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NSR database version of April 11, 2024.

Search: Author = J.R.Stone

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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
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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
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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
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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
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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
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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
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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
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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
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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
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2016ST11      Eur.Phys.J. A 52, 66 (2016)

J.R.Stone

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
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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
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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
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2014PA54      Phys.Rev. C 90, 065802 (2014)

H.Pais, W.G.Newton, J.R.Stone

Phase transitions in core-collapse supernova matter at sub-saturation densities

doi: 10.1103/PhysRevC.90.065802
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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
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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
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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
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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
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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
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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
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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
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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
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2009NE06      Phys.Rev. C 79, 055801 (2009)

W.G.Newton, J.R.Stone

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
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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
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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
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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
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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
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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
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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
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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
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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
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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)

J.R.Stone, P.-G.Reinhard

The Skyrme interaction in finite nuclei and nuclear matter

doi: 10.1016/j.ppnp.2006.07.001
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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
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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
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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
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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
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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
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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
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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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