NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = P.D.Stevenson Found 56 matches. 2023MO04 Phys.Lett. B 838, 137675 (2023) L.Morrison, K.Hadynska-Klek, Zs.Podolyak, L.P.Gaffney, M.Zielinska, B.A.Brown, H.Grawe, P.D.Stevenson, T.Berry, A.Boukhari, M.Brunet, R.Canavan, R.Catherall, J.Cederkall, S.J.Colosimo, J.G.Cubiss, H.De Witte, D.T.Doherty, Ch.Fransen, G.Georgiev, E.Giannopoulos, M.Gorska, H.Hess, L.Kaya, T.Kroll, N.Lalovic, B.Marsh, Y.Martinez Palenzuela, G.O'Neill, J.Pakarinen, J.P.Ramos, P.Reiter, J.A.Rodriguez, D.Rosiak, S.Rothe, M.Rudigier, M.Siciliano, E.C.Simpson, J.Snall, P.Spagnoletti, S.Thiel, N.Warr, F.Wenander, R.Zidarova Quadrupole and octupole collectivity in the semi-magic nucleus 20680Hg126 NUCLEAR REACTIONS 94Mo, 104Pd(206Hg, 206Hg'), E=4.195 MeV/nucleon; measured reaction products, Eγ, Iγ. 206Hg; deduced γ-ray energies, B(E2), B(E3). Comparison with shell model predictions, systematics. The HIE-ISOLDE facility at CERN.
doi: 10.1016/j.physletb.2023.137675
2023SH07 Chin.Phys.C 47, 034105 (2023) Isoscalar monopole strength in 100Mo: an indicator for static triaxial deformation in the ground state NUCLEAR STRUCTURE 100Mo; calculated the isoscalar monopole (ISM) mode, static potential-energy-surface (PES) using deformation constraint symmetry-unrestricted three-dimensional time-dependent density functional theory (TDDFT).
doi: 10.1088/1674-1137/acac6b
2021BH10 J.Phys.(London) G48, 075105 (2021) M.Bhuyan, B.Maheshwari, H.A.Kassim, N.Yusof, S.K.Patra, B.V.Carlson, P.D.Stevenson The kinks in charge radii across N = 82 and 126 revisited NUCLEAR STRUCTURE 126,128,130,132,134,136,138Sn, 202,204,206,208,210,212,214Pb; analyzed available data; deduced isotopic shift over the isotopic chains, energy levels, J, π, yrast states within the relativistic mean-field (RMF) and relativistic-Hartree-Bogoliubov (RHB) approach.
doi: 10.1088/1361-6471/abf7d7
2021QI05 Phys.Rev. C 103, L031304 (2021) Y.Qiang, J.C.Pei, P.D.Stevenson Fission dynamics of compound nuclei: Pairing versus fluctuations NUCLEAR REACTIONS 239Pu(n, F)240Pu*, E*=10.6, 16.1, 53.2 MeV; calculated detailed fission observables of compound 240Pu with TD-BCS plus thermal fluctuations: fission evolution time, mass of heavy fragments, proton and neutron numbers of heavy and light fragments, excitation energies of heavy and light fragments, total excitation energies of fragments, total kinetic energies TKE, the quadrupole and octupole deformations before scission, neutron and proton pairing energies. Time-dependent Hartree-Fock+BCS approach.
doi: 10.1103/PhysRevC.103.L031304
2021WA31 Phys.Rev. C 103, 064305 (2021) Configuration mixing and K-forbidden E2 decays NUCLEAR STRUCTURE 171mTm, 175mLu, 171m,175mHf, 173m,175m,177m,179m,181m,185mTa, 179m,181m,183mW, 191mRe, 181mOs; analyzed reduced Weisskopf hindrance factors and two-level mixing strengths for K-forbidden E2 transitions from three-quasiparticle isomers; deduced significant configuration dependence.
doi: 10.1103/PhysRevC.103.064305
2019WE15 Acta Phys.Pol. B50, 567 (2019) K.Wen, M.C.Barton, A.Rios, P.D.Stevenson Dissipation Dynamics of Nuclear Fusion Reactions NUCLEAR REACTIONS 16O(16O, X)32S, E=40 MeV; collective potential, calculated friction coefficient and intrinsic excitation energy using time-dependent density matrix (TDDM) and time-dependent Hartree-Fock (TDHF) models.
doi: 10.5506/aphyspolb.50.567
2018WE06 Phys.Rev. C 98, 014603 (2018) K.Wen, M.C.Barton, A.Rios, P.D.Stevenson Two-body dissipation effect in nuclear fusion reactions NUCLEAR REACTIONS 16O(16O, X)32S*, E(cm)=20, 40 MeV; calculated total energy of the fusion system, collective potential, friction coefficient, and intrinsic excitation energy using time-dependent density matrix (TDDM) and time-dependent Hartree-Fock (TDHF) models. Dissipative dynamics.
doi: 10.1103/PhysRevC.98.014603
2016GR15 Phys.Rev. C 94, 044327 (2016) T.Grahn, S.Stolze, D.T.Joss, R.D.Page, B.Saygi, D.O'Donnell, M.Akmali, K.Andgren, L.Bianco, D.M.Cullen, A.Dewald, P.T.Greenlees, K.Heyde, H.Iwasaki, U.Jakobsson, P.Jones, D.S.Judson, R.Julin, S.Juutinen, S.Ketelhut, M.Leino, N.Lumley, P.J.R.Mason, O.Moller, K.Nomura, M.Nyman, A.Petts, P.Peura, N.Pietralla, Th.Pissulla, P.Rahkila, P.J.Sapple, J.Saren, C.Scholey, J.Simpson, J.Sorri, P.D.Stevenson, J.Uusitalo, H.V.Watkins, J.L.Wood Excited states and reduced transition probabilities in 168Os NUCLEAR REACTIONS 92Mo(78Kr, 2p), E=335, 345, 348 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin, level half-lives by recoil-distance method using a plunger device, RITU separator, GREAT spectrometer, JUROGAM array at Jyvaskyla accelerator facility. 168Os; deduced high-spin levels, J, π, bands, B(E2), B(E1), transition quadrupole and dipole moments. Comparisons with interacting boson model (IBM-2) calculations based on the SkM* energy-density functional. Systematics of ground bands, and excited positive-parity level energies up to 8+ in 168,170,172,174,176,178,180,182,184Os.
doi: 10.1103/PhysRevC.94.044327
2016RE07 Phys.Rev. C 93, 044618 (2016) P.-G.Reinhard, A.S.Umar, P.D.Stevenson, J.Piekarewicz, V.E.Oberacker, J.A.Maruhn Sensitivity of the fusion cross section to the density dependence of the symmetry energy NUCLEAR REACTIONS 48Ca(48Ca, X)96Zr*, E(cm)=45-65 MeV; calculated folding model ion-ion interaction potentials, fusion σ(E). Impact of nuclear fusion on the nuclear equation of state (EOS). 48Ca; calculated Neutron root-mean-square radius (rms), neutron diffraction radius, and neutron halo. Dynamic microscopic method based on density-constrained time-dependent Hartree-Fock (DC-TDHF) approach, and direct TDHF study of barrier cross sections using a family of Skyrme parametrization.
doi: 10.1103/PhysRevC.93.044618
2016ST13 Phys.Rev. C 93, 054617 (2016) P.D.Stevenson, E.B.Suckling, S.Fracasso, M.C.Barton, A.S.Umar Skyrme tensor force in heavy ion collisions NUCLEAR REACTIONS 16O(16O, X), E(cm)=100 MeV; calculated contributions from terms involving time-odd densities and currents to the total energy as the sum of isoscalar and isovector contributions, energy contributions from (pseudo)scalar-, vector- and (pseudo)tensor-decomposed form of spin-current tensor J. Symmetry-unrestricted Time-dependent Hartree-Fock (TDHF) energy density functional calculations with full version of Skyrme force, including terms arising only from the Skyrme tensor force. Discussed role of Skyrme tensor force in dynamic processes in nuclei.
doi: 10.1103/PhysRevC.93.054617
2013GO01 Phys.Rev.Lett. 110, 032503 (2013) P.M.Goddard, P.D.Stevenson, A.Rios Charge Radius Isotope Shift Across the N=126 Shell Gap NUCLEAR STRUCTURE 210Po, 208,210Pb; calculated neutron single particle energies, isotope shifts in mean square charge radius, proton orbitals. NRAPRii parameterization, comparison with available data.
doi: 10.1103/PhysRevLett.110.032503
2013GO19 Phys.Rev. C 88, 064308 (2013) P.M.Goddard, N.Cooper, V.Werner, G.Rusev, P.D.Stevenson, A.Rios, C.Bernards, A.Chakraborty, B.P.Crider, J.Glorius, R.S.Ilieva, J.H.Kelley, E.Kwan, E.E.Peters, N.Pietralla, R.Raut, C.Romig, D.Savran, L.Schnorrenberger, M.K.Smith, K.Sonnabend, A.P.Tonchev, W.Tornow, S.W.Yates Dipole response of 76Se above 4 MeV NUCLEAR REACTIONS 76Se(polarized γ, γ'), E=4-9 MeV; measured Eγ, Iγ, γ(θ), integrated σ, γ(linear polarization) at HIγS facility at TUNL. 76Se; deduced levels, J, π, Γ, level half-lives, B(E1), B(M1), branching ratios. Comparison with theoretical calculations.
doi: 10.1103/PhysRevC.88.064308
2013MA66 Phys.Rev. C 88, 044301 (2013) P.J.R.Mason, Zs.Podolyak, N.Marginean, P.H.Regan, P.D.Stevenson, V.Werner, T.Alexander, A.Algora, T.Alharbi, M.Bowry, R.Britton, A.M.Bruce, D.Bucurescu, M.Bunce, G.Cata-Danil, I.Cata-Danil, N.Cooper, D.Deleanu, D.Delion, D.Filipescu, W.Gelletly, D.Ghita, I.Gheorghe, T.Glodariu, G.Ilie, D.Ivanova, S.Kisyov, S.Lalkovski, R.Lica, S.N.Liddick, R.Marginean, C.Mihai, K.Mulholland, C.R.Nita, A.Negret, S.Pascu, S.Rice, O.J.Roberts, T.Sava, J.F.Smith, P.-A.Soderstrom, L.Stroe, G.Suliman, R.Suvaila, S.Toma, C.Townsley, E.Wilson, R.T.Wood, M.Zhekova, C.Zhou Half-life of the yrast 2+ state in 188W: Evolution of deformation and collectivity in neutron-rich tungsten isotopes NUCLEAR REACTIONS 186W(7Li, pα), E=35 MeV; measured Eγ, γγ-coin, T1/2 of first 2+ state by γγ(t) at IFIN-HH, Bucharest facility. 188W; deduced level, B(E2) for first 2+ state, enhanced γ softness in 188W. Systematics of energies of low-lying 0+, 2+ and 4+ states and B(E2) values for first 2+ states in even-even Hf, W, Os and Pt nuclei with N=102-120. NUCLEAR STRUCTURE 184,186,188,190,192,194W; calculated Woods-Saxon potential energy surface (PES) contours in (β, γ) plane; deduced prolate to oblate shape transition.
doi: 10.1103/PhysRevC.88.044301
2013MA74 Phys.Rev. C 88, 044301 (2013) P.J.R.Mason, Zs.Podolyak, N.Marginean, P.H.Regan, P.D.Stevenson, V.Werner, T.Alexander, A.Algora, T.Alharbi, M.Bowry, R.Britton, A.M.Bruce, D.Bucurescu, M.Bunce, G.Cata-Danil, I.Cata-Danil, N.Cooper, D.Deleanu, D.Delion, D.Filipescu, W.Gelletly, D.Ghita, I.Gheorghe, T.Glodariu, G.Ilie, D.Ivanova, S.Kisyov, S.Lalkovski, R.Lica, S.N.Liddick, R.Marginean, C.Mihai, K.Mulholland, C.R.Nita, A.Negret, S.Pascu, S.Rice, O.J.Roberts, T.Sava, J.F.Smith, P.-A.Soderstrom, L.Stroe, G.Suliman, R.Suvaila, S.Toma, C.Townsley, E.Wilson, R.T.Wood, M.Zhekova, C.Zhou Half-life of the yrast 2+ state in 188W: Evolution of deformation and collectivity in neutron-rich tungsten isotopes
doi: 10.1103/PhysRevC.88.044301
2013PA02 Phys.Rev. C 87, 014330 (2013) Continuum time-dependent Hartree-Fock method for giant resonances in spherical nuclei NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated time evolution of monopole (E0) moment for nuclear giant monopole resonances in the small and large amplitude regimes. Spherically symmetric time-dependent Hartree-Fock approximation discretized using a Crank-Nicholson scheme.
doi: 10.1103/PhysRevC.87.014330
2012AL05 Phys.Rev. C 85, 034301 (2012); Pub.Note Phys.Rev. C 85, 039904 (2012) N.Al-Dahan, P.H.Regan, Zs.Podolyak, P.M.Walker, N.Alkhomashi, G.D.Dracoulis, G.Farrelly, J.Benlliure, S.B.Pietri, R.F.Casten, P.D.Stevenson, W.Gelletly, S.J.Steer, A.B.Garnsworthy, E.Casarejos, J.Gerl, H.J.Wollersheim, J.Grebosz, M.Gorska, I.Kojouharov, H.Schaffner, A.Algora, G.Benzoni, A.Blazhev, P.Boutachkov, A.M.Bruce, I.J.Cullen, A.M.D.Bacelar, A.Y.Deo, M.E.Estevez, Y.Fujita, R.Hoischen, R.Kumar, S.Lalkovski, Z.Liu, P.J.Mason, C.Mihai, F.Molina, D.Mucher, B.Rubio, A.Tamii, S.Tashenov, J.J.Valiente-Dobon, P.J.Woods Multiple Β- decaying states in 194Re: Shape evolution in neutron-rich osmium isotopes NUCLEAR REACTIONS 9Be(208Pb, X)186Hf/187Hf/188Hf/189Hf/188Ta/189Ta/190Ta/191Ta/190W/191W/192W/193W/192Re/193Re/194Re/195Re/196Re/195Os/196Os/197Os/198Os, E=1 GeV/nucleon; measured fragment yields, ion identification by energy loss and time-of-flight methods; deduced decay properties. GSI FRagment Separator (FRS), RISING spectrometer. RADIOACTIVITY 192,194Re[from 9Be(208Pb, X), E=1 GeV/nucleon](β-); 194Os[from 194Re decay](α); measured Eγ, Iγ, βγ-, (implants)γ-coin, recoil-decay tagging method, half-life. 194Os; deduced levels, J, π. 187Hf, 188,189,190Ta, 190,191W, 192,193Re(IT); measured Eγ, Iγ, half-lives. GSI FRagment Separator (FRS), RISING spectrometer. Systematics of low-lying 0+, 2+, 4+ and 6+ states in N=110-122 Os and W nuclei. NUCLEAR STRUCTURE 194Re; calculated levels, J, π, configurations using Nilsson multi-quasiparticle (MQP) model.
doi: 10.1103/PhysRevC.85.034301
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
2012FR06 Phys.Rev. C 86, 044303 (2012) S.Fracasso, E.B.Suckling, P.D.Stevenson Unrestricted Skyrme-tensor time-dependent Hartree-Fock model and its application to the nuclear response from spherical to triaxial nuclei NUCLEAR STRUCTURE 16O, 24Mg, 28Si, 120Sn, 178Os, 190W, 238U; calculated transition strength distributions of isovector giant dipole resonances using the Skyrme energy density functional (EDF) in the three dimensional time-dependent Hartree-Fock. Comparison with predictions from the (quasi)-particle random-phase approximation and experimental data.
doi: 10.1103/PhysRevC.86.044303
2012LO10 Phys.Rev. C 86, 024608 (2012) N.Loebl, A.S.Umar, J.A.Maruhn, P.-G.Reinhard, P.D.Stevenson, V.E.Oberacker Single-particle dissipation in a time-dependent Hartree-Fock approach studied from a phase-space perspective NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=160, 200, 240 MeV; calculated β and γ deformation parameter, quadrupole moment, and volume phase-space global observables in momentum and coordinate space using the time-dependent Hartree-Fock (TDHF) theory and the Wigner distribution function in the full six-dimensional phase space. Significance of extra time-odd terms.
doi: 10.1103/PhysRevC.86.024608
2012ST23 J.Phys.:Conf.Ser. 381, 012105 (2012) P.D.Stevenson, S.Fracasso, E.B.Suckling The tensor-kinetic field in nuclear collisions
doi: 10.1088/1742-6596/381/1/012105
2011AV01 J.Phys.(London) G38, 025104 (2011) M.Avgoulea, Yu.P.Gangrsky, K.P.Marinova, S.G.Zemlyanoi, S.Fritzsche, D.Iablonskyi, C.Barbieri, E.C.Simpson, P.D.Stevenson, J.Billowes, P.Campbell, B.Cheal, B.Tordoff, M.L.Bissell, D.H.Forest, M.D.Gardner, G.Tungate, J.Huikari, A.Nieminen, H.Penttila, J.Aysto Nuclear charge radii and electromagnetic moments of radioactive scandium isotopes and isomers NUCLEAR MOMENTS 42,43,44,45,46Sc; measured hyperfine structure; deduced nuclear magnetic dipole moments and electric quadrupole moments, isotope shifts, charge radii, deformation. Shell model calculation, laser spectroscopy. NUCLEAR STRUCTURE 42,43,44,45,46Sc, 40,41,42,43,44,45,46,47,48Ca; calculated nuclear isomer shifts, radii, magnetic moment, spectroscopic quadrupole moments. Comparison with other data.
doi: 10.1088/0954-3899/38/2/025104
2011NO05 Phys.Rev. C 83, 054303 (2011) K.Nomura, T.Otsuka, R.Rodriguez-Guzman, L.M.Robledo, P.Sarriguren, P.H.Regan, P.D.Stevenson, Zs.Podolyak Spectroscopic calculations of the low-lying structure in exotic Os and W isotopes NUCLEAR STRUCTURE 186,188,190,192,194,196,198Os, 184,186,188,190,192,194,196W; calculated levels, J, π, B(E2), potential energy surfaces, g.s. and quasi γ bands. Interacting boson model (IBM) Hamiltonian determined by (constrained) Hartree-Fock-Bogoliubov calculations with the Gogny-D1S energy density functional (EDF). Comparison with experimental data.
doi: 10.1103/PhysRevC.83.054303
2010BI03 Phys.Lett. B 690, 15 (2010) L.Bianco, R.D.Page, I.G.Darby, D.T.Joss, J.Simpson, J.S.Al-Khalili, A.J.Cannon, B.Cederwall, S.Eeckhaudt, S.Erturk, B.Gall, M.B.Gomez Hornillos, T.Grahn, P.T.Greenlees, B.Hadinia, K.Heyde, U.Jakobsson, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Labiche, M.Leino, A.-P.Leppanen, M.Nyman, D.O'Donnell, E.S.Paul, M.Petri, P.Peura, A.Puurunen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, P.J.Sapple, J.Saren, C.Scholey, N.A.Smirnova, A.N.Steer, P.D.Stevenson, E.B.Suckling, J.Thomson, J.Uusitalo, M.Venhart Discovery of 157W and 161Os NUCLEAR REACTIONS 106Cd(58Ni, 3n), E=290, 310 MeV; measured reaction products; deduced α spectra, α-branching, T1/2, fine structure, ground state J, π. RADIOACTIVITY 161Os(α), 157W(β+); measured decay products; deduced T1/2, β-branching. Comparison with shell model calculations.
doi: 10.1016/j.physletb.2010.04.056
2010CE01 J.Phys.(London) G37, 075107 (2010) M.Centelles, S.K.Patra, X.Roca-Maza, B.K.Sharma, P.D.Stevenson, X.Vinas The influence of the symmetry energy on the giant monopole resonance of neutron-rich nuclei analyzed in Thomas-Fermi theory NUCLEAR STRUCTURE 90Zr, 208,266Pb; calculated neutron skin thickness, energy per particle, giant monopole resonance. Relativistic extended Thomas-Fermi method.
doi: 10.1088/0954-3899/37/7/075107
2010ST16 J.Phys.:Conf.Ser. 205, 012027 (2010) P.D.Stevenson, J.M.A.Broomfield Testing a variational method for fluctuations
doi: 10.1088/1742-6596/205/1/012027
2010SU09 Europhys.Lett. 90, 12001 (2010) The effect of the tensor force on the predicted stability of superheavy nuclei NUCLEAR STRUCTURE 298Fl, 310126; calculated single-particle energies, proton shell structures, two-proton shell gap. Tensor component of the Skyrme nucleon-nucleon interaction.
doi: 10.1209/0295-5075/90/12001
2010WA08 Phys.Rev. C 81, 041304 (2010) P.M.Walker, S.Lalkovski, P.D.Stevenson Configuration dependence of K-forbidden transition rates from three-quasiparticle isomers NUCLEAR STRUCTURE 171Tm, 171,172,174,175,176,177,178Hf, 174Yb, 175Lu, 175,177,179,181,185Ta, 178,179,181,182,183W, 181,183Re, 181,184,191Os; analyzed reduced hindrance factors for K-forbidden E2 transitions from two- and three-quasiparticle isomers, NpNn correlations.
doi: 10.1103/PhysRevC.81.041304
2008BR13 J.Phys.(London) G35, 095102 (2008) J.M.A.Broomfield, P.D.Stevenson Mass dispersions from giant dipole resonances using the Balian-Veneroni variational approach NUCLEAR STRUCTURE 32S, 132Sn; calculated mass dispersions in giant dipole resonances; three dimensional TDHF method with Skyrme interaction.
doi: 10.1088/0954-3899/35/9/095102
2008GU11 J.Phys.(London) G35, 075106 (2008) R.K.Gupta, S.K.Patra, P.D.Stevenson, C.Beck, W.Greiner Fission of hyper-hyperdeformed 56Ni: a clustering analysis within mean-field approaches NUCLEAR STRUCTURE 56Ni; calculated binding energy, radii, matter density distributions; deduced alpha-clustering effect. Compared two models.
doi: 10.1088/0954-3899/35/7/075106
2008RE14 Int.J.Mod.Phys. E17, Supplement 1, 8 (2008) P.H.Regan, N.Alkhomashi, N.Al-Dahan, Zs.Podolyak, S.B.Pietri, S.J.Steer, A.B.Garnsworthy, E.B.Suckling, P.D.Stevenson, G.Farrelly, I.J.Cullen, W.Gelletly, P.M.Walker, J.Benlliure, A.I.Morales, E.Casajeros, M.E.Estevez, J.Gerl, M.Gorska, H.J.Wollersheim, P.Boutachkov, S.Tashenov, I.Kojouharov, H.Schaffner, N.Kurz, R.Kumar, B.Rubio, A.Algora, F.Molina, J.Grebosz, G.Benzoni, D.Mucher, A.M.Bruce, A.M.D.Bacelar, S.Lalkovski, Y.Fujita, A.Tamii, R.Hoischen, Z.Liu, P.J.Woods, C.Mihai, J.J.Valiente-Dobon First results with the rising active stopper
doi: 10.1142/S0218301308011719
2007GU20 Int.J.Mod.Phys. E16, 1721 (2007) R.K.Gupta, S.K.Patra, P.D.Stevenson, W.Greiner A highly neutron-rich cluster and/or a superheavy nucleus in the compound nucleus 238U+238U: A Mean field study NUCLEAR REACTIONS 238U(238U, X), E not given; calculated neutron and proton matter density distributions, resonance state properties, clustering structures in the superheavy nucleus using a relativistic mean field and non-relativistic Hartree-Fock approach.
doi: 10.1142/S0218301307006137
2007JO13 Phys.Rev. C 76, 047303 (2007) G.A.Jones, P.H.Regan, P.M.Walker, Zs.Podolyak, P.D.Stevenson, M.P.Carpenter, J.J.Carroll, R.S.Chakrawarthy, P.Chowdhury, A.B.Garnsworthy, R.V.F.Janssens, T.L.Khoo, F.G.Kondev, G.J.Lane, Z.Liu, D.Seweryniak, N.J.Thompson, S.Zhu, S.J.Williams Identification of a high-spin isomer in 99Mo NUCLEAR REACTIONS 27Al(178Hf, X), E=1150 MeV; measured Eγ, Iγ, γγ-coin. 99Mo deduced levels, J, π, half-life, isomer, band structure.
doi: 10.1103/PhysRevC.76.047303
2007PA27 Phys.Rev. C 75, 061302 (2007) R.D.Page, L.Bianco, I.G.Darby, J.Uusitalo, D.T.Joss, T.Grahn, R.-D.Herzberg, J.Pakarinen, J.Thomson, S.Eeckhaudt, P.T.Greenlees, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Leino, A.-P.Leppanen, M.Nyman, P.Rahkila, J.Saren, C.Scholey, A.Steer, M.B.Gomez Hornillos, J.S.Al-Khalili, A.J.Cannon, P.D.Stevenson, S.Erturk, B.Gall, B.Hadinia, M.Venhart, J.Simpson α decay of 159Re and proton emission from 155Ta RADIOACTIVITY 159Re(α) [from 106Cd(58Ni, X)]; 155Ta(p); measured Eα, Iα, Ep, Ip. deduced separation energies.
doi: 10.1103/PhysRevC.75.061302
2007PA30 J.Phys.(London) G34, 2073 (2007) S.K.Patra, R.K.Gupta, B.K.Sharma, P.D.Stevenson, W.Greiner Exotic clustering in heavy and superheavy nuclei within the relativistic and non-relativistic mean field formalisms NUCLEAR STRUCTURE 222Ra, 232U, 236Pu, 242Cm; Z=114; calculated binding energies, deformation parameters, and rms charge radii within the relativistic mean field approach and the non-relativistic Skyrme-Hartree-Fock formalism.
doi: 10.1088/0954-3899/34/9/016
2007ST27 Nucl.Phys. A788, 343c (2007) P.D.Stevenson, D.Almehed, P.-G.Reinhard, J.A.Maruhn Monopole Giant Resonances and TDHF boundary conditions
doi: 10.1016/j.nuclphysa.2007.01.091
2006BR26 Int.J.Mod.Phys. E15, 1417 (2006) M.P.Brine, P.D.Stevenson, J.A.Maruhn, P.-G.Reinhard Dipole response in neutron-rich magnesium NUCLEAR STRUCTURE 34Mg; calculated isovector dipole response.
doi: 10.1142/S0218301306005009
2006JO10 Phys.Lett. B 641, 34 (2006) D.T.Joss, I.G.Darby, R.D.Page, J.Uusitalo, S.Eeckhaudt, T.Grahn, P.T.Greenlees, P.M.Jones, R.Julin, S.Juutinen, S.Ketelhut, M.Leino, A.-P.Leppanen, M.Nyman, J.Pakarinen, P.Rahkila, J.Saren, C.Scholey, A.Steer, A.J.Cannon, P.D.Stevenson, J.S.Al-Khalili, S.Erturk, M.Venhart, B.Gall, B.Hadinia, J.Simpson Probing the limit of nuclear existence: Proton emission from 159Re NUCLEAR REACTIONS 106Cd(58Ni, 4np), E=300 MeV; measured Eα, Iα, Ep, Ip, (recoil)α-coin following residual nucleus decay. Recoil-decay correlation technique. RADIOACTIVITY 159Re(p) [from 106Cd(58Ni, 4np)]; measured Ep, T1/2; deduced ground-state configuration.
doi: 10.1016/j.physletb.2006.08.014
2006MA54 Phys.Rev. C 74, 027601 (2006) J.A.Maruhn, P.-G.Reinhard, P.D.Stevenson, M.R.Strayer Spin-excitation mechanisms in Skyrme-force time-dependent Hartree-Fock calculations NUCLEAR REACTIONS 16O(16O, X), E(cm)=75-150 MeV; calculated energy loss, spin excitations, role of odd-odd couplings. Skyrme-force time-dependent Hartree-Fock calculations.
doi: 10.1103/PhysRevC.74.027601
2006OR10 Phys.Rev. C 74, 034318 (2006) J.N.Orce, A.M.Bruce, A.Emmanouilidis, A.P.Byrne, G.D.Dracoulis, T.Kibedi, M.Caamano, H.El-Masri, C.J.Pearson, Zs.Podolyak, P.D.Stevenson, P.M.Walker, F.R.Xu, D.M.Cullen, C.Wheldon Shape-driving effects in the triaxial nucleus, 128Xe NUCLEAR REACTIONS 124Sn(9Be, 5n), E=58 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 128Xe deduced high-spin levels, J, π, configurations, isomer T1/2, shape-driving effects. Caesar array. Potential energy surface calculations, configuration-constrained blocking method.
doi: 10.1103/PhysRevC.74.034318
2006PE01 Nucl.Phys. A765, 29 (2006) J.C.Pei, F.R.Xu, P.D.Stevenson Deformation effects on the structures of N = 7 halo nuclei NUCLEAR STRUCTURE 9He, 11Be, 13C, 15O; calculated particle density distributions, binding energies, radii. Skyrme-Hartree-Fock model.
doi: 10.1016/j.nuclphysa.2005.10.004
2006SH01 J.Phys.(London) G32, L1 (2006) B.K.Sharma, P.Arumugam, S.K.Patra, P.D.Stevenson, R.K.Gupta, W.Greiner Clustering in superheavy nuclei within the relativistic mean field approach NUCLEAR STRUCTURE 292,296,300,304120; calculated binding energies, deformation parameters, radii, matter density distributions; deduced cluster configurations. Relativistic mean field approach.
doi: 10.1088/0954-3899/32/1/L01
2006SH20 J.Phys.(London) G32, 2089 (2006) B.K.Sharma, S.K.Patra, R.K.Gupta, A.Shukla, P.Arumugam, P.D.Stevenson, W.Greiner Reaction cross-sections for light nuclei on 12C using relativistic mean field formalism NUCLEAR REACTIONS 12C(8B, X), (9B, X), (10B, X), (11B, X), (12B, X), (13B, X), (14B, X), (15B, X), (16B, X), (17B, X), (18B, X), (19B, X), (7Be, X), (8Be, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (13Be, X), (14Be, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (10Li, X), (11Li, X), E ≈ 800 MeV/nucleon; calculated reaction σ. Relativistic mean field approach. NUCLEAR STRUCTURE 6,7,8,9,10,11Li, 10,11,12,13,14Be, 15,16,17B; calculated binding energies, deformation. Relativistic mean field approach.
doi: 10.1088/0954-3899/32/11/004
2005AL41 J.Phys.(London) G31, S1819 (2005) Isovector giant monopole resonances in spherical nuclei NUCLEAR STRUCTURE 90Zr, 100,120,132Sn, 140Ce, 208Pb; calculated isovector giant monopole resonance energies, energy-dependent mixing with isoscalar resonance. Time-dependent Hartree-Fock method, Skyrme forces.
doi: 10.1088/0954-3899/31/10/079
2005CA02 Eur.Phys.J. A 23, 201 (2005) M.Caamano, P.M.Walker, P.H.Regan, M.Pfutzner, Zs.Podolyak, J.Gerl, M.Hellstrom, P.Mayet, M.N.Mineva, A.Aprahamian, J.Benlliure, A.M.Bruce, P.A.Butler, D.Cortina Gil, D.M.Cullen, J.Doring, T.Enqvist, C.Fox, J.Garces Narro, H.Geissel, W.Gelletly, J.Giovinazzo, M.Gorska, H.Grawe, R.Grzywacz, A.Kleinbohl, W.Korten, M.Lewitowicz, R.Lucas, H.Mach, C.D.O'Leary, F.De Oliveira, C.J.Pearson, F.Rejmund, M.Rejmund, M.Sawicka, H.Schaffner, C.Schlegel, K.Schmidt, K.-H.Schmidt, P.D.Stevenson, Ch.Theisen, F.Vives, D.D.Warner, C.Wheldon, H.J.Wollersheim, S.Wooding, F.Xu, O.Yordanov Isomers in neutron-rich A ≈ 190 nuclides from 208Pb fragmentation NUCLEAR REACTIONS Be(208Pb, X), E=1 GeV/nucleon; measured fragments isotopic yields, delayed Eγ, γγ-, (particle)γ-coin; deduced isomer production ratios. RADIOACTIVITY 188Ta, 190W, 192,193Re, 195Os, 197,198Ir, 200,201,202Pt, 203Au(IT) [from Be(208Pb, X)]; measured Eγ, Iγ, γγ-coin, T1/2. 188Ta, 190W, 192,193Re, 195Os, 197,198Ir, 200,201,202Pt, 203Au deduced transitions. 190W, 200,201,202Pt deduced levels, J, π. 174,175Er, 185Hf, 191,194Re, 199Ir(IT) [from Be(208Pb, X)]; measured Eγ, Iγ.
doi: 10.1140/epja/i2004-10079-7
2005MA41 Phys.Rev. C 71, 064328 (2005) J.A.Maruhn, P.G.Reinhard, P.D.Stevenson, J.Rikovska Stone, M.R.Strayer Dipole giant resonances in deformed heavy nuclei NUCLEAR STRUCTURE 132Sn, 142,144,146,148,150Nd, 152Dy, 188Os, 238U; calculated dipole strength distributions, resonance features, deformation dependence. Time-dependent Skyrme-Hartree-Fock method.
doi: 10.1103/PhysRevC.71.064328
2005PE04 Phys.Rev. C 71, 034302 (2005) J.C.Pei, F.R.Xu, P.D.Stevenson Density distributions of superheavy nuclei NUCLEAR STRUCTURE 254,256,258Rf, 258,260,266Sg, 264,266,270Hs, 270Ds, 284Cn, 288,298Fl, 292Lv; calculated deformation parameters, radii, Qα. 208Pb, 270,280,290Ds, 286,292,298,304,310Fl, 292120; calculated particle density distributions. Skyrme-Hartree-Fock model.
doi: 10.1103/PhysRevC.71.034302
2005ST32 Phys.Rev. C 72, 047303 (2005) P.D.Stevenson, M.P.Brine, Zs.Podolyak, P.H.Regan, P.M.Walker, J.Rikovska Stone Shape evolution in the neutron-rich tungsten region NUCLEAR STRUCTURE 180,182,184,186,188,190,192Yb, 182,184,186,188,190,192,194Hf, 184,186,188,190,192,194,196W, 186,188,190,192,194,196,198Os, 188,190,192,194,196,198,200Pt; calculated potential energy vs deformation, shape coexistence features; deduced role in level energy systematics. Self-consistent Hartree-Fock approach.
doi: 10.1103/PhysRevC.72.047303
2005XU08 J.Phys.(London) G31, S1541 (2005) F.R.Xu, J.C.Pei, P.D.Stevenson Densities of superheavy nuclei at closed shells NUCLEAR STRUCTURE Z=114; Z=120; Z=126; calculated matter density distributions.
doi: 10.1088/0954-3899/31/10/028
2004ST06 Int.J.Mod.Phys. E13, 181 (2004) P.D.Stevenson, M.R.Strayer, J.Rikovska Stone, W.G.Newton Giant resonances from TDHF NUCLEAR STRUCTURE 16O; calculated giant resonance strength functions. TDHF approach.
doi: 10.1142/S0218301304001928
2003OR04 Acta Phys.Pol. B34, 2253 (2003) J.N.Orce, A.M.Bruce, A.Emmanouilidis, C.Wheldon, F.R.Xu, P.M.Walker, M.Caamano, Zs.Podolyak, H.El-Masri, P.D.Stevenson, A.P.Byrne, G.D.Dracoulis, J.C.Hazel, T.Kibedi, D.M.Cullen Interplay between K-isomerism and γ-softness in 128Xe NUCLEAR REACTIONS 124Sn(9Be, 5n), E=58 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 128Xe deduced levels, J, π, configurations, deformation effects. Potential energy surface calculations.
2003RA44 Phys.Rev. C 68, 044315 (2003) A.K.Rath, P.D.Stevenson, P.H.Regan, F.R.Xu, P.M.Walker Self-consistent description of dysprosium isotopes in the doubly midshell region NUCLEAR STRUCTURE 160,162,164,166,168,170,172,174,176,178,180Dy; calculated binding energies, quadrupole deformations. 170Dy; calculated levels, J, π, configurations, rotational band features. Density-dependent Hartree-Fock approach, angular-momentum projection.
doi: 10.1103/PhysRevC.68.044315
2003RI07 Phys.Rev. C 68, 034324 (2003) J.Rikovska Stone, J.C.Miller, R.Koncewicz, P.D.Stevenson, M.R.Strayer Nuclear matter and neutron-star properties calculated with the Skyrme interaction
doi: 10.1103/PhysRevC.68.034324
2002OI03 Prog.Theor.Phys.(Kyoto), Suppl. 146, 609 (2002) M.Oi, P.H.Regan, R.R.Xu, P.M.Walker, A.K.Rath, P.D.Stevenson Cranked-Hartree-Fock-Bogoliubov Analysis at the Valence Maximum: Yrast Behaviour of 17066Dy104 NUCLEAR STRUCTURE 170Dy; calculated deformation vs angular momentum. Cranked-Hartree-Fock-Bogoliubov approach.
doi: 10.1143/PTPS.146.609
2002RE11 Phys.Rev. C65, 037302 (2002) P.H.Regan, F.R.Xu, P.M.Walker, M.Oi, A.K.Rath, P.D.Stevenson Structure of the Doubly Midshell Nucleus 66170Dy104 NUCLEAR STRUCTURE 170Dy; calculated total Routhian surfaces, deformation features, rotational band moment of inertia.
doi: 10.1103/PhysRevC.65.037302
2002SH21 Phys.Rev. C65, 064310 (2002) T.Shizuma, P.D.Stevenson, P.M.Walker, Y.Toh, T.Hayakawa, M.Oshima, K.Furuno, T.Komatsubara High-K Negative Parity States in 184Os NUCLEAR REACTIONS 170Er(18O, 4n), E=85 MeV; measured Eγ, Iγ, γγ-coin. 184Os deduced high-spin levels, J, π, configurations, isomeric state T1/2. Cranked mean-field calculations.
doi: 10.1103/PhysRevC.65.064310
2002ST30 Phys.Lett. 545B, 291 (2002) P.D.Stevenson, J.Rikovska Stone, M.R.Strayer Mean field calculation of Ne, Mg and Si nuclei at N = 20 with the separable monopole interaction NUCLEAR STRUCTURE 28,30,32Ne, 30,32,34Mg, 32,34,36Si; calculated radii, quadrupole deformation parameters, single-particle levels; deduced shell-closure effects. 30,32,34Mg; calculated transitions B(E2). Mean-field approach, comparison with data.
doi: 10.1016/S0370-2693(02)02634-5
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