NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = N.Auerbach Found 134 matches. Showing 1 to 100. [Next]2024LE03 Phys.Rev. C 109, 024313 (2024) N.Le Anh, B.Minh Loc, P.Papakonstantinou, N.Auerbach Landscape of nuclear deformation softness with spherical quasiparticle random-phase approximation
doi: 10.1103/PhysRevC.109.024313
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
2023LO07 Phys.Rev. C 108, 024303 (2023) B.M.Loc, N.L.Anh, P.Papakonstantinou, N.Auerbach Origin of octupole deformation softness in atomic nuclei NUCLEAR STRUCTURE 32S, 64Zn, 72Se, 96Zr, 96Ru, 98Zr, 146Ba, 152Sm, 226Ra, 240Pu; calculated levels, J, π, energy of first 3- state, B(E3), octupole polarizability. Calculations based on fully self-consistent random-phase approximation (RPA) approach and quasiparticle RPA to diagnose octupole softness in nuclei.
doi: 10.1103/PhysRevC.108.024303
2022AN22 Phys.Rev. C 106, L051302 (2022) N.L.Anh, B.M.Loc, N.Auerbach, V.Zelevinsky Single-particle properties of the near-threshold proton-emitting resonance in 11B NUCLEAR STRUCTURE 11Be; calculated energy, width and J, π of near-threshold proton-emitting resonance seen in the recent experiment (2022AY04). Self-consistent Skyrme Hartree-Fock in the continuum with SkM*, SGII, SLy4 and SAMi interactions. NUCLEAR REACTIONS 10Be(p, p), E(cm)=100-350 keV; calculated σ(θ), s-wave phase shift. Self-consistent Skyrme Hartree-Fock in the continuum. Comparison to experimental data and other theoretical calculations.
doi: 10.1103/PhysRevC.106.L051302
2022AU04 Nucl.Phys. A1027, 122521 (2022) Coulomb corrections to Fermi beta decay in nuclei
doi: 10.1016/j.nuclphysa.2022.122521
2019LO01 Phys.Rev. C 99, 014311 (2019) Isospin mixing and Coulomb mixing in ground states of even-even nuclei NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 90Zr, 100,120Sn, 208Pb; calculated isovector monopole (IVM) strength and Coulomb strength for 208Pb, isospin mixing and Coulomb mixing in the ground states of even-even nuclei, isospin properties of the IVM resonance for 48Ca. HF-RPA and HF-pnRPA calculations using several different Skyrme interactions. Relevance to isospin symmetry.
doi: 10.1103/PhysRevC.99.014311
2018AU05 Phys.Rev. C 98, 064301 (2018) Nuclear structure studies of double-charge-exchange Gamow-Teller strength RADIOACTIVITY 42,44,46,48Ca(2β-); calculated double charge-exchange Gamow-Teller (DGT) strength distributions for 0+ to 0+ and 0+ to 2+ states using shell model, with the application of the single Gamow-Teller operator two times sequentially on the ground state of the parent nuclei, and FPD6 and KB3G interactions. 42,44,46,48Ti; calculated total number of final states in the fp-model space and f-model space for 2β- daughter nuclei. 48Sc; calculated cumulative sum of the single Gamow-Teller strength B(GT-) as a function of the number of 1+ states, and their excitation energies in intermediate nucleus 48Sc.
doi: 10.1103/PhysRevC.98.064301
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
2017LO07 Phys.Rev. C 96, 014311 (2017) Single-charge-exchange reactions and the neutron density at the surface of the nucleus NUCLEAR STRUCTURE 58Ni, 90Zr, 120Sn, 208Pb; calculated nuclear densities calculated using the Skyrme HF-BCS calculation. NUCLEAR REACTIONS 58Ni, 90Zr, 208Pb(3He, t), E=420 MeV; 120Sn(p, n), E=170 MeV; calculated differential σ(θ) for the population of the isobaric analog state (IAS) using the DWBA approach with the single-charge-exchange (SCX) form factors obtained from nuclear density calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.014311
2017ZE03 Phys.Rev. C 96, 044319 (2017) V.Zelevinsky, N.Auerbach, B.M.Loc Nuclear structure features of Gamow-Teller excitations NUCLEAR STRUCTURE 44,46Ti; calculated B(E2), B(GT), anticorrelation between B(GT) and collectivity of the first B(E2) using the nuclear shell-model.
doi: 10.1103/PhysRevC.96.044319
2014AU01 Phys.Rev. C 89, 014335 (2014) N.Auerbach, Ch.Stoyanov, M.R.Anders, S.Shlomo Isoscalar and isovector dipole strength distributions in nuclei and the Schiff moment NUCLEAR STRUCTURE 40,48Ca, 56,78Ni, 90,104Zr, 144Sm, 208Pb; calculated strength distribution S(E), S(E)/E, centroid energies, inverse energy moments of isoscalar and isovector dipole resonances (ISD and IVD). Influence dipole strength distribution on nuclear Schiff moment. Self-consistent HF-based RPA calculations using 18 different Skyrme-type effective interactions.
doi: 10.1103/PhysRevC.89.014335
2014AU04 Phys.Rev. C 90, 034315 (2014) Decay through a doorway state and the puzzle of 180Ta NUCLEAR STRUCTURE 180mTa; analyzed decay of mixed K excited state of an isomeric band populated in photon or Coulomb scattering with the states of other bands decaying to the ground state through a doorway state; described a mechanism contributing to the enhancement of decay rates from intermediate states to the ground state. Discussed experimental results.
doi: 10.1103/PhysRevC.90.034315
2012AU04 Phys.Rev. C 86, 045501 (2012) Dipole resonances and the nuclear Schiff moment
doi: 10.1103/PhysRevC.86.045501
2012AU10 J.Phys.:Conf.Ser. 366, 012001 (2012) Super-radiance and the widths of neutron resonances in the compound nucleus
doi: 10.1088/1742-6596/366/1/012001
2011CE02 Phys.Rev.Lett. 106, 042501 (2011) G.L.Celardo, N.Auerbach, F.M.Izrailev, V.G.Zelevinsky Distribution of Resonance Widths and Dynamics of Continuum Coupling
doi: 10.1103/PhysRevLett.106.042501
2010AU01 Phys.Rev. C 81, 067305 (2010) Neutron-proton radii in N ≈ Z nuclei NUCLEAR STRUCTURE 40Ca, 88Sr, 140Ce, 208Pb; calculated neutron-proton rms radii. Comparison with Skyrme Hartree-Fock calculations.
doi: 10.1103/PhysRevC.81.067305
2010AU02 Nucl.Phys. A834, 167c (2010) Doorway States and the Super-Radiant Mechanism in Nuclear Reactions
doi: 10.1016/j.nuclphysa.2009.12.030
2009AU01 Phys.Rev. C 79, 035502 (2009) Coulomb corrections to superallowed β decay in nuclei
doi: 10.1103/PhysRevC.79.035502
2009AU02 Phys.Rev.Lett. 103, 172501 (2009) η/s Ratio in Finite Nuclei
doi: 10.1103/PhysRevLett.103.172501
2008AU01 J.Phys.(London) G35, 014040 (2008) Search for electric dipole moments in atoms of radioactive nuclei NUCLEAR MOMENTS 223,225Ra, 223Rn, 221,223Fr; calculated intrinsic Schiff moments, induced atomic dipole moments, scaling for the intrinsic Schiff moment.
doi: 10.1088/0954-3899/35/1/014040
2008ZE04 Phys.Rev. C 78, 014310 (2008) V.Zelevinsky, A.Volya, N.Auerbach Nuclear Schiff moment and soft vibrational modes
doi: 10.1103/PhysRevC.78.014310
2007AU01 Nucl.Phys. A781, 67 (2007) Doorway states in nuclear reactions as a manifestation of the "super-radiant" mechanism
doi: 10.1016/j.nuclphysa.2006.10.078
2007AU05 Nucl.Phys. A787, 532c (2007) Tests of time reversal symmetry in radioactive nuclei NUCLEAR STRUCTURE 199Hg, 129Xe, 133Cs, 219,221,223,225Ra, 223Rn, 221,223Fr, 225Ac, 229Pa; calculated Schiff and dipole moments. Quasiparticle RPA. NUCLEAR MOMENTS 199Hg, 129Xe, 133Cs, 219,221,223,225Ra, 223Rn, 221,223Fr, 225Ac, 229Pa; calculated Schiff and dipole moments. Quasiparticle RPA.
doi: 10.1016/j.nuclphysa.2006.12.081
2007AU07 Phys.Atomic Nuclei 70, 1654 (2007) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Senkov, V.G.Zelevinsky Is it possible to enhance the nuclear Schiff moment by nuclear collective modes? NUCLEAR MOMENTS 217,219,221Ra, 217,219,221Rn; calculated the nuclear Schiff moment using the QRPA formalism.
doi: 10.1134/S106377880709027X
2006AU02 Phys.Rev. C 74, 025502 (2006) N.Auerbach, V.F.Dmitriev, V.V.Flambaum, A.Lisetskiy, R.A.Sen'kov, V.G.Zelevinsky Nuclear Schiff moment in nuclei with soft octupole and quadrupole vibrations NUCLEAR STRUCTURE 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA. NUCLEAR MOMENTS 217,219,221Ra; calculated Schiff moments, role of soft collective quadrupole and octupole vibrations. Quasiparticle RPA.
doi: 10.1103/PhysRevC.74.025502
2005DM01 Phys.Rev. C 71, 035501 (2005) V.F.Dmitriev, R.A.Senkov, N.Auerbach Effects of core polarization on the nuclear Schiff moment NUCLEAR MOMENTS 129Xe, 133Cs, 199Hg, 211Rn, 213,225Ra, 223Fr; calculated Schiff moments, core polarization contributions. NUCLEAR STRUCTURE 129Xe, 133Cs, 199Hg, 211Rn, 213,225Ra, 223Fr; calculated Schiff moments, core polarization contributions.
doi: 10.1103/PhysRevC.71.035501
2002AU01 Phys.Rev. C65, 024322 (2002) Weak Interaction Rates Involving 12C, 14N, and 16O NUCLEAR REACTIONS 12C, 14N, 16O(ν, e), (ν, μ-), (μ-, γ), E < 300 MeV; calculated σ, reaction rates; deduced isovector strength quenching. Large shell-model basis, comparisons with data.
doi: 10.1103/PhysRevC.65.024322
2002AU02 Phys.Rev. C65, 034601 (2002) ' Super-Radiant ' States and Narrow Resonances in the Δ-Nucleus System NUCLEAR STRUCTURE 12C; calculated Δ-nucleus configurations, possible super-radiant state formation.
doi: 10.1103/PhysRevC.65.034601
2002VO06 Phys.Rev. C65, 044603 (2002) C.Volpe, N.Auerbach, G.Colo, N.Van Giai Charged-Current Neutrino-208Pb Reactions NUCLEAR REACTIONS 208Pb(ν, e), E=0-50 MeV; 208Pb(ν, μ), E=0-300 MeV; calculated non-flux-averaged σ. Self-consistent charge-exchange RPA, charged-current neutrinos.
doi: 10.1103/PhysRevC.65.044603
2001AU01 Phys.Rev. C63, 017301 (2001) About Coulomb Energy Shifts in Halo Nuclei NUCLEAR STRUCTURE 17O, 17F, 11Be, 11N; calculated single-particle energies, Coulomb energy shifts.
doi: 10.1103/PhysRevC.63.017301
2001AU05 Nucl.Phys. A687, 289c (2001) N.Auerbach, C.Volpe, G.Colo, T.Suzuki, N.Van Giai Neutrino-Nucleus Interactions and Nuclear Giant Resonances NUCLEAR REACTIONS 12C(ν, e), (ν, μ-), E not given; calculated energy averaged σ. RPA, QRPA, Shell Model, comparison between different theoretical approaches and with data.
doi: 10.1016/S0375-9474(01)00634-0
2001VO18 Yad.Fiz. 64, No 7, 1242 (2001); Phys.Atomic Nuclei 64, 1165 (2001) C.Volpe, N.Auerbach, G.Colo, T.Suzuki, N.Van Giai Neutrino-12C Reactions and the LSND and KARMEN Experiments on Neutrino Oscillations NUCLEAR REACTIONS 12C(ν, e), (ν, μ-), E=spectrum; calculated flux-averaged σ. Charge-exchange RPA, shell model. Comparison with data.
doi: 10.1134/1.1389536
2000BR54 Phys.Rev. C62, 044313 (2000) B.A.Brown, V.Zelevinsky, N.Auerbach Microscopic Calculation of Double-Dipole Excitations NUCLEAR STRUCTURE 16O, 40Ca; calculated single-, double-dipole strength distributions. Shell model.
doi: 10.1103/PhysRevC.62.044313
2000RO20 Phys.Rev. C62, 017302 (2000) S.J.Q.Robinson, L.Zamick, A.Mekjian, N.Auerbach Effects of Deformation on Weak Charge Transfer Transition Strengths NUCLEAR STRUCTURE 12C; calculated isovector dipole, spin dipole, orbital dipole excitations summed strengths; deduced no deformation dependence.
doi: 10.1103/PhysRevC.62.017302
2000VO13 Phys.Rev. C62, 015501 (2000) C.Volpe, N.Auerbach, G.Colo, T.Suzuki, N.Van Giai Microscopic Theories of Neutrino-12C Reactions NUCLEAR REACTIONS 12C(ν, e), (ν, μ-), E < 300 MeV; calculated σ, flux-averaged σ, multipole strength distributions. Shell model, RPA, quasiparticle RPA. Comparisons with data.
doi: 10.1103/PhysRevC.62.015501
1999AU04 Phys.Rev. C60, 025501 (1999) Core-Polarization Contribution to the Nuclear Anapole Moment NUCLEAR STRUCTURE 133Sb, 207Tl, 207Pb, 209Bi; calculated anapole moments, core-polarization corrections. 208Pb; calculated B(E1), anapole moments distributions. Shell-model configuration mixing.
doi: 10.1103/PhysRevC.60.025501
1999ZA17 Nucl.Phys. A658, 285 (1999) The Effects of Deformation on Isovector Electromagnetic and Weak Transition Strengths NUCLEAR STRUCTURE 12C; calculated B(M1), isovector dipole strengths for spherical and deformed shapes. Rotational Model.
doi: 10.1016/S0375-9474(99)00347-4
1997AU01 Phys.Lett. 391B, 249 (1997) Microscopic Calculations of Parity Nonconserving Spreading Widths in Nuclei NUCLEAR STRUCTURE A ≤ 250; calculated compound states parity nonconserving spreading widths. Induced parity nonconserving interaction, microscopic approach.
doi: 10.1016/S0370-2693(96)01477-3
1997AU05 Phys.Rev. C56, R2368 (1997) N.Auerbach, N.Van Giai, O.K.Vorov Neutrino Scattering from 12C and 16O NUCLEAR REACTIONS 12C, 16O(ν, e), (ν, μ-), E=spectrum; calculated flux-averaged inclusive, exclusive σ; 12C, 16O(μ-, X), E not given; calculated capture rates; deduced pairing term effect. Hartree-Fock RPA calculations. Comparisons with data.
doi: 10.1103/PhysRevC.56.R2368
1997AU06 Phys.Lett. 414B, 1 (1997) Renormalization of the One-Body Off-Diagonal Coulomb Field in Nuclei
doi: 10.1016/S0370-2693(97)01160-X
1997SP03 Phys.Rev. C56, 1357 (1997) V.Spevak, N.Auerbach, V.V.Flambaum Enhanced T-Odd, P-Odd Electromagnetic Moments in Reflection Asymmetric Nuclei NUCLEAR STRUCTURE 223,225Ra, 223Rn, 221,223Fr, 225Ac, 229Pa; calculated T-odd, P-odd collective electric moments; deduced atomic electric dipole moments enhancement. Reflection asymmetry, two-fluid liquid drop model, particle plus core model.
doi: 10.1103/PhysRevC.56.1357
1996AU06 Phys.Rev.Lett. 76, 4316 (1996) N.Auerbach, V.V.Flambaum, V.Spevak Collective T- and P-Odd Electromagnetic Moments in Nuclei with Octupole Deformations NUCLEAR STRUCTURE 223,225Ra, 223Rn, 229Pa, 199Hg, 129Xe; analyzed collective T-odd, P-odd electromagnetic moments, octupole deformation for nuclei.
doi: 10.1103/PhysRevLett.76.4316
1996VO16 Phys.Lett. 385B, 17 (1996) O.K.Vorov, N.Auerbach, V.V.Flambaum Structure of Low-Energy Collective 0--States in Doubly Magic Nuclei and Matrix Elements of the P-Odd and P- and T-Odd Weak Interaction
doi: 10.1016/0370-2693(96)00861-1
1995AU03 Phys.Rev.Lett. 74, 2638 (1995) N.Auerbach, J.D.Bowman, V.Spevak Nearby Doorway States, Parity Doublets, and Parity Mixing in Compound Nuclear States NUCLEAR STRUCTURE 232Th; calculated parity doublet role in parity mixing. Doorway state model.
doi: 10.1103/PhysRevLett.74.2638
1995SP05 Phys.Lett. 359B, 254 (1995) Parity Mixing and Time Reversal Violation in Nuclei with Octupole Deformations
doi: 10.1016/0370-2693(95)01099-C
1994AU04 Phys.Rev. C50, 1456 (1994) Theory of Parity Violation in Compound Nuclear States: One particle aspects NUCLEAR STRUCTURE 233Th; calculated parity violating spreading width. Feshbach projection operator formalism.
doi: 10.1103/PhysRevC.50.1456
1994AU05 Phys.Rev. C50, 1606 (1994) ' Super-Radiant ' States in Intermediate Energy Nuclear Physics NUCLEAR STRUCTURE 16O; calculated N(N-bar) excitation energy; deduced super-radiant state, width characteristics. Relativistic approach, intermediate energy.
doi: 10.1103/PhysRevC.50.1606
1994AU07 Nucl.Phys. A577, 443c (1994) The Spin-Dipole Resonance and Parity Mixing in Compound Nuclear States NUCLEAR STRUCTURE 232Th; compiled, reviewed, analyzed neutron scattering data, analyses; deduced spin-dipole contribution to parity nonconserving average spreading width, asymmetry. Doorway state approximation.
doi: 10.1016/0375-9474(94)90894-X
1994AU09 Phys.Lett. 340B, 6 (1994) Enhancement of Symmetry Violation in a Chaotic System NUCLEAR STRUCTURE A=9; calculated parity nonconserving matrix elements. Extended shell model space.
doi: 10.1016/0370-2693(94)91289-0
1993AU01 Phys.Lett. 304B, 17 (1993) N.Auerbach, D.C.Zheng, L.Zamick, B.A.Brown Correlation between the Quenching of Total GT(+) Strength and the Increase of E2 Strength NUCLEAR STRUCTURE 20Ne, 44Ti; calculated total β+-decay Gamow-Teller, spin, orbital total M1 transition strengths. Shell model.
doi: 10.1016/0370-2693(93)91392-Z
1993AU03 Nucl.Phys. A556, 190 (1993) N.Auerbach, G.F.Bertsch, B.A.Brown, L.Zhao β+ Gamow-Teller Strength in Nuclei RADIOACTIVITY 26Mg, 54Fe, 56Ni(β+); calculated Gamow-Teller transition strength, B(λ). Quasiparticle RPA, large basis shell model.
doi: 10.1016/0375-9474(93)90347-Z
1993GR03 Phys.Rev. C47, 1466 (1993) Y.Grof, N.Auerbach, D.Benton, H.T.Fortune, K.Johnson, M.A.Kagarlis, G.Kahrimanis, S.Mordechai, C.L.Morris, J.M.O'Donnell, I.Orion, D.Saunders, D.A.Smith, H.Ward, C.F.Moore Double Giant Resonances in Pion Double Charge Exchange on 51V, 115In, and 197Au NUCLEAR REACTIONS 51V, 115In, 197Au(π+, π-), E=295 MeV; measured σ(θ, E(π)), σ(θ). 51Mn, 197Tl, 115Sb deduced GDR, double IAS excitation, Γ.
doi: 10.1103/PhysRevC.47.1466
1993WA02 Phys.Rev. C47, 687 (1993) H.Ward, J.M.Applegate, N.Auerbach, J.Beck, J.Johnson, K.Koch, C.F.Moore, S.Mordechai, C.L.Morris, J.M.O'Donnell, M.Rawool-Sullivan, B.G.Ritchie, D.L.Watson, C.Whitley Systematics of the Double Isobaric Analog State Cross Section at 50 MeV NUCLEAR REACTIONS 44Ca, 56Fe, 93Nb(π+, π-), E=50 MeV; measured σ(θ, E(π)); deduced short range component of effective double charge exchange operator. 93Tc level deduced isospin mixing mechanism role in excitation.
doi: 10.1103/PhysRevC.47.687
1992AU01 Phys.Rev. C45, R514 (1992) One-Body, Collective Contributions to Parity Mixing in Compound Nuclear States
doi: 10.1103/PhysRevC.45.R514
1992AU02 Phys.Rev. C45, 1108 (1992) Nuclear Structure Properties of the Double-Charge-Exchange Transition Amplitudes NUCLEAR STRUCTURE 42,44,46,48Ca, 58,60,62,64,66,68Ni; calculated double isobaric analog state transition amplitudes; deduced valence nucleon two-body correlations role.
doi: 10.1103/PhysRevC.45.1108
1992AU03 Phys.Lett. 282B, 263 (1992) Comment on QCD Effects in the Nuclear Medium, the Effective Nucleon Mass and the Nolen-Schiffer Anomaly NUCLEAR STRUCTURE 41Ca, 41Sc; calculated binding energies; deduced corrections to Coulomb displacement energies restrictions.
doi: 10.1016/0370-2693(92)90635-H
1992AU06 Phys.Rev. C46, 2582 (1992) Doorway State Approximation and Sign Correlations in Parity Nonconservation in Compound Neutron Resonances NUCLEAR REACTIONS 232Th(polarized n, X), E=1 eV; analyzed asymmetry data; deduced parity nonconserving matrix element inconsistency with model values. Doorway model, shell model comparison.
doi: 10.1103/PhysRevC.46.2582
1992OA01 Phys.Rev. C45, 2254 (1992) D.S.Oakley, J.R.Shepard, N.Auerbach Nuclear Compressibility and the Isoscalar Monopole Resonance in a Relativistic Continuum Random Phase Approximation NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar monopole strength distribution, transition density. Dirac-Hartree RPA, continuum.
doi: 10.1103/PhysRevC.45.2254
1992WA11 Phys.Rev. C45, 2723 (1992) H.Ward, K.Johnson, G.Kahrimanis, D.Saunders, C.F.Moore, S.Mordechai, C.L.Morris, N.Auerbach Double Giant Dipole Resonance in the (π-, π+) Reaction NUCLEAR REACTIONS 13C, 27Al, 40Ca, 56Fe, 59Co, 93Nb(π-, π+), E=295 MeV; measured σ(θ), σ(θ, E(π)); deduced Pauli blocking effects, isospin splitting features. 13Be, 27Na, 40Ar, 59Mn, 93Y, 56Cr deduced double giant dipole resonance. Coupled-channels impulse approximation.
doi: 10.1103/PhysRevC.45.2723
1991AU04 Nucl.Phys. A527, 443c (1991) The Pion Double Charge Exchange Reaction NUCLEAR STRUCTURE 56Fe, 59Co, 93Nb, 130Te, 138Ba, 197Au; analyzed pion scattering data; deduced isotensor double giant resonance excitation features.
doi: 10.1016/0375-9474(91)90136-T
1991MO15 Phys.Rev. C44, 2209 (1991) C.F.Moore, K.Johnson, G.P.Kahrimanis, J.McDonald, M.Snell, H.J.Ward, S.H.Yoo, C.L.Morris, S.Mordechai, M.Burlein, N.Claytor, H.T.Fortune, R.Ivie, G.B.Liu, J.M.O'Donnell, D.Smith, N.Auerbach, D.Robson Angular Distributions for the Double Isobaric Analog and a T (<) State at High Excitation in Pion Double Charge Exchange on 93Nb NUCLEAR REACTIONS 93Nb(π+, π-), E=295 MeV; measured σ(θ(π), E(π)), σ(θ). 93Tc deduced large probability for T< excitation.
doi: 10.1103/PhysRevC.44.2209
1990AU01 Ann.Phys.(New York) 197, 376 (1990) Isotensor Double Giant Resonances in Double Charge-Exchange Reactions NUCLEAR STRUCTURE 56Fe, 59Co, 93Nb, 130Te, 138Ba, 197Au; calculated isotensor GDR, widths, excitation by double charge exchange reactions.
doi: 10.1016/0003-4916(90)90216-B
1990MO02 Phys.Rev. C41, 202 (1990) S.Mordechai, H.T.Fortune, J.M.O'Donnell, G.Liu, M.Burlein, A.H.Wuosmaa, S.Greene, C.L.Morris, N.Auerbach, S.H.Yoo, C.F.Moore Observation of Double Isovector Giant Dipole Resonances from Pion Double Charge Exchange NUCLEAR REACTIONS 40Ca, 93Nb, 56Fe(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 56Ni, 40Ti, 93Tc deduced isovector GDR excitation. Other data analyzed.
doi: 10.1103/PhysRevC.41.202
1990ZH01 Ann.Phys.(New York) 197, 343 (1990) D.-C.Zheng, L.Zamick, N.Auerbach Nuclear Structure Studies of Double Gamow-Teller and Double Beta Decay Strength RADIOACTIVITY 8He, 20O, 22Ne, 42,44Ca(2β); calculated double Gamow-Teller transition following 2β-decay. Shell model.
doi: 10.1016/0003-4916(90)90215-A
1989AU02 Phys.Lett. 219B, 184 (1989) N.Auerbach, F.Osterfeld, T.Udagawa The Spin Isovector Monopole Strength and the (3He, t) Reaction NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; 90Zr(3He, t), E=600 MeV; calculated σ(θ), energy integrated σ; deduced spin-flip isovector monopole resonance role.
doi: 10.1016/0370-2693(89)90374-2
1989AU05 Ann.Phys.(New York) 192, 77 (1989) N.Auerbach, L.Zamick, D.C.Zheng Double Gamow-Teller Strength in Nuclei NUCLEAR STRUCTURE 12C, 12N, 12O, 22Ne, 22Na, 22Mg; calculated double Gamow-Teller strength. Shell model, extended space.
doi: 10.1016/0003-4916(89)90117-6
1989MO09 Phys.Rev. C40, 850 (1989) S.Mordechai, N.Auerbach, S.Greene, C.L.Morris, J.M.O'Donnell, H.T.Fortune, G.Liu, M.Burlein, A.Wuosmaa, S.H.Yoo, C.F.Moore Properties of the Giant Dipole Resonance Built on the Isobaric Analog State NUCLEAR REACTIONS 13C, 59Co, 93Nb, 138Ba, 197Au(π+, π-), E=292 MeV; measured σ(θ). 13O, 59Cu, 93Tc, 138Ce, 197Tl deduced GDR built on IAS.
doi: 10.1103/PhysRevC.40.850
1989MO19 Phys.Lett. 230B, 41 (1989) M.A.Moinester, A.Trudel, K.Raywood, S.Yen, B.M.Spicer, R.Abegg, W.P.Alford, N.Auerbach, A.Celler, D.Frekers, O.Hausser, R.L.Helmer, R.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, N.S.P.King, S.Long, C.A.Miller, M.Vetterli, J.Watson, A.I.Yavin A Study of Spin Isovector Giant Resonances with the 208Pb(n, p)208Tl Reaction NUCLEAR REACTIONS 208Pb(n, p), E=198, 458 MeV; measured σ(θp, Ep). 208Tl deduced spin isovector giant resonances.
doi: 10.1016/0370-2693(89)91650-X
1989ZH07 Phys.Rev. C40, 936 (1989) D.C.Zhang, L.Zamick, N.Auerbach Generalization of the Sum Rule for Double Gamow-Teller Operators NUCLEAR STRUCTURE 8He, 12Be, 20,22O, 42,44,46,48Ca; calculated double Gamow-Teller transition sum rules.
doi: 10.1103/PhysRevC.40.936
1988AU05 Phys.Rev. C38, 1277 (1988) N.Auerbach, W.R.Gibbs, J.N.Ginocchio, W.B.Kaufmann Pion-Nucleus Double Charge Exchange and the Nuclear Shell Model NUCLEAR REACTIONS 42,44,46,48Ca, 46,48,50Ti, 52Cr, 54Fe(π+, π-), E=35, 45, 292 MeV; calculated ground, IAS transition σ(θ). Shell model.
doi: 10.1103/PhysRevC.38.1277
1988AU07 Phys.Rev. C38, 2921 (1988) Core Polarization Effects in sd-Shell Nuclei and Charge-Symmetry Breaking in the Nuclear Mean Field NUCLEAR STRUCTURE 28Si, 32Si, 40Ca; calculated proton, neutron densities, single-particle potentials. Hartree-Fock method, spherical, deformed nuclei, symmetry potential.
doi: 10.1103/PhysRevC.38.2921
1988MO01 Phys.Rev.Lett. 60, 408 (1988) S.Mordechai, N.Auerbach, G.R.Burleson, K.S.Dhuga, M.Dwyer, J.A.Faucett, H.T.Fortune, R.Gilman, S.J.Greene, C.Laymon, C.F.Moore, C.L.Morris, D.S.Oakley, M.A.Plum, S.J.Seestrom-Morris, P.A.Seidl, M.J.Smithson, Z.F.Wang, J.D.Zumbro Giant Dipole Resonances Built on Isobaric Analog States in Pion Double Charge Exchange NUCLEAR REACTIONS 56Fe, 80Se, 208Pb(π+, π-), E at 292 MeV/c; measured σ(E(π-), θ(π-)), σ(θ(π-)). 56Ni, 80Kr, 208Po deduced giant dipole resonance parameters. Coupled-channel impulse approximation calculations.
doi: 10.1103/PhysRevLett.60.408
1988MO15 Phys.Rev.Lett. 61, 531 (1988) S.Mordechai, N.Auerbach, M.Burlein, H.T.Fortune, S.J.Greene, C.F.Moore, C.L.Morris, J.M.O'Donnell, M.W.Rawool, J.D.Silk, D.L.Watson, S.H.Yoo, J.D.Zumbro Pion Double Charge Exchange to the Double Dipole Resonance NUCLEAR REACTIONS 32S(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 32Ar deduced resonances, Γ.
doi: 10.1103/PhysRevLett.61.531
1988MO33 Phys.Rev. C38, 2709 (1988) S.Mordechai, N.Auerbach, H.T.Fortune, C.L.Morris, C.F.Moore Isospin Splitting of the Giant Dipole Built on the Isobaric Analog State NUCLEAR REACTIONS 56Fe(π+, π-), E=292 MeV; measured σ(E(π), θ(π)), σ(θ). 56Fe deduced double IAS, giant resonances, Γ.
doi: 10.1103/PhysRevC.38.2709
1987AU03 Phys.Rev.Lett. 59, 1076 (1987) N.Auerbach, W.R.Gibbs, E.Piasetzky Pion Double Charge Exchange and the Nuclear Shell Model NUCLEAR REACTIONS 42,44,46,48Ca(π+, π-), E=35 MeV; calculated double charge exchange σ.
doi: 10.1103/PhysRevLett.59.1076
1987AU05 Phys.Rev. C36, 2694 (1987) Significance of the 54Fe(n, p) Measurement of the Gamow-Teller Transition NUCLEAR REACTIONS 54Fe(n, p), (p, n), E not given; analyzed data; deduced Gamow-Teller transition strength quenching.
doi: 10.1103/PhysRevC.36.2694
1987ZU03 Phys.Rev. C36, 1479 (1987) J.D.Zumbro, H.T.Fortune, M.Burlein, C.L.Morris, Z.-F.Wang, R.Gilman, K.S.Dhuga, G.R.Burleson, M.W.Rawool, R.W.Garnett, M.J.Smithson, D.S.Oakley, S.Mordechai, C.F.Moore, M.A.Machuca, D.L.Watson, N.Auerbach Double Charge Exchange to the Double Isobaric Analog State at T(π) ≈ 292 MeV NUCLEAR REACTIONS 30Si, 34S, 44Ca, 50Ti, 51V, 52Cr, 58Ni(π+, π-), E ≈ 292 MeV; measured σ(θ), σ(π). 44Ti, 51Mn, 52Fe, 50Cr levels deduced ground state, double IAS excitation σ.
doi: 10.1103/PhysRevC.36.1479
1986AU03 Nucl.Phys. A452, 398 (1986) A Microscopic Phenomenological Approach to the Spreading Widths of Giant Resonances NUCLEAR STRUCTURE 208Pb; calculated isoscalar, isovector dipole, monopole, quadrupole strengths, giant resonance spreading width. Hartree-Fock RPA, extended response functions.
doi: 10.1016/0375-9474(86)90205-8
1985AU01 Phys.Rev. C51, 682 (1985) N.Auerbach, A.Klein, E.R.Siciliano Isospin Composition of Giant Resonances and Asymmetries in π+ Compared to π- Inelastic Scattering NUCLEAR REACTIONS 40,48Ca, 90Zr, 120Sn, 208Pb(π+, π+'), (π-, π-'), E not given; calculated σ(θ), ratios. Microscopic model. NUCLEAR STRUCTURE 40,48Ca, 90Zr, 120Sn, 208Pb; calculated GQR, total strengths. 120Sn; calculated T=0, GQR transition densities. RPA, isoscalar, isovector modes.
doi: 10.1103/PhysRevC.51.682
1985AU08 Phys.Rev. C32, 1102 (1985) Double Isobaric Analog Resonance in 208Po and the Isobaric Multiplet Mass Equation NUCLEAR STRUCTURE 208Po; analyzed double IAS resonance data; deduced isobaric mass multiplet equation parameters, sizeable second or higher order Coulomb energy contribution evidence. Input data from (π+, π-) reactions.
doi: 10.1103/PhysRevC.32.1102
1985KL01 Phys.Rev. C31, 710 (1985) Continuum Charge-Exchange Spectra and the Quenching of Gamow-Teller Strength NUCLEAR REACTIONS 90Zr(p, n), E=200 MeV; calculated σ(θ, En), θ<10°. 90Nb deduced Gamow-Teller transition strength characteristics. Charge exchange, Hartree-Fock RPA, Skyrme interaction.
doi: 10.1103/PhysRevC.31.710
1985KL07 Phys.Rev. C32, 1998 (1985) A.Klein, E.R.Siciliano, N.Auerbach Continuum Spectra for 165 MeV Pion-Nucleus Single Charge Exchange NUCLEAR REACTIONS 40Ca, 90Zr, 120Sn(π+, π0), (π-, π0), E=165 MeV; calculated σ(θ, E(π)); deduced giant isovector resonances role. Single scattering approximation.
doi: 10.1103/PhysRevC.32.1998
1984AU02 Phys.Rev. C29, 526 (1984) N.Auerbach, M.B.Johnson, A.Klein, E.R.Siciliano Nuclear Structure Effects in Pion Single Charge Exchange NUCLEAR REACTIONS 90Zr, 120Sn, 208Pb(π-, π0), (π+, π0), E=100-300 MeV; calculated IAR, isovector monopole resonance transition densities; deduced structure effects role. DWIA model.
doi: 10.1103/PhysRevC.29.526
1984AU07 Nucl.Phys. A422, 480 (1984) A Microscopic Theory of Muon Capture in Nuclei NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated binding energies, muon capture rates. Microscopic model.
doi: 10.1016/0375-9474(84)90360-9
1984AU08 Nucl.Phys. A422, 501 (1984) Excitation of Giant Resonances in the Ca Isotopes in (π±, π0) Reactions NUCLEAR REACTIONS 40,42,44,46,48Ca(π+, π0), (π-, π0), E=165 MeV; calculated σ(θ) for isovector monopole, GDR excitations. Microscopic charge exchange RPA, sum rule transition densities. NUCLEAR STRUCTURE 40,42,44,46,48Ca; calculated radial moments, transition densities, isovector monopole, GDR. Microscopic RPA, sum rule approach.
doi: 10.1016/0375-9474(84)90361-0
1984AU09 J.Phys.(Paris), Colloq.C4, 305 (1984); See 1984Au15 Excitation of Giant Resonances in Pion Charge-Exchange Reactions
1984AU10 Phys.Rev. C30, 736 (1984) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love Reply to '' Comment on ' (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances ' '' NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; calculated IAS, isovector monopole resonance excitation σ(θ=0°); deduced medium corrections role.
doi: 10.1103/PhysRevC.30.736
1984AU11 Phys.Rev. C30, 1032 (1984) Structure of Isovector Spin Excitations in Nuclei NUCLEAR STRUCTURE 60,62,64Ni; calculated isovector spin excitations. 90,92,94,96Zr; calculated M1, Gamow-Teller excitation energies. 90Zr, 208Pb; calculated spin isovector monople, strength distribution, transition density, charge exchange nonenergy weighted sum rule. 60Ni; calculated spin isovector monopole, charge exchange nonenergy weighted sum rule. Hartree-Fock, charge exchange, RPA.
doi: 10.1103/PhysRevC.30.1032
1984AU15 J.Phys.(Paris), Colloq.C-4, 305 (1984) Excitation of Giant Resonances in Pion Charge-Exchange Reactions NUCLEAR REACTIONS 40,48Ca, 60Ni, 90Zr, 120Sn, 208Pb(π+, π0), (π-, π0), E ≤ 70 MeV; calculated σ(E(π0), θ(π0)), σ(θ).
1983AD07 Phys.Lett. 131B, 11 (1983) Widths of Isovector Monopole Resonances NUCLEAR STRUCTURE 208Tl, 140La, 120In, 90Y; calculated isovector monopole components, widths. Self-consistent Hartree-Fock, charge exchange, RPA, Skyrme interaction.
doi: 10.1016/0370-2693(83)91081-X
1983AU01 Nucl.Phys. A395, 77 (1983) A Microscopic Theory of Giant Electric Isovector Resonances NUCLEAR STRUCTURE 48Ca, 90Zr, 120Sn, 208Pb; calculated levels, dipole, quadrupole isospin components, charge exchange analog strength distributions. Self-consistent Hartree-Fock, RPA.
doi: 10.1016/0375-9474(83)90090-8
1983AU02 Phys.Rev. C27, 1346 (1983) Influence of Nucleon Internal Degrees of Freedom on the Strength of Electric Giant Resonances at Low Energies NUCLEAR STRUCTURE 90Zr, 208Pb; calculated electric giant resonance strength quenching factor. Formalism with nucleon internal degrees of freedom.
doi: 10.1103/PhysRevC.27.1346
1983AU03 Phys.Rev. C27, 1818 (1983) Transition Densities for Charge-Exchange Components of Giant Isovector Resonances and the Proton-Neutron Density Distributions in Nuclei NUCLEAR REACTIONS 40Ca(π+, π0), (π-, π0), E not given; calculated σ for giant resonances excitation. RPA transition densities. NUCLEAR STRUCTURE 40Ca; calculated isovector giant resonances, strengths, charge exchange component transition densities. RPA, sum rules.
doi: 10.1103/PhysRevC.27.1818
1983AU05 Phys.Rev. C28, 280 (1983) N.Auerbach, J.D.Bowman, M.A.Franey, W.G.Love (p, n) and (n, p) Reactions as Probes of Isovector Giant Monopole Resonances NUCLEAR REACTIONS 90Zr, 40Ca, 120Sn, 208Pb(p, n), E=120, 800 MeV; calculated σ(θ) for isovector giant monopole resonance excitation. DWIA, RPA based charge exchange transition densities.
doi: 10.1103/PhysRevC.28.280
1983AU07 Phys.Rev. C28, 2075 (1983) Excitation of Giant Electric Isovector Resonances in Pion Charge Exchange Reactions NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated proton, neutron charge rms radii, charge exchange dipole, monopole, quadrupole energies, total transition strength distribution, transition densities. Hartree-Fock, RPA approximations, sum rule method. NUCLEAR REACTIONS 40,48Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π-, π0), (π+, π0), E not given; calculated isovector monopole, dipole, quadrupole excitation σ(θ), σ(θ, E(π0)) vs excitation energy. DWIA, RPA, sum rule method transition densities.
doi: 10.1103/PhysRevC.28.2075
1982AU03 Phys.Rev. C25, 2841 (1982) Pion Charge-Exchange Reaction and Transition Densities to Isobaric Analog States NUCLEAR REACTIONS 41,42,44,46,48Ca, 90Zr, 208Pb(π+, π0), E=180 MeV; calculated σ(θ), σ. DWIA, Hartree-Fock transition densities.
doi: 10.1103/PhysRevC.25.2841
1982AU06 Phys.Lett. 114B, 95 (1982) Calculation of Inclusive μ--Capture Rates in Heavy Nuclei ATOMIC PHYSICS, Mesic-Atoms 48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated 1s μ- orbit binding energy. Dirac equation, Hartree-Fock charge density, Skyrme interaction. NUCLEAR STRUCTURE 48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated muon capture rates. Self-consistent RPA.
doi: 10.1016/0370-2693(82)90122-8
1982AU08 Phys.Rev.Lett. 49, 913 (1982) Excitation of Giant Resonances in Pion Charge Exchange and the Proton-Neutron Density Distributions in Nuclei NUCLEAR REACTIONS 40Ca(π-, π0), (π+, π0), E=164 MeV; analyzed data. 40Ca levels deduced Coulomb polarization effects, charge exchange dipole component transition densities. RPA.
doi: 10.1103/PhysRevLett.49.913
1982AU09 Phys.Lett. 118B, 256 (1982) RPA Calculations of Isovector Spin-Flip Excitations NUCLEAR STRUCTURE 60Ni, 90Zr, 208Pb; calculated Gamow-Teller, M1 resonances, transition strengths, isovector spin-flip excitations. RPA, TDA formalisms, continuum effects.
doi: 10.1016/0370-2693(82)90179-4
1982ZA05 Phys.Rev. C26, 2185 (1982) Nilsson-Pairing Model for Double Beta Decay RADIOACTIVITY 48Ca, 76Ge; calculated double β-decay matrix element. Nilsson wave functions, pairing correlations, delta admixtures.
doi: 10.1103/PhysRevC.26.2185
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