NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = J.D.Vergados Found 73 matches. 2019EJ01 J.Phys.(London) G46, 025104 (2019) Neutron disappearance inside the nucleus RADIOACTIVITY 2H, 9,11Be, 15C(n); analyzed available data; deduced expected widths for neutron decay into a dark matter particle inside a nucleus.
doi: 10.1088/1361-6471/aaf55b
2018AV02 J. Cosmol. Astropart. Phys. 2018, 021 (2018) F.T.Avignone, III, R.J.Creswick, J.D.Vergados, P.Pirinen, P.C.Srivastava, J.Suhonen Estimating the flux of the 14.4 keV solar axions NUCLEAR STRUCTURE 57Fe; calculated energy levels, J, π, magnetic dipole moment using nuclear shell model. Comparison with available data.
doi: 10.1088/1475-7516/2018/01/021
2016VE05 J.Phys.(London) G43, 115002 (2016) J.D.Vergados, F.T.Avignone, III, M.Kortelainen, P.Pirinen, P.C.Srivastava, J.Suhonen, A.W.Thomas Inelastic WIMP-nucleus scattering to the first excited state in 125Te NUCLEAR STRUCTURE 125Te; calculated energy levels, J, π, B(E2), B(M1). Comparison with available data.
doi: 10.1088/0954-3899/43/11/115002
2016VE07 Int.J.Mod.Phys. E25, 1630007 (2016) J.D.Vergados, H.Ejiri, F.Simkovic Neutrinoless double beta decay and neutrino mass RADIOACTIVITY 76Ge, 82Se, 100Mo, 116Cd, 130Te, 136Xe, 150Nd(2β-); calculated neutrino mass sensitivities, nuclear matrix elements.
doi: 10.1142/S0218301316300071
2015VE08 Phys.Rev. D 92, 015015 (2015) J.D.Vergados, F.T.Avignone, III, P.Pirinen, P.C.Srivastava, M.Kortelainen, J.Suhonen Theoretical direct WIMP detection rates for transitions to the first excited state in 83Kr NUCLEAR STRUCTURE 83Kr; calculated energy levels, J, π, B(E2), B(M1), electric quadrupole moments. Comparison with available data.
doi: 10.1103/PhysRevD.92.015015
2012VE07 Rep.Prog.Phys. 75, 103601 (2012) J.D.Vergados, H.Ejiri, F.Simkovic Theory of neutrinoless double-beta decay RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 110Pd, 116Cd, 124Sn, 128,130Te, 136Xe, 150Nd(2β-); calculated nuclear matrix elements. Comparison with available data.
doi: 10.1088/0034-4885/75/10/106301
2011VE10 Phys.Rev. C 84, 044328 (2011) Transition operators entering neutrinoless double electron capture to excited nuclear states
doi: 10.1103/PhysRevC.84.044328
2006DI05 Nucl.Phys. A767, 259 (2006) P.C.Divari, J.D.Vergados, T.S.Kosmas Transition matrix elements for the exotic double-charge exchange μ- → e+ conversion in 27Al NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated transition matrix elements for neutrinoless conversion; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2005.12.003
2006EJ03 Phys.Lett. B 639, 218 (2006) H.Ejiri, Ch.C.Moustakidis, J.D.Vergados Dark matter search by exclusive studies of X-rays following WIMPs nuclear interactions
doi: 10.1016/j.physletb.2006.03.037
2005VE02 Nucl.Phys. B(Proc.Supp.) S143, 211 (2005) Neutrinoless Double Beta Decay in Theories Beyond the Standard Model RADIOACTIVITY 76Ge, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β-); calculated 0νββ-decay matrix elements, lepton violating parameters.
doi: 10.1016/j.nuclphysbps.2005.01.107
2005VE05 Int.J.Mod.Phys. E14, 751 (2005) J.D.Vergados, P.Quentin, D.Strottman Direct detection of supersymmetric dark matter: theoretical rates for transitions to excited states NUCLEAR STRUCTURE 127I; calculated matrix elements, transition rate for interaction with light supersymmetric particle.
doi: 10.1142/S0218301305003508
2002DI14 Nucl.Phys. A703, 409 (2002) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras The Exotic Double-Charge Exchange μ- → e+ Conversion in Nuclei NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated transition matrix elements for neutrinoless conversion; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01533-0
2002VE10 Phys.Rep. 361, 1 (2002) The neutrinoless double beta decay from a modern perspective
doi: 10.1016/S0370-1573(01)00068-0
2001DI21 Part. and Nucl., Lett. 104, 53 (2001) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras Exotic Muon-to-Positron Conversion in Nuclei: Partial transition sum evaluation by using shell model NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated matrix elements, strength distribution, total rate. Intermediate neutrino mixing model.
2000DI12 Phys.Rev. C61, 054612 (2000) P.C.Divari, T.S.Kosmas, J.D.Vergados, L.D.Skouras Shell Model Calculations for Light Supersymmetric Particle Scattering Off Light Nuclei NUCLEAR STRUCTURE 19F, 23Na, 29Si; calculated wave functions, matrix elements, form factors for elastic scattering of light supersymmetric particles. Shell model. Application to cold dark matter search discussed.
doi: 10.1103/PhysRevC.61.054612
2000FA18 Nucl.Phys. B587, 25 (2000) A.Faessler, T.S.Kosmas, S.Kovalenko, J.D.Vergados Exotic μ--e- Conversion in Nuclei and R-Parity Violating Supersymmetry NUCLEAR STRUCTURE 27Al, 48Ti, 208Pb; calculated μ--e- conversion transition matrix elements; deduced limits on R-parity violating parameters. Minimal supersymmetric standard model.
doi: 10.1016/S0550-3213(00)00446-6
2000VE05 Yad.Fiz. 63, No 7, 1213 (2000); Phys.Atomic Nuclei 63, 1137 (2000) Double-Beta Decay in Gauge Theories RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β-); calculated 0ν accompanied 2β decay T1/2, neutrino mass limits, lepton-violating parameters. Supersymmetry.
doi: 10.1134/1.855759
1999SI18 Phys.Rev. C60, 055502 (1999) F.Simkovic, G.Pantis, J.D.Vergados, A.Faessler Additional Nucleon Current Contributions to Neutrinoless Double β Decay RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β); calculated 0ν accompanied 2β-decay matrix elements; deduced nucleon current contributions.
doi: 10.1103/PhysRevC.60.055502
1998KO41 Yad.Fiz. 61, No 7, 1261 (1998); Phys.Atomic Nuclei 61, 1161 (1998) T.S.Kosmas, J.D.Vergados, A.Faessler Muon-Number-Violating Processes in Nuclei NUCLEAR REACTIONS 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb(μ-, e-), E not given; calculated exotic muon-electron conversion matrix elements, rates, mean excitation energies; deduced dominance of coherent mode.
1997KO20 J.Phys.(London) G23, 693 (1997) T.S.Kosmas, A.Faessler, J.D.Vergados The New Limits of the Neutrinoless (μ-, e-) Conversion Branching Ratio NUCLEAR REACTIONS 208Pb, 48Ti(μ-, e-), E not given; calculated exotic μ- → e- conversion ratio; deduced new limits on associated elementary particle parameters. Different models.
doi: 10.1088/0954-3899/23/6/008
1997KO26 Phys.Rev. C56, 526 (1997) T.S.Kosmas, A.Faessler, F.Simkovic, J.D.Vergados State-by-State Calculations for All Channels of the Exotic (μ-, e-) Conversion Process NUCLEAR STRUCTURE 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb; calculated coherent, total μ- → e- conversion matrix elements; deduceddependence on mass, Z. Quasiparticle RPA.
doi: 10.1103/PhysRevC.56.526
1996KO34 Phys.Rep. 264, 251 (1996) (μ-, e-) Conversion: A symbiosis of particle and nuclear physics NUCLEAR STRUCTURE 48Ti, 60Ni, 72Ge, 112Cd, 162Yb, 208Pb; calculated coherent (μ-, e-) conversion matrix elements. Shell model, RPA approaches comparison.
doi: 10.1016/0370-1573(95)00041-0
1996PA02 Phys.Rev. C53, 695 (1996) G.Pantis, F.Simkovic, J.D.Vergados, A.Faessler Neutrinoless Double Beta Decay within the Quasiparticle Random-Phase Approximation with Proton-Neutron Pairing RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe(2β); calculated 0ν-accompanied 2β-decay T1/2, limits on lepton nonconserving parameters. Quasiparticle RPA.
doi: 10.1103/PhysRevC.53.695
1996SI29 Nucl.Phys.(Proc.Suppl.) S48, 257 (1996) F.Simkovic, G.Pantis, J.D.Vergados, A.Faessler The QRPA Study of Neutrinoless Double Beta Decay with and without Proton-Neutron Pairing RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe; analyzed 0ν-accompanied 2β-decay T1/2 data; deduced lepton number nonconserving parameters lower limits. Quasiparticle RPA with, without proton-neutron pairing.
doi: 10.1016/0920-5632(96)00255-1
1996VE01 J.Phys.(London) G22, 253 (1996) Searching for Cold Dark Matter NUCLEAR STRUCTURE 3He, 19F, 23Na, 40Ca, 71Ga, 76,72Ge, 75As, 127I, 134Xe, 207Pb; calculated isospin, total coherent corrections, light supersymmetric particle scattering σ. Supersymmetric theories.
doi: 10.1088/0954-3899/22/2/010
1994KO09 Nucl.Phys. A570, 637 (1994) T.S.Kosmas, J.D.Vergados, O.Civitarese, A.Faessler Study of the Muon Number Violating (μ-, e-) Conversion in a Nucleus by using Quasi-Particle RPA NUCLEAR REACTIONS 48Ti(μ-, e-), E at rest; calculated total, coherent conversion rates. Quasiparticle RPA.
doi: 10.1016/0375-9474(94)90077-9
1993CH28 Nucl.Phys. A559, 526 (1993) H.C.Chiang, E.Oset, T.S.Kosmas, A.Faessler, J.D.Vergados Coherent and Incoherent (μ-, e-) Conversion in Nuclei NUCLEAR STRUCTURE A=12-238; calculated coherent, incoherent (μ-, e-) conversion matrix elements, form factors, widths. Flavour lepton number violating theories.
doi: 10.1016/0375-9474(93)90259-Z
1993LE09 Phys.Lett. 305B, 242 (1993) Neutrino Masses in Flipped SU(5)
doi: 10.1016/0370-2693(93)90114-W
1992KO03 Nucl.Phys. A536, 72 (1992) Nuclear Densities with Fractional Occupation Probabilities of the States NUCLEAR STRUCTURE 40Ca; calculated charge density distribution, charge form factor. Z=2-92; calculated mean square radii. Harmonic oscillator shell model, surface orbits fractional occupation probabilities.
doi: 10.1016/0375-9474(92)90246-G
1992PA07 J.Phys.(London) G18, 605 (1992) G.Pantis, A.Faessler, W.A.Kaminski, J.D.Vergados Description of the 0νββ Decay of 48Ca, 76Ge, 100Mo, 128,130Te RADIOACTIVITY 48Ca, 76Ge, 100Mo, 128,130Te(2β); calculated 0ν-accompanied 2β-decay T1/2, matrix elements; deduced lepton violating parameters limits. Quasiparticle RPA, no closure approximation.
doi: 10.1088/0954-3899/18/4/003
1992SI14 J.Phys.(London) G18, 1377 (1992) J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados Shell-Model Calculations in the A = 80-100 Mass Region: I. A study of the N = 50 nuclei NUCLEAR STRUCTURE 94Ru, 92Mo, 90Zr, 88Sr, 86Kr, 84Se, 93Tc, 91Nb, 89Y, 87Rb, 95Rh; calculated levels, B(λ). 96Pd; calculated levels. Shell model.
doi: 10.1088/0954-3899/18/8/012
1992SI15 J.Phys.(London) G18, 1401 (1992) J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados Shell-Model Calculations in the A = 80-100 Mass Region: II. A study of the N = 49, 48 nuclei NUCLEAR STRUCTURE 91Mo, 89Zr, 93Ru, 87Sr, 90Nb, 88Y, 92Ru, 90Mo, 88Zr, 86Sr, 91Tc, 89Nb; calculated levels, B(λ). 87Y; caluclated levels. Shell model.
doi: 10.1088/0954-3899/18/8/013
1991FA01 Phys.Rev. C43, R21 (1991) A.Faessler, W.A.Kaminski, G.Pantis, J.D.Vergados Double-β-Decay Matrix Elements RADIOACTIVITY 76Ge(2β); calculated 0ν associated 2β-decay matrix elements; deduced closure approximation validity.
doi: 10.1103/PhysRevC.43.R21
1991VE01 Phys.Rev. C44, 276 (1991) Pion Double-Charge-Exchange Reaction: Shell model formalism NUCLEAR STRUCTURE A=14, 48, 42; calculated 0+ → 0+ transition matrix elements. Shell model, pion double charge exchange reaction.
doi: 10.1103/PhysRevC.44.276
1990KO10 Nucl.Phys. A510, 641 (1990) Study of the Flavour Violating (μ-, e-) Conversion in Nuclei NUCLEAR STRUCTURE A=4-208; calculated total (μ-, e-) conversion rate; deduced coherent conversion rate ratio. Shell model, effective operators.
doi: 10.1016/0375-9474(90)90353-N
1990PA15 Phys.Lett. 242B, 1 (1990) Neutrinoless Double Beta Decay Matrix Elements Beyond Closure Approximation RADIOACTIVITY 48Ca(2β); calculated neutrinoless β-decay matrix elements.
doi: 10.1016/0370-2693(90)91584-X
1990VE03 Nucl.Phys. A506, 482 (1990) Theory of 0ν ββ-Decay Beyond Closure Approximation
doi: 10.1016/0375-9474(90)90199-V
1989ER03 Nucl.Phys. A495, 602 (1989) The Effects of Pion-Exchange Corrections on the 2ν ββ Decay Nuclear Matrix Elements RADIOACTIVITY 48Ca(2β); calculated two-neutrino accompanied β-decay matrix element. Pion exchange corrections.
doi: 10.1016/0375-9474(89)90362-X
1989KO01 Phys.Lett. 217B, 19 (1989) Sum Rules for the Inclusive μ-e Conversion Exotic Reaction NUCLEAR STRUCTURE A=4-208; calculated (μ-, e-) total conversion rate. Sum rules.
doi: 10.1016/0370-2693(89)91508-6
1989VE02 Phys.Lett. 218B, 119 (1989) Does the Δ((3/2), (3/2)) Resonance Contribute to 0+ → 0+ ββ-Decay ( Question ) NUCLEAR STRUCTURE 48Ca(2β); calculated β-decay rate. Nucleon-Δ contribution.
doi: 10.1016/0370-2693(89)91404-4
1989VE04 Nucl.Phys. A492, 654 (1989) J.D.Vergados, S.B.Khadkikar, A.Faessler Non-Static Contributions to the 0+ → 0+ ββ-Decay in the Presence of the Δ((3/2), (3/2)) Resonance NUCLEAR STRUCTURE 48Ca(2β); calculated nonstatic contribution to two β-decay in presence of Δ resonance.
doi: 10.1016/0375-9474(89)90113-9
1988KO30 Phys.Lett. 215B, 460 (1988) Nuclear Matrix Elements for the Coherent μ-e Conversion Process NUCLEAR STRUCTURE A ≤ 200; analyzed n, p elastic nuclear form factor systematics; deduced coherent (μ-e) conversion process matrix elements.
doi: 10.1016/0370-2693(88)91341-X
1988SI03 Phys.Rev. C37, 1229 (1988) J.Sinatkas, L.D.Skouras, J.D.Vergados Shell Model Nuclear Matrix Elements for Double β Decay RADIOACTIVITY 76Ge, 80,82Se, 86Kr(2β); calculated β-decay matrix elements; deduced neutrino mass limits. Shell model.
doi: 10.1103/PhysRevC.37.1229
1988VE09 Nucl.Phys. A490, 556 (1988) J.D.Vergados, A.Faessler, T.Tomoda The Δ((3/2), (3/2)) Contribution to the 0+ → 2+ ββ-Decay Transitions RADIOACTIVITY 48Ca(2β); calculated matrix elements; deduced isobar Δ role.
doi: 10.1016/0375-9474(88)90013-9
1988VO07 Phys.Lett. 212B, 259 (1988) P.Vogel, M.Ericson, J.D.Vergados Sum Rules for Two-Particle Operators and Double Beta Decay RADIOACTIVITY 76Ge, 54Fe(2β); calculated double Gamow-Teller, Fermi operator sum rules, Gamow-Teller transition strength.
doi: 10.1016/0370-2693(88)91313-5
1985VE07 Nucl.Phys. B250, 618 (1985) Six-Quark Clusters and Neutrinoless Double β-Decay NUCLEAR STRUCTURE 16O, 48Ca, 56Ni; calculated six quark cluster probability in nuclear interior. RADIOACTIVITY 48Ca(2β); calculated heavy Majorana neutrino associated decay matrix elements. Six quark clusters.
doi: 10.1016/0550-3213(85)90497-3
1984VE02 Nucl.Phys. B234, 213 (1984) Neutrinoless Double β-Decay to Excited States RADIOACTIVITY 48Ca(2β); calculated neutrinoless double β-decay T1/2; deduced lepton violating parameter lower limits. Gauge theories.
doi: 10.1016/0550-3213(84)90232-3
1983LE21 Nucl.Phys. B224, 137 (1983) Study of the Lepton-Violating (μ-, e+) Reaction in Modern Gauge Theories NUCLEAR REACTIONS 58Ni(μ-, e+), E at rest; calculated lepton violating reaction branching ratio upper limit. Gauge theory, left-, right-handed symmetric models.
doi: 10.1016/0550-3213(83)90317-6
1983SK04 Phys.Rev. C28, 2122 (1983) Double β-Decay Nuclear Matrix Elements for the A = 48 and A = 58 Systems NUCLEAR STRUCTURE 48Ca, 58Ni; calculated double β-decay matrix elements; deduced β+-decay T1/2 for A=58, lepton violating parameters for A=48.
doi: 10.1103/PhysRevC.28.2122
1981MO22 Phys.Rev.Lett. 47, 1713 (1981) New Contribution to Neutrinoless Double Beta Decay in Gauge Models RADIOACTIVITY 48Ca; calculated neutrinoless double β-decay contribution. Gauge Models.
doi: 10.1103/PhysRevLett.47.1713
1981PI13 Phys.Rev. C24, 2343 (1981) Lepton Nonconserving (μ-, e+) Raction to Individual Nuclear States NUCLEAR REACTIONS 40Ca(μ-, e+), E at rest; calculated branching ratio. Gauge model.
doi: 10.1103/PhysRevC.24.2343
1978GO11 Phys.Rev. C18, 944 (1978) B.Goulard, A.Laverne, J.D.Vergados Panofsky Ratio, Threshold Pion Photoproduction, and Axial-Vector Form Factor in the A = 3 System NUCLEAR REACTIONS 3He(π-, γ), 3He(π-, π0), E=0 MeV; calculated σ, Panofsky ratio.
doi: 10.1103/PhysRevC.18.944
1977GO13 Phys.Rev. C16, 1999 (1977) B.Goulard, B.Lorazo, H.Primakoff, J.D.Vergados Beta Decays and Related Processes in the A = 14 Nuclei RADIOACTIVITY 14N, 14C, 14O; analyzed decay processes, wave functions.
doi: 10.1103/PhysRevC.16.1999
1977VE05 Phys.Rev. C16, 292 (1977) Threshold π0 Photoproduction from Complex Nuclear Targets NUCLEAR REACTIONS 4He, 6Li(γ, π0); calculated σ(θ).
doi: 10.1103/PhysRevC.16.292
1976PI01 Phys.Rev. C13, 412 (1976) S.Pittel, C.M.Vincent, J.D.Vergados Perturbative Approximations to the Effective Interaction: Comparisons with Exact Results for Large Matrices NUCLEAR STRUCTURE 18O; calculated perturbative approximations to the effective interaction. Pade approximants.
doi: 10.1103/PhysRevC.13.412
1976VE02 Phys.Rev. C13, 865 (1976) Double β-Decay Nuclear Matrix Elements and Lepton Conservation RADIOACTIVITY 48Ca, 130,128Te; calculated double β-decay nuclear matrix elements.
doi: 10.1103/PhysRevC.13.865
1975BA52 Phys.Rev. C12, 921 (1975) H.W.Baer, J.A.Bistirlich, N.de Botton, S.Cooper, K.M.Crowe, P.Truol, J.D.Vergados Excitation of Giant Magnetic and Spin-Isospin Dipole States in Radiative π Capture on 14N and 10B NUCLEAR REACTIONS 10B, 14N(π-, γ); measured γ-spectrum. 10Be, 14C levels deduced γ-branching.
doi: 10.1103/PhysRevC.12.921
1975VE01 Nucl.Phys. A239, 271 (1975) The T = T(z) + 2 GDR and the Dipole States of the A = 6 and 14 Nuclei NUCLEAR STRUCTURE 14N, 14C, 6Li, 6He; calculated dipole transitions.
doi: 10.1016/0375-9474(75)90451-0
1975VE05 Phys.Rev. C12, 1278 (1975) Shell Model Theory of Radiative Pion Capture NUCLEAR REACTIONS 16O(π-, γ); calculated wave functions. 16N calculated branching ratio to dipole, quadrupole states.
doi: 10.1103/PhysRevC.12.1278
1974BA44 Phys.Rev. C10, 1140 (1974) H.W.Baer, J.A.Bistirlich, N.de Botton, S.Cooper, K.M.Crowe, P.Truol, J.D.Vergados Radiative Pion Capture in 209Bi NUCLEAR REACTIONS 209Bi(π-, γ); measured σ(E, Eγ). 209Pb deduced levels, γ-width.
doi: 10.1103/PhysRevC.10.1140
1974LE25 Phys.Lett. 53B, 125 (1974) Realistic Calculations of the (π-, nγ) Reaction NUCLEAR REACTIONS 14N(π-, nγ), (π-, γ); calculated capture rate.
doi: 10.1016/0370-2693(74)90510-3
1974VE02 Nucl.Phys. A220, 259 (1974) The Structure, Transition Probabilities and the π- Capture Rates of the A = 6 Nuclei NUCLEAR STRUCTURE 6Li; calculated levels, level-width, J, π, μ, quadrupole moment. 6He calculated log ft.
doi: 10.1016/0375-9474(74)90718-0
1974VE10 Phys.Lett. 53B, 151 (1974) The Fragmentation of the Giant Dipole Resonance in the Schematic Model NUCLEAR STRUCTURE A=14; calculated dipole transitions, B(E1).
doi: 10.1016/0370-2693(74)90517-6
1973DI03 Phys.Rev. C7, 705 (1973) E.M.Diener, J.F.Amann, P.Paul, J.D.Vergados Isospin Effects in the Giant Dipole Resonance of 42Ca NUCLEAR REACTIONS 41K(p, γ), E=4-13 MeV; measured σ(E;Eγ, θ). 42Ca deduced giant dipole resonance structure, level-width.
doi: 10.1103/PhysRevC.7.705
1972HE04 Phys.Rev. C5, 791 (1972) S.H.Henson, S.Cochavi, D.B.Fossan, J.D.Vergados Experimental 0+2(2.12 Mev) → 2+1(1.46 Mev) B(E2) Strength and Pairing-Vibration Calculations in 40Ar NUCLEAR REACTIONS 40Ar(p, p'γ), E=5.3 MeV; measured p'γ-delay. 40Ar level deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.5.791
1972VE07 Phys.Lett. 41B, 560 (1972) Importance of Momentum Dependent Terms in Radiative Pion Capture NUCLEAR REACTIONS 6Li(π-, γ), E approx 0; calculated capture rate; analyzed contribution of momentum-dependent terms.
doi: 10.1016/0370-2693(72)90633-8
1971VE01 Phys.Lett. 34B, 121 (1971) How Pure Are the Single Particle States in Pb Region (Question) NUCLEAR STRUCTURE 207,209Pb, 209Bi, 207Tl; calculated levels.
doi: 10.1016/0370-2693(71)90684-8
1971VE02 Phys.Lett. 34B, 458 (1971) Microscopic Description of 2p-2h States in 208Pb NUCLEAR STRUCTURE 208Pb; calculated levels, 2p-2h states. Microscopic description realistic N-N interaction.
doi: 10.1016/0370-2693(71)90653-8
1971VE05 Nucl.Phys. A166, 285 (1971) First-Forbidden Unique β-Decays in the Sr Region RADIOACTIVITY 88Rb, 89Sr, 90Y, 90Sr; calculated first-forbidden unique β-decay moments.
doi: 10.1016/0375-9474(71)90431-3
1971VE06 Phys.Lett. 35B, 93 (1971) Electric Dipole Transitions in 88Sr and 90Zr NUCLEAR STRUCTURE 88Sr, 90Zr; calculated E1 transition widths. Shell model wave functions, definite isospin.
doi: 10.1016/0370-2693(71)90227-9
1971VE07 Nucl.Phys. A168, 225 (1971) Energy Spectrum and Dipole Transitions of 89Y NUCLEAR STRUCTURE 89Y; calculated levels, level-width for dipole transitions. Bound shell-model formalism.
doi: 10.1016/0375-9474(71)90790-1
1971VE09 Phys.Lett. 36B, 12 (1971) Configuration Mixing Effects on M1 Transitions and Magnetic Moments in Pb Region NUCLEAR STRUCTURE 207Pb, 207Tl, 208Pb, 208Tl, 206Pb; calculated μ, B(M1). Shell model, configuration mixing effects.
doi: 10.1016/0370-2693(71)90307-8
1969JA11 Phys.Letters 30B, 455 (1969) A.D.Jackson, T.T.S.Kuo, J.D.Vergados Test of the Pairing-Vibration Model in 40A NUCLEAR STRUCTURE 40Ar; calculated levels. Pairing- vibration model, Hamada-Johnston potential, core polarization corrections.
doi: 10.1016/0370-2693(69)90168-3
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