NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.R.Stone Found 40 matches. 2022NE01 Phys.Rev. C 105, 025806 (2022) W.G.Newton, S.Cantu, S.Wang, A.Stinson, M.A.Kaltenborn, J.R.Stone Glassy quantum nuclear pasta in neutron star crusts
doi: 10.1103/PhysRevC.105.025806
2020AN18 Phys.Rev. C 102, 065801 (2020) S.Antic, J.R.Stone, J.C.Miller, K.L.Martinez, P.A.M.Guichon, A.W.Thomas Outer crust of a cold, nonaccreting neutron star within the quark-meson-coupling model NUCLEAR STRUCTURE Z=26-50, N=20-90; calculated nuclear binding energies, two-neutron drip line using the QMCπ-III mass model, and compared with experimental data. 56Fe, 62,64,66,78Ni, 80Zn, 82Ge, 84Se, 86,118,120Kr, 120,122,124Sr, 121Y, 122Zr, 124Mo, 126Ru; calculated numerical results of the equation of state (EOSs) in the outer crust of cold nonaccreting, nonrotating neutron stars, such as baryon number densities at the bottom and top of each layer, and neutron and electron chemical potentials, and properties of individual layers in the outer crust. Comparison with results from FRDM, HFB24, and NL3 mass models.
doi: 10.1103/PhysRevC.102.065801
2020BA15 Acta Phys.Pol. B51, 611 (2020) P.Baczyk, M.Konieczka, K.M.L.Martinez, S.Antic, P.A.M.Guichon, W.Satula, J.R.Stone, A.W.Thomas On Introducing Charge-Symmetry-Breaking Terms to Nuclear Energy Density Functionals
doi: 10.5506/APhysPolB.51.611
2020MA43 Phys.Rev. C 102, 034304 (2020) K.L.Martinez, A.W.Thomas, P.A.M.Guichon, J.R.Stone Tensor and pairing interactions within the quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, N=14-38; Z=28, N=20-50; Z=50, N=50-88; Z=82, N=96-138; calculated binding energies with and without tensor contribution, two-neutron shell gaps. 40,48Ca, 56,78Ni, 100,132Sn; calculated proton and neutron single-particle states, deformation energies, spin-orbit splittings with and without tensor contribution. 90,92,94,96,98,100,102,104,106,108,110,112Zr; calculated β2 deformation parameters and deformation energies. 254,256,254,256,258,260,262,264Fm, 254,256,258,260,262,264,266,268Rf; calculated two-neutron shell gaps. Quark-meson coupling (QMC) model (QMCπ-III-T), with the density functional which included tensor component, and pairing interaction from the QMC framework. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.034304
2019MA57 Phys.Rev. C 100, 024333 (2019) K.L.Martinez, A.W.Thomas, J.R.Stone, P.A.M.Guichon Parameter optimization for the latest quark-meson coupling energy-density functional NUCLEAR STRUCTURE Z=20, 28, 50, 82; N=20, 28, 50, 82, 126; calculated binding energies, rms charge radii, and pairing gaps for 70 nuclei. Z=8-96, N=8-160; calculated binding energies, rms charge radii, and S(2n) for 739 even-even nuclei. Z=20, N=16-36; Z=28, N=26-52; Z=50, N=52-86; Z=82, N=98-142; calculated S(2n) for even-even nuclei. Z=20, A=34-58; Z=82, A=178-220; calculated isotopic shifts for even-even nuclei. 36,38,40,48Ca, 54Fe, 58,60,64Ni, 90Zr, 112,116,124Sn, 208Pb; calculated skin thicknesses. 40Ca, 78Ni, 132Sn; calculated proton and neutron single-particle states. Z=64, A=134-170; calculated B(E2) and β2 for the first 2+ states in even-even nuclei. 90Zr, 116Sn, 144Sm, 208Pb; calculated energies of giant monopole resonances (GMR). Z>96, A=232-294; calculated binding energies for superheavy nuclei. HF+BCS calculations with quark-meson-coupling (QMC) model, using QMCπ-II energy density functional. Optimization of model parameters by detailed comparisons and fittings with the experimental data. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.100.024333
2019ST10 Phys.Rev. C 100, 044302 (2019) J.R.Stone, K.Morita, P.A.M.Guichon, A.W.Thomas Physics of even-even superheavy nuclei with 96 < Z < 110 in the quark-meson-coupling model NUCLEAR STRUCTURE 244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm; calculated ground state binding energies and compared to values in AME-2016. 234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280Cm, 236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282Cf, 238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284Fm, 240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286No, 242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288Rf, 244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290Sg, 246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Hs, 248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294Ds; calculated deformation energies and neutron pairing energies as a function of the quadrupole deformation parameter β2, S(2n), Q(α), shape coexistence in N=168-184 Sg nuclei. 40,48Ca, 56,68,78Ni, 90Zr, 100,132Sn, 146Gd, 208Pb; calculated proton and neutron single-particle energies. 244Cm, 248Cf, 252Fm, 256No, 260Rf, 264Sg, 268Hs, 272Ds; calculated neutron single-particle states. Quark-meson-coupling (QMC) model. Comparison with available experimental data from AME-2016 and databases at NNDC.
doi: 10.1103/PhysRevC.100.044302
2017OH01 J.Phys.(London) G44, 044010 (2017) T.Ohtsubo, S.Roccia, N.J.Stone, J.R.Stone, C.Gaulard, U.Koster, J.Nikolov, G.S.Simpson, M.Veskovic The on-line low temperature nuclear orientation facility NICOLE
doi: 10.1088/1361-6471/aa5f22
2017ST13 Phys.Rev. C 96, 014612 (2017) J.R.Stone, P.Danielewicz, Y.Iwata Proton and neutron density distributions at supranormal density in low- and medium-energy heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 48Ca(48Ca, X), 100Sn(100Sn, X), 120Sn(120Sn, X), 48Ca(40Ca, X), 120Sn(100Sn, X), E<800 MeV/nucleon; calculated time evolution of maximal proton and neutron densities, Contour plots of neutron and proton densities, maximum neutron and proton densities and asymmetry parameter. Boltzmann-Uhlenbeck-Uehling (pBUU) transport model, with time-dependent Hartree-Fock (TDHF) model and Skyrme interaction for heavy-ion collisions at E<40 MeV/nucleon. 40,48Ca, 100,120Sn; calculated neutron and proton densities as a function of distance from the center of nucleus from static Hartree-Fock (HF) and Thomas-Fermi (TF) equations.
doi: 10.1103/PhysRevC.96.014612
2016ST07 Phys.Rev.Lett. 116, 092501 (2016) J.R.Stone, P.A.M.Guichon, P.G.Reinhard, A.W.Thomas Finite Nuclei in the Quark-Meson Coupling Model NUCLEAR STRUCTURE 270Db, 264,255Hs, 260,262Sg, 256,258Rf, 254,256No, 246,248,250,252,254,256Fm; calculated ground-state binding energies, deformation parameters. Effective quark-meson coupling (QMC) energy density functional (EDF), comparison with available data.
doi: 10.1103/PhysRevLett.116.092501
2016ST11 Eur.Phys.J. A 52, 66 (2016) Neutron stars interiors: Theory and reality NUCLEAR STRUCTURE 246,248,250,252,254,256Fm, 254,256No, 256,258Rf, 260,262Sg, 264,266Hs, 270Ds; calculated binding energy, mass excess, quadrupole deformation using QMC (Quark-Meson-CouplingModel). Binding energy compared to data, both deformation and binding energy to other calculations.
doi: 10.1140/epja/i2016-16066-5
2014DU14 Phys.Rev. C 90, 055203 (2014) M.Dutra, O.Lourenco, S.S.Avancini, B.V.Carlson, A.Delfino, D.P.Menezes, C.Providencia, S.Typel, J.R.Stone Relativistic mean-field hadronic models under nuclear matter constraints
doi: 10.1103/PhysRevC.90.055203
2014MU03 Phys.Rev. C 89, 044309 (2014) S.Muto, N.J.Stone, C.R.Bingham, J.R.Stone, P.M.Walker, G.Audi, C.Gaulard, U.Koster, J.Nikolov, K.Nishimura, T.Ohtsubo, Z.Podolyak, L.Risegari, G.S.Simpson, M.Veskovic, W.B.Walters Magnetic properties of 177Hf and 180Hf in the strong-coupling deformed model NUCLEAR REACTIONS Ta, W(p, X), E=1.4 GeV; measured Eγ, Iγ, γ(θ, temp), resonance, magnetic dipole moment of 37/2- isomer in 177Hf and 8- isomer in 180Hf using NICOLE on-line low-temperature nuclear orientation system and NMR at ISOLDE-CERN facility. 177,180Hf; deduced high-spin levels, multipolarity, mixing ratio, (gK-gR)/Q0. Comparison with previous experimental results. NUCLEAR MOMENTS 177,180Hf; measured magnetic moments of high-spin K-isomers by on-line low-temperature nuclear orientation combined with NMR using NICOLE system at ISOLDE-CERN facility. Discussed dependence of gR parameter upon the quasiproton and quasineutron structure of high-K isomeric states in this mass region.
doi: 10.1103/PhysRevC.89.044309
2014PA54 Phys.Rev. C 90, 065802 (2014) Phase transitions in core-collapse supernova matter at sub-saturation densities
doi: 10.1103/PhysRevC.90.065802
2014ST09 Phys.Rev. C 89, 044316 (2014) J.R.Stone, N.J.Stone, S.A.Moszkowski Incompressibility in finite nuclei and nuclear matter NUCLEAR STRUCTURE 56Fe, 58,60Ni, 90Zr, 92Mo, 106,110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 144,148Sm, 208Pb; analyzed experimental data for energies of giant-monopole resonances (GMR); deduced incompressibility (compression modulus) K0, and expressed in terms of leptodermous expansion with volume, surface, isospin, and Coulomb coefficients. Role of surface properties in vibrating nuclei. Developed a self-consistent simple (toy) model to connect surface properties of a vibrating nucleus and its incompressibility.
doi: 10.1103/PhysRevC.89.044316
2014WH01 Phys.Rev. C 89, 065801 (2014) D.L.Whittenbury, J.D.Carroll, A.W.Thomas, K.Tsushima, J.R.Stone Quark-meson coupling model, nuclear matter constraints, and neutron star properties
doi: 10.1103/PhysRevC.89.065801
2012DU06 Phys.Rev. C 85, 035201 (2012) M.Dutra, O.Lourenco, J.S.Sa Martins, A.Delfino, J.R.Stone, P.D.Stevenson Skyrme interaction and nuclear matter constraints
doi: 10.1103/PhysRevC.85.035201
2012OH01 Phys.Rev.Lett. 109, 032504 (2012) T.Ohtsubo, N.J.Stone, J.R.Stone, I.S.Towner, C.R.Bingham, C.Gaulard, U.Koster, S.Muto, J.Nikolov, K.Nishimura, G.S.Simpson, G.Soti, M.Veskovic, W.B.Walters, F.Wauters Magnetic Dipole Moment of the Doubly-Closed-Shell Plus One Proton Nucleus 49Sc NUCLEAR MOMENTS 49Sc; measured hyperfine field, β asymmetry; deduced magnetic dipole moment. Comparison with available data. NUCLEAR STRUCTURE 41,49Sc; calculated magnetic dipole moment.
doi: 10.1103/PhysRevLett.109.032504
2012TS04 Phys.Rev. C 86, 015803 (2012) M.B.Tsang, J.R.Stone, F.Camera, P.Danielewicz, S.Gandolfi, K.Hebeler, C.J.Horowitz, J.Lee, W.G.Lynch, Z.Kohley, R.Lemmon, P.Moller, T.Murakami, S.Riordan, X.Roca-Maza, F.Sammarruca, A.W.Steiner, I.Vidana, S.J.Yennello Constraints on the symmetry energy and neutron skins from experiments and theory NUCLEAR STRUCTURE 208Pb; analyzed neutron-skin thickness, symmetry energy constraints. Contributions of three-body forces in neutron matter models.
doi: 10.1103/PhysRevC.86.015803
2012ZH08 Phys.Rev. C 85, 034336 (2012) S.Zhu, R.V.F.Janssens, M.P.Carpenter, C.J.Chiara, R.Broda, B.Fornal, N.Hoteling, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, I.Stefanescu, J.R.Stone, W.B.Walters, X.Wang, J.Wrzesinski Nature of yrast excitations near N=40: Level structure of 67Ni NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(t) using Gammasphere array at ATLAS facility. 67Ni; deduced high-spin levels, J, π, half-life, multipolarity, mixing ratio, configurations. Comparison with shell-model calculations. 64Ni; measured Eγ; deduced levels.
doi: 10.1103/PhysRevC.85.034336
2009AR04 Acta Phys.Pol. B40, 437 (2009) O.Arndt, S.Hennrich, N.Hoteling, C.J.Jost, B.E.Tomlin, J.Shergur, K.-L.Kratz, P.F.Mantica, B.A.Brown, R.V.F.Janssens, W.B.Walters, B.Pfeiffer, A.Wohr, S.Zhu, R.Broda, M.P.Carpenter, B.Fornal, A.A.Hecht, W.Krolas, T.Lauritsen, T.Pawlat, J.Pereira, D.Seweryniak, I.Stefanescu, J.R.Stone, J.Wrzesinski Structure of Neutron-Rich Odd-Mass 127, 129, 131In Populated in the Decay of 127, 129, 131Cd RADIOACTIVITY 127,129,131Cd(β-); measured Iγ, Eγ; deduced Jπ, level scheme. Comparison with calculations.
2009FL03 Phys.Rev.Lett. 103, 142501 (2009) K.T.Flanagan, P.Vingerhoets, M.Avgoulea, J.Billowes, M.L.Bissell, K.Blaum, B.Cheal, M.De Rydt, V.N.Fedosseev, D.H.Forest, Ch.Geppert, U.Koster, M.Kowalska, J.Kramer, K.L.Kratz, A.Krieger, E.Mane, B.A.Marsh, T.Materna, L.Mathieu, P.L.Molkanov, R.Neugart, G.Neyens, W.Nortershauser, M.D.Seliverstov, O.Serot, M.Schug, M.A.Sjoedin, J.R.Stone, N.J.Stone, H.H.Stroke, G.Tungate, D.T.Yordanov, Yu.M.Volkov Nuclear Spins and Magnetic Moments of 71, 73, 75Cu: Inversion of π2p3/2 and π1f5/2 Levels in 75Cu NUCLEAR MOMENTS 71,73,75Cu; measured hfs spectra; deduced ground-state spins, magnetic moments, hyperfine parameters, shell inversion. Comparison with large-scale shell-model calculation.
doi: 10.1103/PhysRevLett.103.142501
2009GO09 Phys.Rev. C 79, 034316 (2009) C.Goodin, J.R.Stone, N.J.Stone, A.V.Ramayya, A.V.Daniel, J.H.Hamilton, K.Li, J.K.Hwang, G.M.Ter-Akopian, J.O.Rasmussen g factors of first 2+ states of neutron-rich Xe, Ba, and Ce isotopes NUCLEAR MOMENTS 140,142Xe, 146Ba, 146,148Ce; measured g factors of first 2+ states by integral perturbed angular correlation (IPAC) method. 130,132,134,136,138,140,142Xe, 130,132,134,136,138,140,142,144,146Ba, 140,142,146,148Ce, 148,150Nd, 152,154Sm, 154,156,158,160Gd, 160,162,164Dy; systematics of experimental and theoretical g factors and ratio of proton to neutron holes outside the nearest closed shell. Comparison with interacting boson model-2 and rotation-vibration model calculations. 146Ba, 146,148Ce; deduced ratio of neutron to proton deformation. RADIOACTIVITY 252Cf(SF); measured Eγ, (particle)γ-, γγ-coin, attenuated γγ(θ). 136,140,142Xe, 142,146Ba, 146,148Ce; deduced levels, J, g factors.
doi: 10.1103/PhysRevC.79.034316
2009NE06 Phys.Rev. C 79, 055801 (2009) Modeling nuclear "pasta" and the transition to uniform nuclear matter with the 3D Skyrme-Hartree-Fock method at finite temperature: Core-collapse supernovae NUCLEAR STRUCTURE 16O, 40Ca, 56Fe; calculated binding energies and rms radii. A=100-2000; calculated free energy functions versus nucleon number, neutron density profiles and energy deformation surfaces. Implications for Core-collapse supernovae. Three-dimensional finite temperature Skyrme-Hatree-Fock+BCS calculations for inhomogeneous phase of bulk nuclear matter using computer code TAMAR.
doi: 10.1103/PhysRevC.79.055801
2009PA16 Phys.Rev. C 79, 044309 (2009) D.Pauwels, O.Ivanov, N.Bree, J.Buscher, T.E.Cocolios, M.Huyse, Yu.Kudryavtsev, R.Raabe, M.Sawicka, J.Van de Walle, P.Van Duppen, A.Korgul, I.Stefanescu, A.A.Hecht, N.Hoteling, A.Wohr, W.B.Walters, R.Broda, B.Fornal, W.Krolas, T.Pawlat, J.Wrzesinski, M.P.Carpenter, R.V.F.Janssens, T.Lauritsen, D.Seweryniak, S.Zhu, J.R.Stone, X.Wang Structure of 65, 67Co studied through the β decay of 65, 67Fe and a deep-inelastic reaction RADIOACTIVITY 65,65mFe, 65Co, 67Fe(β-)[from 238U(p, F), E=30 MeV]; measured Eγ, Iγ, γγ-, βγ-coin, half-lives. 65Co, 65Ni, 67Co; deduced levels, J, π, configurations. 61,63,65Co; level systematics. Interpretation in terms of core coupled states with proton intruder orbitals. NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin. 65Co; deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.79.044309
2009RI14 Eur.Phys.J. A 42, 307 (2009) L.Risegari, A.Astier, G.Audi, S.Cabaret, C.Gaulard, G.Georgiev, N.J.Stone, J.R.Stone POLAREX; Study of polarized exotic nuclei at millikelvin temperatures
doi: 10.1140/epja/i2009-10779-4
2009ST05 Phys.Rev. C 79, 034319 (2009) I.Stefanescu, W.B.Walters, R.V.F.Janssens, N.Hoteling, R.Broda, M.P.Carpenter, B.Fornal, A.A.Hecht, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, J.R.Stone, X.Wang, A.Wohr, J.Wrzesinski, S.Zhu Levels above the 19/2- isomer in 71Cu: Persistence of the N=40 neutron shell gap NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin. 71Cu; deduced levels, J, π, configurations. 70Ni, 71Cu, 92Mo; level systematics. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.79.034319
2009ST12 Phys.Rev. C 79, 064302 (2009) I.Stefanescu, W.B.Walters, R.V.F.Janssens, S.Zhu, R.Broda, M.P.Carpenter, C.J.Chiara, B.Fornal, B.P.Kay, F.G.Kondev, W.Krolas, T.Lauritsen, C.J.Lister, E.A.McCutchan, T.Pawlat, D.Seweryniak, J.R.Stone, N.J.Stone, J.Wrzesinski Identification of the g9/2-proton bands in the neutron-rich 71, 73, 75, 77Ga nuclei NUCLEAR REACTIONS 238U(76Ge, X), E=530 MeV; measured Eγ, Iγ, γγ-coin. 71,73,75,77Ga; deduced levels, J, π. Discussed level systematics of A=65-77, odd-A Ga and Cu nuclides.
doi: 10.1103/PhysRevC.79.064302
2009ST28 Eur.Phys.J. A 42, 407 (2009) I.Stefanescu, W.B.Walters, P.F.Mantica, B.A.Brown, A.D.Davies, A.Estrade, P.T.Hosmer, N.Hoteling, S.N.Liddick, W.D.M.Rae, T.J.Mertzimekis, F.Montes, A.C.Morton, W.F.Mueller, M.Ouellette, E.Pellegrini, P.Santi, D.Seweryniak, H.Schatz, J.Shergur, A.Stolz, J.R.Stone, B.E.Tomlin Spectroscopy of exotic 121, 123, 125Ag produced in fragmentation reactions NUCLEAR REACTIONS 9Be(136Xe, X)121Pd/123Ag/125Ag, E=120 MeV/nucleon; measured Eγ, Iγ, γγ-, (fragment)γ-coin. 121,123,125Ag; deduced levels, J, π, T1/2. Comparison with shell model and systematics. RADIOACTIVITY 121Pd(β-) [from 9Be(136Xe, X), E=120 MeV/nucleon]; measured Eγ, Iγ, γγ-, (fragment)γ-coin. 121Ag; deduced levels, J, π. Comparison with shell model and systematics.
doi: 10.1140/epja/i2008-10754-7
2008BE14 Phys.Lett. B 664, 241 (2008) N.Benczer-Koller, G.J.Kumbartzki, G.Gurdal, C.J.Gross, A.E.Stuchbery, B.Krieger, R.Hatarik, P.O'Malley, S.Pain, L.Segen, C.Baktash, J.Beene, D.C.Radford, C.H.Yu, N.J.Stone, J.R.Stone, C.R.Bingham, M.Danchev, R.Grzywacz, C.Mazzocchi Measurement of g factors of excited states in radioactive beams by the transient field technique: 132Te NUCLEAR REACTIONS C(132Te, 132Te'), E=396 MeV; measured Eγ, Iγ, (particle)γ-coin. 132Te; deduced g-factor.
doi: 10.1016/j.physletb.2008.05.048
2008GO28 Phys.Rev. C 78, 044331 (2008) C.Goodin, N.J.Stone, A.V.Ramayya, A.V.Daniel, J.R.Stone, J.H.Hamilton, K.Li, J.K.Hwang, Y.X.Luo, J.O.Rasmussen, A.Gargano, A.Covello, G.M.Ter-Akopian g factors, spin-parity assignments, and multipole mixing ratios of excited states in N = 82 isotones 134Te, 135I RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, angular correlations, g-factors. 134Te, 135I; deduced levels, J, π, mixing ratios. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.78.044331
2008HO05 Phys.Rev. C 77, 044314 (2008) N.Hoteling, W.B.Walters, R.V.F.Janssens, R.Broda, M.P.Carpenter, B.Fornal, A.A.Hecht, M.Hjorth-Jensen, W.Krolas, T.Lauritsen, T.Pawlat, D.Seweryniak, J.R.Stone, X.Wang, A.Wohr, J.Wrzesinski, S.Zhu Rotation-aligned coupling in 61Fe NUCLEAR REACTIONS 238U(64Ni, X), E=430 MeV; measured Eγ, Iγ, γγ-coin. 61Fe; deduced levels, J, π. 59Fe; measured Eγ, Iγ. 56,57,58,59,60Fe; systematics. Comparisons with shell model and particle-triaxial rotor model.
doi: 10.1103/PhysRevC.77.044314
2008ZA01 Acta Phys.Pol. B39, 411 (2008) D.Zakoucky, J.R.Stone, G.Goldring, N.J.Stone, N.Severijns, M.Hass, T.Giles, U.Koester, I.S.Kraev, S.Lakshmi, M.Lindroos, F.Wauters Parity Non-Conservation Observed in Nuclear γ-Decay of 180mHf RADIOACTIVITY 180Hf(IT); measured Eγ, Iγ as a function of temperature and nuclear orientation. Deduced assymetry of the isomeric transition, parity mixing.
2007ST01 Prog.Part.Nucl.Phys. 58, 587 (2007) The Skyrme interaction in finite nuclei and nuclear matter
doi: 10.1016/j.ppnp.2006.07.001
2007ST20 Phys.Rev. C 76, 025502 (2007) J.R.Stone, G.Goldring, N.J.Stone, N.Severijns, M.Hass, D.Zakoucky, T.Giles, U.Koster, I.S.Kraev, S.Lakshmi, M.Lindroos, F.Wauters Confirmation of parity violation in the γ decay of 180Hfm RADIOACTIVITY 180Hf(IT); measured Eγ, Iγ, angular distributions and mixing ratio. Deduced presence of irregular E2 admixture in the isomeric transition.
doi: 10.1103/PhysRevC.76.025502
2007ST23 Nucl.Phys. A793, 1 (2007) N.J.Stone, J.R.Stone, M.Lindroos, P.Richards, M.Veskovic, D.A.Williams On the absence of appreciable half-life changes in alpha emitters cooled in metals to 1 Kelvin and below RADIOACTIVITY 224,225Ra, 227Ac(α); analyzed T1/2 for source in metallic environment; deduced no temperature dependence.
doi: 10.1016/j.nuclphysa.2007.06.003
2006DO15 Phys.Lett. B 638, 455 (2006) C.Downum, T.Barnes, J.R.Stone, E.S.Swanson Nucleon-meson coupling constants and form factors in the quark model
doi: 10.1016/j.physletb.2006.05.084
2005BR12 Phys.Rev. C 71, 044317 (2005); Erratum Phys.Rev. C 72, 029901 (2005) B.A.Brown, N.J.Stone, J.R.Stone, I.S.Towner, M.Hjorth-Jensen Magnetic moments of the 2+1 states around 132Sn NUCLEAR STRUCTURE 130Sn, 132Sb, 132,134Te; calculated levels, J, π. 124,126,128,130,134Sn, 130,132,134,136Te, 134,136,138Xe, 138Ba; calculated g factors, μ. Shell model, comparisons with data.
doi: 10.1103/PhysRevC.71.044317
2005DA42 Nucl.Instrum.Methods Phys.Res. B241, 971 (2005) M.Danchev, J.Pavan, N.J.Stone, A.E.Stuchbery, C.Baktash, J.Beene, N.Benczer-Koller, C.R.Bingham, J.Dupak, A.Galindo-Uribarri, C.J.Gross, G.Kumbartzki, D.C.Radford, J.R.Stone, C.L.Timlin, C.-H.Yu, N.V.Zamfir g-Factor measurements of first 2+ states of heavy Te isotopes based on nuclear spin deorientation for nuclei recoiling in vacuum NUCLEAR REACTIONS 12C(132Te, 132Te'), (130Te, 130Te'), (126Te, 126Te'), (122Te, 122Te'), E=3 MeV/nucleon; measured Eγ, Iγ(θ), (particle)γ-coin following projectile Coulomb excitation. 132Te level deduced g-factor. Recoil-in-vacuum technique.
doi: 10.1016/j.nimb.2005.07.156
2005ST18 Phys.Rev.Lett. 94, 192501 (2005) N.J.Stone, A.E.Stuchbery, M.Danchev, J.Pavan, C.L.Timlin, C.Baktash, C.Barton, J.Beene, N.Benczer-Koller, C.R.Bingham, J.Dupak, A.Galindo-Uribarri, C.J.Gross, G.Kumbartzki, D.C.Radford, J.R.Stone, N.V.Zamfir First Nuclear Moment Measurement with Radioactive Beams by the Recoil-in-Vacuum Technique: The g Factor of the 2+1 State in 132Te NUCLEAR REACTIONS C(132Te, 132Te'), (122Te, 122Te'), (126Te, 126Te'), (130Te, 130Te'), E=3 MeV/nucleon; measured Eγ, Iγ(θ, φ), (particle)γ-coin following projectile Coulomb excitation; deduced parameters. 132Te level deduced g factor. Clarion, Hyball arrays, recoil-in-vacuum technique.
doi: 10.1103/PhysRevLett.94.192501
2005ST33 Eur.Phys.J. A 25, Supplement 1, 205 (2005) N.J.Stone, A.E.Stuchbery, M.Danchev, J.Pavan, C.L.Timlin, C.Baktash, C.Barton, J.R.Beene, N.Benczer-Koller, C.R.Bingham, J.Dupak, A.Galindo-Uribarri, C.J.Gross, G.Kumbartzki, D.C.Radford, J.R.Stone, N.V.Zamfir First nuclear moment measurement with radioactive beams by recoil-in-vacuum method: g-factor of the 2+1 state in 132Te NUCLEAR REACTIONS C(132Te, 132Te'), (122Te, 122Te'), (126Te, 126Te'), (130Te, 130Te'), E=3 MeV/nucleon; measured Eγ, Iγ(θ, φ), (particle)γ-coin following projectile Coulomb excitation; deduced parameters. 132Te level deduced g factor. Clarion, Hyball arrays, recoil-in-vacuum technique.
doi: 10.1140/epjad/i2005-06-123-0
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