAR STRUCTURE 36Ar, 40Ca; calculated superdeformed bands transition energies vs spin, B(E2), quadrupole moments. Large-scale shell model calculations, comparison with data.
doi: 10.1140/epja/i2002-10336-9
2004ZU01 Int.J.Mod.Phys. E13, 53 (2004) Shell formation and three-body forces
doi: 10.1142/S0218301304001722
2003VE01 Phys.Rev. C 67, 034311 (2003) V.Velazquez, J.G.Hirsch, A.Frank, A.P.Zuker A study of randomness, correlations, and collectivity in the nuclear shell model NUCLEAR STRUCTURE 24Mg, 44Ti, 48Cr; calculated levels, J, π, B(E2), rotational bands. Comparison of random and collective behavior.
doi: 10.1103/PhysRevC.67.034311
2003ZU01 Phys.Rev.Lett. 90, 042502 (2003) Three-Body Monopole Corrections to Realistic Interactions NUCLEAR STRUCTURE 10B, 22,23Na, 24Mg, 27,28Si, 48Cr; calculated level energies, J, contribution from three-body monopole term.
doi: 10.1103/PhysRevLett.90.042502
2002DU20 Phys.Rev. C 66, 051304 (2002) Mirror displacement energies and neutron skins NUCLEAR STRUCTURE A=6-250; analyzed radii, Coulomb displacement energies; deduced neutron skin parameters.
doi: 10.1103/PhysRevC.66.051304
2002VE01 Phys.Rev.Lett. 88, 072502 (2002) Spectroscopy with Random and Displaced Random Ensembles NUCLEAR STRUCTURE 48Ca, 44,46Ti, 48Cr; calculated probability densities for level energy ratios, B(E2), collectivity features. Two-body random ensemble.
doi: 10.1103/PhysRevLett.88.072502
2002ZU04 Phys.Rev.Lett. 89, 142502 (2002) A.P.Zuker, S.M.Lenzi, G.Martinez-Pinedo, A.Poves Isobaric Multiplet Yrast Energies and Isospin Nonconserving Forces NUCLEAR STRUCTURE 47V, 47,49,50Cr, 49,51Mn, 50,51Fe; analyzed rotational bands energy differences; deduced role of isospin nonconserving forces.
doi: 10.1103/PhysRevLett.89.142502
2001LE31 Phys.Rev.Lett. 87, 122501 (2001) S.M.Lenzi, N.Marginean, D.R.Napoli, C.A.Ur, A.P.Zuker, G.de Angelis, A.Algora, M.Axiotis, D.Bazzacco, N.Belcari, M.A.Bentley, P.G.Bizzeti, A.Bizzeti-Sona, F.Brandolini, P.von Brentano, D.Bucurescu, J.A.Cameron, C.Chandler, M.De Poli, A.Dewald, H.Eberth, E.Farnea, A.Gadea, J.Garces-Narro, W.Gelletly, H.Grawe, R.Isocrate, D.T.Joss, C.A.Kalfas, T.Klug, T.Lampman, S.Lunardi, T.Martinez, G.Martinez-Pinedo, R.Menegazzo, J.Nyberg, Zs.Podolyak, A.Poves, R.V.Ribas, C.Rossi Alvarez, B.Rubio, J.Sanchez-Solano, P.Spolaore, T.Steinhardt, O.Thelen, D.Tonev, A.Vitturi, W.von Oertzen, M.Weiszflog Coulomb Energy Differences in T = 1 Mirror Rotational Bands in 50Fe and 50Cr NUCLEAR REACTIONS 28Si(28Si, 2nα), (28Si, 2pα), E=110 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 50Fe, 50Cr deduced high-spin levels, J, π, Coulomb energy differences. Euroball, ISIS arrays. Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.87.122501
2001ZU01 Phys.Rev. C64, 021303 (2001) Binomial Level Densities NUCLEAR STRUCTURE 55Mn, 56Fe, 60Ni; calculated level densities vs excitation energy. Continuous binomial function, comparison with data.
doi: 10.1103/PhysRevC.64.021303
2001ZU02 Phys.Rev. C64, 021304 (2001) A.P.Zuker, L.Waha Ndeuna, F.Nowacki, E.Caurier Canonical Form of Hamiltonian Matrices NUCLEAR STRUCTURE 48Sc, 48Ca; calculated matrix elements.
doi: 10.1103/PhysRevC.64.021304
2000ZU02 Phys.Scr. T88, 157 (2000) Monopole, Quadrupole and Pairing: A shell model view
doi: 10.1238/Physica.Topical.088a00157
1999CA12 Phys.Rev. C59, 2033 (1999) E.Caurier, G.Martinez-Pinedo, F.Nowacki, A.Poves, J.Retamosa, A.P.Zuker Full 0(h-bar)ω Shell Model Calculation of the Binding Energies of the 1f7/2 Nuclei NUCLEAR STRUCTURE 42,43,44,45,46,47,48Ca, 42,43,44,45,46,47,48,49Sc, 42,43,44,45,46,47,48,49,50Ti, 43,44,45,46,47,48,49,50,51V, 44,45,46,47,48,49,50,51,52Cr, 45,46,47,48,49,50,51Mn, 46,47,48,49,50,51,52,54Fe, 48,49,50,51,54Co, 50,51,52,54,56Ni; calculated binding energies, M1, E2, Gamow-Teller sum rules. Shell model, quasispin formalism.
doi: 10.1103/PhysRevC.59.2033
1999CA60 Nucl.Phys. (Supplement) A654, 747c (1999) E.Caurier, F.Nowacki, A.P.Zuker, G.Martinez-Pinedo, A.Poves, J.Retamosa Large Scale Diagonalizations in the pf Shell: Achievements and perspectives NUCLEAR STRUCTURE 48,50Cr; calculated levels, J, π. Shell model, comparison with data and with Hartree-Fock-Bogolyubov results. 58,60Ni; calculated level densities vs excitation energy. Shell model, comparison with data.
doi: 10.1016/S0375-9474(00)88541-3
1999DE07 Phys.Rev. C59, 2474 (1999) D.J.Dean, M.T.Ressell, M.Hjorth-Jensen, S.E.Koonin, K.Langanke, A.P.Zuker Shell-Model Monte Carlo Studies of Neutron-Rich Nuclei in the 1s-0d-1p-0f Shells NUCLEAR STRUCTURE 22,32Mg, 20Ne, 36,46Ar, 40,42,44S, 42Si, 44Ti; calculated binding energies, levels J, π, B(E2), Gamow-Teller strength, configurations. Shell model Monte Carlo calculations.
doi: 10.1103/PhysRevC.59.2474
1999DU05 Phys.Rev. C59, R2347 (1999) The Nuclear Monopole Hamiltonian NUCLEAR STRUCTURE 39,41,47,49Ca, 47K, 49Sc, 15,17,21,23O, 21N, 23F, 27,29,33,35,41,43Si, 33,41Al, 35,43P, 55,57,67,69,77,79Ni, 67,77Co, 69,79Cu, 79,81,89,91Zr, 89Y, 91Nb, 99,101,131,133Sn, 131In, 133Sb, 207Tl, 207,209Pb, 209Bi; calculated single-particle orbits. 12,14C, 16,22,28O, 18,34,42Si, 40,48Ca, 56,68,78Ni, 80,90Zr, 100,132Sn, 208Pb; calculated shell gaps. Monopole Hamiltonian.
doi: 10.1103/PhysRevC.59.R2347
1997MA01 Phys.Rev. C55, 187 (1997) G.Martinez-Pinedo, A.P.Zuker, A.Poves, E.Caurier Full pf Shell Study of A = 47 and A = 49 Nuclei NUCLEAR STRUCTURE 49Ca, 49Sc, 49Ti, 49V, 49Cr; calculated levels, B(λ), μ, binding energies, quadrupole moment, β-decay T1/2. 47Ca, 47Sc, 47V, 47Cr, 47Mn, 47Fe; calculated β-decay T1/2, levels, intrinsic quadrupole moments, g-factors, B(λ) ratios in some cases. Shell model approach.
doi: 10.1103/PhysRevC.55.187
1996DU13 Phys.Rev. C54, 1641 (1996) Realistic Collective Nuclear Hamiltonian NUCLEAR STRUCTURE A=18-38; analyzed level spectra predictions; deduced different realistic interactions similarity.
doi: 10.1103/PhysRevC.54.1641
1996MA17 Phys.Rev. C53, R2602 (1996) G.Martinez-Pinedo, A.Poves, E.Caurier, A.P.Zuker Effective g(A) in the pf Shell RADIOACTIVITY A=41-50; calculated β-decay associated Gamow-Teller matrix elements; deduced average quenching factor.
doi: 10.1103/PhysRevC.53.R2602
1996MA56 Phys.Rev. C54, R2150 (1996) G.Martinez-Pinedo, A.Poves, L.M.Robledo, E.Caurier, F.Nowacki, J.Retamosa, A.Zuker Backbending in 50Cr NUCLEAR STRUCTURE 50Cr; analyzed collective yrast, high-spin states; deduced backbending features. Spherical shell model, cranked HFB method.
doi: 10.1103/PhysRevC.54.R2150
1995CA08 Phys.Rev.Lett. 74, 1517 (1995) Missing and Quenched Gamow-Teller Strength NUCLEAR REACTIONS 48Ca(p, n), E not given; calculated Gamow-Teller transition strength; deduced missing strength, quenching related features, correlations role.
doi: 10.1103/PhysRevLett.74.1517
1995CA31 Phys.Rev. C52, R1736 (1995) E.Caurier, G.Martinez-Pinedo, A.Poves, A.P.Zuker Gamow-Teller Strength in 54Fe and 56Fe NUCLEAR REACTIONS 54,56Fe(p, n), (n, p), E not given; calculated Gamow-Teller transition strength. Large scale shell model.
doi: 10.1103/PhysRevC.52.R1736
1995CA33 Phys.Rev.Lett. 75, 2466 (1995) E.Caurier, J.L.Egido, G.Martinez-Pinedo, A.Poves, J.Retamosa, L.M.Robledo, A.P.Zuker Intrinsic vs Laboratory Frame Description of the Deformed Nucleus 48Cr NUCLEAR STRUCTURE 48Cr; calculated levels, g vs spin, B(E2), intrinsic quadrupole moment. Spherical shell model, HFB method.
doi: 10.1103/PhysRevLett.75.2466
1995DU06 Phys.Rev. C52, R23 (1995) Microscopic Mass Formulas NUCLEAR STRUCTURE Z ≥ 8; N ≥ 8; analyzed binding energies; deduced parameters, rms errors. General scaling arguments based mass formulas.
doi: 10.1103/PhysRevC.52.R23
1995ZU02 Phys.Rev. C52, R1741 (1995) A.P.Zuker, J.Retamosa, A.Poves, E.Caurier Spherical Shell Model Description of Rotational Motion NUCLEAR STRUCTURE 152,154,156,158Nd, 154,156,158,160Sm, 156,158,160,162Gd, 158,160,162,164Dy; calculated B(E2). Spherical shell model.
doi: 10.1103/PhysRevC.52.R1741
1994CA21 Phys.Rev. C50, 225 (1994) E.Caurier, A.P.Zuker, A.Poves, G.Martinez-Pinedo Full pf Shell Model Study of A = 48 Nuclei NUCLEAR STRUCTURE 48Ca, 48Sc, 48Ti, 48V, 48Cr, 48Mn; calculated levels, B(λ), Gamow-Teller strength functions. 48Fe deduced binding energy. Full pf shell model study.
doi: 10.1103/PhysRevC.50.225
1994ZU06 Nucl.Phys. A576, 65 (1994) On the Microscopic Derivation of a Mass Formula NUCLEAR STRUCTURE Z > 20; N > 20; calculated Coulomb corrected 2 proton-2 neutron separation energies. General microscopic mass formula.
doi: 10.1016/0375-9474(94)90738-2
1991AB07 Phys.Rev.Lett. 66, 1134 (1991) A.Abzouzi, E.Caurier, A.P.Zuker Influence of Saturation Properties on Shell-Model Calculations NUCLEAR STRUCTURE N=50, 82; Z=28; analyzed radii, spectroscopic data; deduced monopole field role in saturation. Shell model.
doi: 10.1103/PhysRevLett.66.1134
1991CA07 Phys.Lett. 256B, 301 (1991) Spin Quenching and Orbital Enhancement in the Ti Isotopes NUCLEAR STRUCTURE 44,45,46,47,48Ti; calculated spin, M1 transition strength functions; deduced intruder states features. Exact shell model.
doi: 10.1016/0370-2693(91)91765-N
1990CA42 Phys.Lett. 252B, 13 (1990) A Full 0(h-bar x Omega) Description of the 2νββ Decay of 48Ca RADIOACTIVITY 48Ca(2β); calculated 2β-decay T1/2, Gamow-Teller transition amplitude. 48Ti, 48Ca; calculated Gamow-Teller β-decay strength function. Shell model.
doi: 10.1016/0370-2693(90)91071-I
1988DU14 At.Data Nucl.Data Tables 39, 205 (1988) G.Dussel, E.Caurier, A.P.Zuker Mass Predictions Based on α-Line Systematics NUCLEAR STRUCTURE N ≤ 152; compiled 4-nucleon separation energies; deduced masses.
doi: 10.1016/0092-640X(88)90021-6
1982CO13 Phys.Lett. 115B, 1 (1982) Transition between Random and Collective Behaviour in Spectra Generated by Two-Body Forces NUCLEAR STRUCTURE 20Ne; calculated levels, rotational band; deduced random to collective behavior transition. Monte Carlo calculations, gaussian orthogonal ensemble.
doi: 10.1016/0370-2693(82)90502-0
1980CA19 Phys.Lett. B96, 11 (1980) Hartree-Fock Versus Isospin Projected Hartree-Fock in Nuclei with Neutron Excess NUCLEAR STRUCTURE 40,41,48Ca calculated levels, neutron, proton radii, isospin mixing. Isospin projected Hartree-Fock method.
doi: 10.1016/0370-2693(80)90200-2
1980CA20 Phys.Lett. B96, 15 (1980) Isotope Shifts and Coulomb Displacement Energies in Calcium Isotopes NUCLEAR STRUCTURE 41,42,43,44,45,46,47,48Ca; calculated isotope shift, neutron-proton radii differences, Coulomb displacement energies. Core polarization, effective force, isospin projected Hartree-Fock.
doi: 10.1016/0370-2693(80)90201-4
1979CO09 Phys.Lett. 84B, 25 (1979) Self-Consistency and Many-Body Monopole Forces in Shell Model Calculations NUCLEAR STRUCTURE 18,19O, 18,19F, 20,21,22Ne, 22Na, 24Mg, 28Si, 32S, 34,35,36Cl, 36,37,38Ar, 38K, 39,40Ca; calculated binding energies. Many-body monopole forces, self-consistent shell model.
doi: 10.1016/0370-2693(79)90641-5
1974BE52 Phys.Rev. C10, 1590 (1974) C.E.Bemis, Jr., F.Plasil, R.L.Ferguson, E.E.Gross, A.Zucker Attempted Coulomb Excitation of the Spontaneous-Fission Isomeric State In 239Pu NUCLEAR REACTIONS 239Pu(20Ne, 20Ne'), E=100, 117 MeV; measured fission fragments. 239mPu deduced upper limit on yield.
doi: 10.1103/PhysRevC.10.1590
1972CH46 Nucl.Phys. A198, 417 (1972) Validity of Spectral Distribution Methods in Spectroscopy
doi: 10.1016/0375-9474(72)90698-7
1972GR07 Phys.Rev. C5, 602 (1972) E.E.Gross, E.Newman, M.B.Greenfield, R.W.Rutkowski, W.J.Roberts, A.Zucker Charge-Asymmetry Effects in the Reaction 2H(4He, 3He)3H NUCLEAR REACTIONS 2H(α, 3He), E=50, 64, 82 MeV; measured σ(θ); deduced charge-asymmetry effects.
doi: 10.1103/PhysRevC.5.602
1972SO10 Phys.Lett. 41B, 135 (1972) Structure of 28Si, Some Answers and their Problems NUCLEAR STRUCTURE 28Si; calculated levels, B(E2). Shell model analysis of Hartree-Fock failure.
doi: 10.1016/0370-2693(72)90444-3
1972WO26 Phys.Lett. 42B, 157 (1972) S.K.M.Wong, J.M.G.Gomez, A.P.Zuker A Truncation Scheme for Shell Model Spaces NUCLEAR STRUCTURE 24Mg; calculated levels, B(E2), B(M1). Wave functions. Shell model;truncation scheme.
doi: 10.1016/0370-2693(72)90049-4
1971ME09 Phys.Rev. C4, 1114 (1971) J.J.H.Menet, E.E.Gross, J.J.Malanify, A.Zucker Total-Reaction-Cross-Section Measurements for 30-60-MeV Protons and the Imaginary Optical Potential NUCLEAR REACTIONS 12C, 54Fe, 58Ni, 59Co, 60Ni, 68Zn, 90Zr, 120Sn, 208Pb(p, X), E=30, 40, 50, 61 MeV; measured σ(T); deduced optical model parameters.
doi: 10.1103/PhysRevC.4.1114
1971PL07 Nucl.Phys. A174, 193 (1971) D.J.Plummer, K.Ramavataram, T.A.Hodges, D.G.Montague, A.Zucker, N.K.Ganguly Measurement of Polarization and Differential Cross Section in p-4He Elastic Scattering between 25 and 29 MeV NUCLEAR REACTIONS 4He(p, p), E=25.0, 26.1, 27.1, 28.2, 29.2 MeV; measured σ(θ), P(θ).
doi: 10.1016/0375-9474(71)91012-8
1971WO13 Phys.Lett. 36B, 437 (1971) A Simple Coupling Scheme for Exact Shell Model Calculations NUCLEAR STRUCTURE 20Ne, 22Na, 24Mg; calculated basis states. Shell model, antisymmetrized weak coupling basis.
doi: 10.1016/0370-2693(71)90523-5
1970GR07 Phys.Rev.Lett. 24, 473 (1970) E.E.Gross, E.Newman, W.J.Roberts, R.W.Rutkowski, A.Zucker Observation of Charge-Asymmetry Effects in the Reaction 2H(α, 3H)3He at 27.4 MeV c.m. NUCLEAR REACTIONS 2H(α, t), E=82 MeV; measured σ(θ); deduced charge asymmetry effects.
doi: 10.1103/PhysRevLett.24.473
1969ME08 Phys.Rev.Letters 22, 1128 (1969) J.J.H.Menet, E.E.Gross, J.J.Malanify, A.Zucker Total Reaction Cross-Section Measurements with 60-MeV Protons NUCLEAR REACTIONS 12C, 27Al, 56Fe, 58Ni, 59Co, 60Ni, 68Zn, 90Zr, 120Sn, 208Pb(p, X), E=60 MeV; measured σ; deduced optical model parameters.
doi: 10.1103/PhysRevLett.22.1128
1968GI07 Phys.Rev.Letters 21, 552(1968) R.O.Ginaven, E.E.Gross, J.J.Malanify, A.Zucker Spin Flip in the Inelastic Scattering of 30- and 40-MeV Protons by 28Si NUCLEAR REACTIONS 28Si(p, p'γ), E=29.7, 40 MeV; measured σ(E;Ep', θ(p'γ)).
doi: 10.1103/PhysRevLett.21.552
1968MO10 Phys.Rev. 169, 825 (1968) B.J.Morton, E.E.Gross, E.V.Hungerford, J.J.Malanify, A.Zucker Proton-Proton Final-State Interactions in the Reactions 3He(d, t)2p, d(3He, t)2p, p(3He, d)2p, and 3He(3He, 4He)2p NUCLEAR STRUCTURE 1H, 2H, 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.169.825
1968ZU02 Phys.Rev.Letters 21, 39 (1968) A.P.Zuker, B.Buck, J.B.McGrory Structure of O16
doi: 10.1103/PhysRevLett.21.39
1967FR12 Phys.Rev. 163, 1153 (1967) M.P.Fricke, E.E.Gross, A.Zucker Inelastic Scattering of 40-MeV Polarized Protons NUCLEAR STRUCTURE 60Ni, 58Ni, 54Fe, 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.163.1153
1967FR20 Phys.Rev. 156, 1207 (1967) M.P.Fricke, E.E.Gross, B.J.Morton, A.Zucker Polarizations and Differential Cross Sections For the Elastic Scattering of 40-MeV Protons.Ii NUCLEAR REACTIONS 12C, 40Ca, 59Co, 68Zn, 90Zr, 120Sn, 208Pb(p, p), E=40 MeV; measured products, 12C, 40Ca, 59Co, 68Zn, 90Zr, 120Sn, 208Pb; deduced σ(θ), polarization data. Data were imported from EXFOR entry O0328.
doi: 10.1103/PhysRev.156.1207
1967GR19 Nucl.Phys. A102, 673(1967) E.E.Gross, R.H.Bassel, L.N.Blumberg, B.J.Morton, A.van der Woude, A.Zucker Energy Dependence of the Elastic Scattering and Polarization of Protons on 40Ca NUCLEAR REACTIONS 40Ca(p, p), Ep=35.8, 45.5 MeV; measured σ(θ), pol(θ).
doi: 10.1016/0375-9474(67)90402-2
1967HA31 Phys.Rev. 162, 919 (1967) M.L.Halbert, F.E.Durham, C.D.Moak, A.Zucker Fluctuations in Angular Distributions of 12C(16O, α)24Mg NUCLEAR STRUCTURE 12C, 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.162.919
1967MO08 Phys.Rev.Letters 18, 1007 (1967) B.J.Morton, E.E.Gross, J.J.Malanify, A.Zucker Two-Proton Final-State Interactions in the Reactions D(3He, t)2p and 3He(d, t)2p at a Center-of-mass Energy of 21 MeV NUCLEAR STRUCTURE 3H, 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.1007
1966BL19 Phys.Rev. 147, 812 (1966) L.N.Blumberg, E.E.Gross, A.Van Der Woude, A.Zucker, R.H.Bassel Polarizations and Differential Cross Sections For the Elastic Scattering of 40-MeV Protons from 12C, 40Ca, 58Ni, 90Zr, and 208Pb NUCLEAR REACTIONS 12C(p, p), 12C(p, p'), 40Ca(p, p), 58Ni(p, p), 90Zr(p, p), 208Pb(p, p), E=40 MeV; measured products, 12C, 40Ca, 58Ni, 90Zr, 208Pb; deduced polarization data, σ(θ). Data were imported from EXFOR entry O0208.
doi: 10.1103/PhysRev.147.812
1966FR01 Phys.Rev.Letters 16, 746 (1966) M.P.Fricke, R.M.Drisko, R.H.Bassel, E.E.Gross, B.J.Morton, A.Zucker Asymmetry in the Inelastic Scattering of 40-MeV Polarized Protons NUCLEAR STRUCTURE 28Si, 60Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.16.746
1965BE40 Nucl.Phys. 65, 1 (1965) D.R.Bes, P.Federman, E.Maqueda, A.Zuker Properties of the γ-Vibrational State NUCLEAR STRUCTURE 150Nd, 152,154Sm, 154,156,158,160Gd, 156,158,160,162,164Dy, 162,164,166,168,170Er, 170,172,174,176Yb, 176,178,180Hf, 182,184,186W, 186Os, 228,230,232,234Th, 230,232,234,236,238U, 238,240,242Pu, 242,244,246,248Cm, 248,250,252,254Cf, 250,252,254,256Fm; calculated B(E2).
doi: 10.1016/0029-5582(65)90290-7
1964HA08 Bull.Am.Phys.Soc. 9, No.4, 418, DA3 (1964) M.L.Halbert, F.E.Durham, C.D.Moak, A.Zucker Fluctuations in the Reaction 12C(16O, α)24Mg NUCLEAR STRUCTURE 12C, 24Mg; measured not abstracted; deduced nuclear properties.
1963HA02 Bull.Am.Phys.Soc. 8, No.1, 25, F4 (1963) M.L.Halbert, F.E.Durham, C.D.Moak, A.Zucker Fluctuations in the Reaction C12(O16, α)Mg24 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1963HA40 Nucl.Phys. 47, 353 (1963); Erratum Nucl.Phys. 56, 174 (1964) M.L.Halbert, F.E.Durham, C.D.Moak, A.Zucker Fluctuations in the C12(O16, α)Mg24 Reaction NUCLEAR STRUCTURE 12C, 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90879-4
1962LI09 Phys.Rev. 127, 1280 (1962) Radiative Capture of N14 on P31 NUCLEAR STRUCTURE 31P, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.127.1280
1961HA04 Phys.Rev. 121, 236 (1961) Inelastic Scattering of N14 by C12 NUCLEAR STRUCTURE 12C, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.121.236
1961NE13 Proc.Rutherford Jubilee Intern.Conf., Manchester England, J.B.Birks, Ed., Academic Press Inc., New York, p.547 (1961) E.Newman, K.S.Toth, M.L.Halbert, A.Zucker Single-Nucleon Transfer Reactions Induced by 28-MeV N14 Ions NUCLEAR STRUCTURE 14N, 25Mg, 10B, 11B; measured not abstracted; deduced nuclear properties.
1960HA16 Phys.Rev. 117, 1545 (1960) M.L.Halbert, C.E.Hunting, A.Zucker Elastic Scattering of Nitrogen by Carbon
doi: 10.1103/PhysRev.117.1545
1960HA20 Nuclear Phys. 16, 158 (1960) Nitrogen-Aluminium Elastic Scattering
doi: 10.1016/S0029-5582(60)81065-6
1960ZU01 Bull.Am.Phys.Soc. 5, No.1, 67, UA8 (1960) Elastic Scattering of 27.3-MeV Nitrogen by Aluminum
1960ZU02 Proc. Conf. On Reactions between Complex Nuclei, 2nd, Gatlinburg, Ed. A.Zucker, E.C.Halbert, F.T.Howard, John Wiley sons, Inc., New York, p.144 (1960) Elastic Scattering of Nitrogen from Light Elements
1959HA28 Phys.Rev. 115, 1635 (1959) Elastic Scattering of N14 by Be9
doi: 10.1103/PhysRev.115.1635
1959HU13 Bull.Am.Phys.Soc. 4, No.4, 253, KA10 (1959) C.E.Hunting, M.L.Halbert, A.Zucker Elastic Scattering of N14 by Carbon
1958ZU24 Nuclear Phys. 6, 420 (1958) Protons and Alpha-Particles from the Nitrogen Bombardment of Aluminium
doi: 10.1016/0029-5582(58)90120-2
1957HA99 Phys.Rev. 106, 251 (1957) M.L.Halbert, T.H.Handley, J.J.Pinajian, W.H.Webb, A.Zucker Neutron-Transfer Reactions from the Nitrogen Bombardment of Be, C, O, Na, and Mg24, 25, 26 NUCLEAR REACTIONS 9Be, C, O, 23Na, 24,25,26Mg(14N, X), E<34 MeV; measured reaction products. 13N; deduced σ.
doi: 10.1103/PhysRev.106.251
1954CO72 Phys.Rev. 96, 1617 (1954) B.L.Cohen, H.L.Reynolds, A.Zucker Comparison of nitrogen- and proton-induced nuclear reactions NUCLEAR REACTIONS 25Mg(p, 2α), 25Mg(p, 2p), 25Mg(p, α), E=6-23.6 MeV; measured products, 24Na, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C1999.
doi: 10.1103/PhysRev.96.1617
1953RE22 Proc.Natl.Acad.Sci USA 39, 975 (1953) H.L.Reynolds, D.W.Scott, A.Zucker Nuclear Reactions with Energetic Nitrogen Ions NUCLEAR REACTIONS 2H(14N, n), 9Be(14N, n), (14N, X)18F, 9Be(14N, 10Be), (14N, 6He), 10B(14N, d), (14N, 13C), (14N, 11B), (14N, 9Be), (14N, 6Li), 11B(14N, p), (14N, 2p), 12C(14N, α), (14N, 8Be), (14N, 2p), (14N, 13C), 13C(14N, 2p), 14N(14N, 15N), (14N, 13C), 16O(14N, 2p), (14N, 8Be), (14N, 12C), (14N, γ), (14N, 15N), (14N, 17O), 32S(14N, p), (14N, 2p), (14N, 12C), 34S(14N, n), 32S(14N, 28Si), E=25 MeV; measured reaction products, En, In, Eβ, Iβ; deduced thick target yields.
doi: 10.1073/pnas.39.9.975
1950ZU01 Phys.Rev. 79, 241 X3 (1950) Concentration of Argon 36 and Study of the A36(d, p)A37 Reactions NUCLEAR REACTIONS 36Ar(d, p), E=3.9 MeV; measured reaction products, Ep, Ip; deduced excited states Q-values.
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