NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Pearson Found 133 matches. Showing 1 to 100. [Next]2023SH20 Phys.Rev. C 108, 025805 (2023) N.N.Shchechilin, N.Chamel, J.M.Pearson Unified equations of state for cold nonaccreting neutron stars with Brussels-Montreal functionals. IV. Role of the symmetry energy in pasta phases
doi: 10.1103/PhysRevC.108.025805
2022PE01 Phys.Rev. C 105, 015803 (2022) Unified equations of state for cold nonaccreting neutron stars with Brussels-Montreal functionals. III. Inclusion of microscopic corrections to pasta phases
doi: 10.1103/PhysRevC.105.015803
2021PE06 Phys.Rev. C 103, 034328 (2021) Reflating the nucleus: The pachydermous droplet model NUCLEAR STRUCTURE A=10-260; calculated rms radii as function of mass number using leptodermous droplet model (LDM) and pachydermous droplet model (PDM); deduced that the tendency of the standard droplet model (DM) to lead to excessive squeezing of nuclei can be rectified by going beyond the leptodermous picture and attributing to the DM a surface skin of finite thickness.
doi: 10.1103/PhysRevC.103.034328
2020PE01 Phys.Rev. C 101, 015802 (2020) J.M.Pearson, N.Chamel, A.Y.Potekhin Unified equations of state for cold nonaccreting neutron stars with Brussels-Montreal functionals. II. Pasta phases in semiclassical approximation
doi: 10.1103/PhysRevC.101.015802
2019MU10 Phys.Rev. C 99, 055805 (2019) Y.D.Mutafchieva, N.Chamel, Zh.K.Stoyanov, J.M.Pearson, L.M.Mihailov Role of Landau-Rabi quantization of electron motion on the crust of magnetars within the nuclear energy density functional theory
doi: 10.1103/PhysRevC.99.055805
2016GO10 Phys.Rev. C 93, 034337 (2016) S.Goriely, N.Chamel, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. XVI. Inclusion of self-energy effects in pairing ATOMIC MASSES N=8-240; calculated masses for 6884 nuclei using new family of three Hartree-Fock-Bogoliubov (HFB) mass models HFB-30, HFB-31, and HFB-32, and respective interactions, BSk30, BSk31, and BSk32, respectively. New feature of a purely phenomenological pairing term that depends on the density gradient. Best fit to the database of 2353 experimental nuclear masses from AME-2012, and to rms charge-radius data. Relevance to neutron superfluidity in the inner crust of neutron stars.
doi: 10.1103/PhysRevC.93.034337
2015AU02 At.Data Nucl.Data Tables 103-104, 1 (2015); See 2014PF01 G.Audi, K.Blaum, M.Block, G.Bollen, S.Goriely, J.C.Hardy, F.Herfurth, F.G.Kondev, H.-J.Kluge, D.Lunney, J.M.Pearson, G.Savard, K.S.Sharma, M.Wang, Y.H.Zhang Comment on "Atomic mass compilation 2012" by B. Pfeiffer, K. Venkataramaniah, U. Czok, C. Scheidenberger COMPILATION 45Cr, 47Ar, 65As, 73Ge, 100Sn, 286Nh; compiled experimental atomic masses; deduced differences with work of B. Pfeiffer et al.
doi: 10.1016/j.adt.2014.05.003
2015CH21 Acta Phys.Pol. B46, 349 (2015) N.Chamel, J.M.Pearson, A.F.Fantina, C.Ducoin, S.Goriely, A.Pastore Brussels-Montreal Nuclear Energy Density Functionals, from Atomic Masses to Neutron Stars
doi: 10.5506/APhysPolB.46.349
2015PE02 Phys.Rev. C 91, 018801 (2015) J.M.Pearson, N.Chamel, A.Pastore, S.Goriely Role of proton pairing in a semimicroscopic treatment of the inner crust of neutron stars
doi: 10.1103/PhysRevC.91.018801
2014PE04 Eur.Phys.J. A 50, 43 (2014) J.M.Pearson, N.Chamel, A.F.Fantina, S.Goriely Symmetry energy: nuclear masses and neutron stars NUCLEAR STRUCTURE Z=10-110; calculated neutron drip line, mass excess, 2n separation energy using HFB nuclear mass models with generalized Skyrme forces.
doi: 10.1140/epja/i2014-14043-8
2013GO11 Phys.Rev. C 88, 024308 (2013) S.Goriely, N.Chamel, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. XIII. The 2012 atomic mass evaluation and the symmetry coefficient ATOMIC MASSES Z=8-110, N=8-250; calculated masses of 8509 nuclei using five Hartree-Fock-Bogoliubov (HFB) mass models using unconventional Skyrme forces; fitted to the evaluated masses in AME-2012; deduced rms deviations from AME-2012 data, symmetry coefficients, charge radii, neutron skin thickness, shell gaps for Z=50, 82, N=28, 50, 82, 126 nuclei. Comparison with experimental data. Relevance of the mass models to a unified treatment of outer and inner crusts and cores of neutron stars.
doi: 10.1103/PhysRevC.88.024308
2013GO18 Phys.Rev. C 88, 061302 (2013) S.Goriely, N.Chamel, J.M.Pearson Hartree-Fock-Bogoliubov nuclear mass model with 0.50 MeV accuracy based on standard forms of Skyrme and pairing functionals ATOMIC MASSES Z>7, N>7; calculated masses for 2353 nuclei using Hartree-Fock-Bogoliubov nuclear mass model with Skyrme force BSk27*, and the pairing parameters. Comparison with evaluated mass data in AME-12.
doi: 10.1103/PhysRevC.88.061302
2012CH04 Phys.Rev. C 85, 015805 (2012) J.Chen, A.A.Chen, G.Amadio, S.Cherubini, H.Fujikawa, S.Hayakawa, J.J.He, N.Iwasa, D.Kahl, L.H.Khiem, S.Kubono, S.Kurihara, Y.K.Kwon, M.La Cognata, J.Y.Moon, M.Niikura, S.Nishimura, J.Pearson, R.G.Pizzone, T.Teranishi, Y.Togano, Y.Wakabayashi, H.Yamaguchi Strong 25Al+p resonances via elastic proton scattering with a radioactive 25Al beam NUCLEAR REACTIONS 1H(25Al, p), [25Al secondary beam from 2H(24Mg, n), E=7.5 MeV/nucleon primary reaction], E=3.4 MeV/nucleon; measured Ep, Ip, energy loss, σ(E, θ). 26Si; deduced levels, resonances, J, π, proton widths. R-matrix analysis of excitation function data. RIKEN-CNS facility. Comparison of energy levels with results from other reaction studies.
doi: 10.1103/PhysRevC.85.015805
2012CH45 Phys.Rev. C 86, 055804 (2012) N.Chamel, R.L.Pavlov, L.M.Mihailov, Ch.J.Velchev, Zh.K.Stoyanov, Y.D.Mutafchieva, M.D.Ivanovich, J.M.Pearson, S.Goriely Properties of the outer crust of strongly magnetized neutron stars from Hartree-Fock-Bogoliubov atomic mass models
doi: 10.1103/PhysRevC.86.055804
2012LE04 Phys.Rev. C 85, 034333 (2012) D.Lebhertz, S.Courtin, F.Haas, D.G.Jenkins, C.Simenel, M.-D.Salsac, D.A.Hutcheon, C.Beck, J.Cseh, J.Darai, C.Davis, R.G.Glover, A.Goasduff, P.E.Kent, G.Levai, P.L.Marley, A.Michalon, J.E.Pearson, M.Rousseau, N.Rowley, C.Ruiz 12C(16O, γ)28Si radiative capture: Structural and statistical aspects of the γ decay NUCLEAR REACTIONS 12C(16O, γ)28Si, E=19.8, 20.5, 21.0 MeV; measured measured energy loss, time of flight, E(28Si recoils), Eγ, Iγ, γ(recoil)-coin, γ(θ), angular momentum distribution using DRAGON spectrometer at TRIUMF; deduced levels, J, π, total and partial radiative capture cross section, dinuclear lifetimes as function of mean angular momentum. Coupled-channel analysis for momentum distributions. GEANT3 simulations. Discussed statistical and structural aspects.
doi: 10.1103/PhysRevC.85.034333
2012PE09 Phys.Rev. C 85, 065803 (2012) J.M.Pearson, N.Chamel, S.Goriely, C.Ducoin Inner crust of neutron stars with mass-fitted Skyrme functionals
doi: 10.1103/PhysRevC.85.065803
2011CH61 Phys.Rev. C 84, 062802 (2011) N.Chamel, A.F.Fantina, J.M.Pearson, S.Goriely Masses of neutron stars and nuclei
doi: 10.1103/PhysRevC.84.062802
2011GO36 J.Korean Phys.Soc. 59, 2100s (2011) S.Goriely, N.Chamel, J.M.Pearson HFB Mass Models for Nucleosynthesis Applications COMPILATION Z≈8-120; calculated Q, mass surfaces using various NN forces, neutron capture rates, abundances.
doi: 10.3938/jkps.59.2100
2011PE16 Phys.Rev. C 83, 065810 (2011) J.M.Pearson, S.Goriely, N.Chamel Properties of the outer crust of neutron stars from Hartree-Fock-Bogoliubov mass models
doi: 10.1103/PhysRevC.83.065810
2010CH11 Phys.Rev. C 81, 045804 (2010) N.Chamel, S.Goriely, J.M.Pearson, M.Onsi Unified description of neutron superfluidity in the neutron-star crust with analogy to anisotropic multiband BCS superconductors
doi: 10.1103/PhysRevC.81.045804
2010GO23 Phys.Rev. C 82, 035804 (2010) S.Goriely, N.Chamel, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. XII. Stiffness and stability of neutron-star matter ATOMIC MASSES Z=8-110, N=8-250; calculated masses for 8509 nuclei using three new Hartree-Fock-Bogoliubov (HFB) mass models, HFB-19, HFB-20, and HFB-21 with unconventional Skyrme forces. 208Pb; calculated isoscalar and isovector effective masses as a function of the radial position, and single-particle proton levels.
doi: 10.1103/PhysRevC.82.035804
2010PE10 Phys.Rev. C 82, 037301 (2010) J.M.Pearson, N.Chamel, S.Goriely Breathing-mode measurements in Sn isotopes and isospin dependence of nuclear incompressibility NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn; analyzed energies of breathing mode isoscalar giant-monopole resonances (GMR) using a higher-order leptodermous expansion; deduced symmetry-incompressibility coefficient Kτ. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.037301
2009CH63 Phys.Rev. C 80, 065804 (2009) N.Chamel, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. XI. Stabilizing neutron stars against a ferromagnetic collapse
doi: 10.1103/PhysRevC.80.065804
2009GO11 Phys.Rev.Lett. 102, 152503 (2009) S.Goriely, N.Chamel, J.M.Pearson Skyrme-Hartree-Fock-Bogoliubov Nuclear Mass Formulas: Crossing the 0.6 MeV Accuracy Threshold with Microscopically Deduced Pairing
doi: 10.1103/PhysRevLett.102.152503
2009GO41 Eur.Phys.J. A 42, 547 (2009) S.Goriely, N.Chamel, J.M.Pearson Recent breakthroughs in Skyrme-Hartree-Fock-Bogoliubov mass formulas ATOMIC MASSES Z=8-110; calculated atomic masses. Comparison with data.
doi: 10.1140/epja/i2009-10784-7
2008BU12 Nucl.Phys. A805, 462c (2008) L.Buchmann, P.Amaudruz, J.D'Auria, D.Hutcheon, C.Matei, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, C.Vockenhuber, P.Walden Nuclear Astrophysics at TRIUMF NUCLEAR REACTIONS 4He(12C, γ), E not given; 1H(26Al, γ), E not given; 4He(40Ca, γ), E(cm)=2.18-4.15 MeV; measured Eγ, Iγ; deduced astrophysical S-factor. RADIOACTIVITY 22Na(β+), 198Au(β-); measured T1/2, temperature dependence not observed. 16N(β-); calculated β-delayed Eα, Iα using GEANT4 code.
doi: 10.1016/j.nuclphysa.2008.02.267
2008CH24 Nucl.Phys. A812, 72 (2008) N.Chamel, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. IX: Constraint of pairing force to 1S0 neutron-matter gap NUCLEAR STRUCTURE Z=8-110; calculated S(n), Q(β), charge radii. Global fit to 2149 mass data. Compared Skyrme-Hartree-Fock-Bogoliubov mass models when constraining the contact pairing force.
doi: 10.1016/j.nuclphysa.2008.08.015
2008GO05 Phys.Rev. C 77, 031301 (2008) Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. VIII. Role of Coulomb exchange NUCLEAR STRUCTURE N>7; Z=8-110; calculated fission barriers, S(n), Q(β), charge radii, mirror nuclei differences. Global fit to 2149 mass data. Compared Skyrme-Hartree-Fock-Bogoliubov mass models when the Coulomb-exchange term is ignored.
doi: 10.1103/PhysRevC.77.031301
2008KA04 Phys.Lett. B 660, 26 (2008) R.Kanungo, A.N.Andreyev, L.Buchmann, B.Davids, G.Hackman, D.Howell, P.Khalili, B.Mills, E.Padilla-Rodal, Steven C.Pieper, J.Pearson, C.Ruiz, G.Ruprecht, A.Shotter, I.Tanihata, C.Vockenhuber, P.Walden, R.B.Wiringa Spectroscopic factors for the 9Li ground state and N = 6 shell closure NUCLEAR REACTIONS 2H(9Li, t), (9Li, d), E=1.68 MeV/nucleon; measured σ(θ); deduced spectroscopic factors.
doi: 10.1016/j.physletb.2007.12.024
2008LE27 Int.J.Mod.Phys. E17, 2044 (2008) D.Lebhertz, S.Courtin, F.Haas, M.-D.Salsac, C.Beck, A.Michalon, M.Rousseau, D.G.Jenkins, P.L.Marley, R.G.Glover, P.E.Kent, D.A.Hutcheon, C.Davis, J.E.Pearson Resonant radiative capture and molecular states in 24Mg and 28Si NUCLEAR REACTIONS 12C(12C, γ), 12C(16O, γ), E=9-12 MeV; measured Eγ, Iγ, particle-γ-coin; deduced feeding states, J, π, energy levels.
doi: 10.1142/S0218301308011069
2008ON01 Phys.Rev. C 77, 065805 (2008), Publishers note Phys.Rev. C 78, 059902 (2008) M.Onsi, A.K.Dutta, H.Chatri, S.Goriely, N.Chamel, J.M.Pearson Semi-classical equation of state and specific-heat expressions with proton shell corrections for the inner crust of a neutron star
doi: 10.1103/PhysRevC.77.065805
2008RA23 Phys.Rev.Lett. 101, 212501 (2008) R.Raabe, A.Andreyev, M.J.G.Borge, L.Buchmann, P.Capel, H.O.U.Fynbo, M.Huyse, R.Kanungo, T.Kirchner, C.Mattoon, A.C.Morton, I.Mukha, J.Pearson, J.Ponsaers, J.J.Ressler, K.Riisager, C.Ruiz, G.Ruprecht, F.Sarazin, O.Tengblad, P.Van Duppen, P.Walden β-Delayed Deuteron Emission from 11Li: Decay of the Halo RADIOACTIVITY 11Li(β-); measured β-delayed deuteron spectrum. Deduced transition probability.
doi: 10.1103/PhysRevLett.101.212501
2008RU01 J.Phys.(London) G35, 014017 (2008) G.Ruprecht, C.Vockenhuber, C.Ruiz, L.Buchmann, J.Pearson, D.Ottewell, K.Czerski, A.Huke On the possible influence of electron screening on the lifetime of radioactive nuclei RADIOACTIVITY 22Na(β+) [from 27Al(p, X), E=70 MeV]; measured Eγ, Iγ, T1/2 as function of temperature. Deduced influence of electron screening on T1/2.
doi: 10.1088/0954-3899/35/1/014017
2008VO01 J.Phys.(London) G35, 014034 (2008) C.Vockenhuber, C.O.Ouellet, L.-S.The, L.Buchmann, J.Caggiano, A.A.Chen, J.M.D'Auria, B.Davids, L.Fogarty, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, D.Ottewell, M.Paul, M.M.Pavan, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, A.Wallner 40Ca(α, γ)44Ti and the production of 44Ti in supernovae NUCLEAR REACTIONS 4He(40Ca, γ), E=600-1150 keV/nucleon; measured Eγ, γγ-, (recoil)γ-coin, excitation function.
doi: 10.1088/0954-3899/35/1/014034
2007GO18 Phys.Rev. C 75, 064312 (2007) S.Goriely, M.Samyn, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. VII. Simultaneous fits to masses and fission barriers NUCLEAR STRUCTURE Z > 7, N > 7; analyzed masses and fission barrier data using a new HFB mass model.
doi: 10.1103/PhysRevC.75.064312
2007GR11 Nucl.Instrum.Methods Phys.Res. B261, 1089 (2007) U.Greife, J.Livesay, C.Jewett, K.Chipps, F.Sarazin, D.Bardayan, J.Blackmon, C.Nesaraja, M.S.Smith, A.Champagne, R.Fitzgerald, K.Jones, J.Thomas, R.Kozub, L.Buchmann, J.Caggiano, D.Hunter, D.Hutcheon, A.Olin, D.Ottewell, J.Rogers, C.Ruiz, G.Ruprecht, M.Trinczek, C.Vockenhuber, S.Bishop, J.D'Auria, M.Lamay, W.Liu, C.Wrede, M.L.Chatterjee, A.A.Chen, J.Pearson, S.Engel, A.M<.Laird, D.Gigliotti, A.Hussein Recent results of experiments with radioactive 21Na and 7Be ion beams NUCLEAR REACTIONS 1H(21Na, γ), E=1.18 MeV/nucleon; measured Eγ, Iγ, yields. 1H(7Be, X), E=4-27 MeV; measured elastic and inelastic scattering σ.
doi: 10.1016/j.nimb.2007.03.055
2007JE08 Phys.Rev. C 76, 044310 (2007) D.G.Jenkins, B.R.Fulton, P.Marley, S.P.Fox, R.Glover, R.Wadsworth, D.L.Watson, S.Courtin, F.Haas, D.Lebhertz, C.Beck, P.Papka, M.Rousseau, A.Sanchez i Zafra, D.A.Hutcheon, C.Davis, D.Ottewell, M.M.Pavan, J.Pearson, C.Ruiz, G.Ruprecht, J.Slater, M.Trinczek, J.D'Auria, C.J.Lister, P.Chowdhury, C.Andreoiu, J.J.Valiente-Dobon, S.Moon Decay strength distributions in 12C(12C, γ) radiative capture NUCLEAR REACTIONS 12C(12C, γ), E(cm)=6.0, 6.8, 7.5, 8.0 MeV; measured Eγ, Iγ, γγ, (recoil)γ-coin; deduced multipolarities, on and off resonances. TRIUMF-ISAC DRAGON recoil spectrometer, GEANT3 array.
doi: 10.1103/PhysRevC.76.044310
2007VO03 Nucl.Instrum.Methods Phys.Res. B259, 688 (2007) C.Vockenhuber, C.O.Ouellet, L.Buchmann, J.Caggiano, A.A.Chen, J.M.D'Auria, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, K.Jayamanna, D.Ottewell, M.Paul, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, A.Wallner The 40Ca(α, γ)44Ti reaction at DRAGON NUCLEAR REACTIONS 4He(40Ca, γ)44Ti, E=1.135 MeV/nucleon; measured yield and resonance strength at DRAGON recoil mass spectrometer.
doi: 10.1016/j.nimb.2007.01.222
2007VO06 Phys.Rev. C 76, 035801 (2007) C.Vockenhuber, C.O.Ouellet, L.-S.The, L.Buchmann, J.Caggiano, A.A.Chen, H.Crawford, J.M.D'Auria, B.Davids, L.Fogarty, D.Frekers, A.Hussein, D.A.Hutcheon, W.Kutschera, A.M.Laird, R.Lewis, E.O'Connor, D.Ottewell, M.Paul, M.M.Pavan, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, B.Wales, A.Wallner Measurement of the 40Ca(α, γ)44Ti reaction relevant for supernova nucleosynthesis NUCLEAR REACTIONS 4He(40Ca, γ)44Ti, E=0.60-1.15 MeV/nucleon; measured recoil energies, yields, and cross section.
doi: 10.1103/PhysRevC.76.035801
2007ZY01 Nucl.Instrum.Methods Phys.Res. B254, 17 (2007) J.Zylberberg, D.Hutcheon, L.Buchmann, J.Caggiano, W.R.Hannes, A.Hussein, E.O'Connor, D.Ottewell, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, C.Vockenhuber Charge-state distributions after radiative capture of helium nuclei by carbon beam NUCLEAR REACTIONS 4He(12C, γ), E=1.068 MeV/nucleon; measured beam and recoil charge state distributions.
doi: 10.1016/j.nimb.2006.09.019
2006GO21 Nucl.Phys. A773, 279 (2006) S.Goriely, M.Samyn, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas VI: Weakened pairing NUCLEAR STRUCTURE Z=8-120; A=16-360; analysed atomic masses. Nuclear matter properties discussed. Skyrme-Hartree-Fock-Bogoliubov approach, comparison with data and earlier models.
doi: 10.1016/j.nuclphysa.2006.05.002
2006MA81 Phys.Rev.Lett. 97, 242503 (2006) C.Matei, L.Buchmann, W.R.Hannes, D.A.Hutcheon, C.Ruiz, C.R.Brune, J.Caggiano, A.A.Chen, J.D'Auria, A.Laird, M.Lamey, ZH.Li, WP.Liu, A.Olin, D.Ottewell, J.Pearson, G.Ruprecht, M.Trinczek, C.Vockenhuber, C.Wrede Measurement of the Cascade Transition via the First Excited State of 16O in the 12C(α, γ)16O Reaction, and Its S Factor in Stellar Helium Burning NUCLEAR REACTIONS 4He(12C, γ), E(cm)=2.22-5.42 MeV; measured Eγ, Iγ, (particle)γ-coin; deduced σ, astrophysical S-factor. Recoil separator.
doi: 10.1103/PhysRevLett.97.242503
2006MU07 Phys.Rev. C 73, 034320 (2006) A.St.J.Murphy, M.Aliotta, T.Davinson, C.Ruiz, P.J.Woods, J.M.D'Auria, L.Buchmann, A.A.Chen, A.M.Laird, F.Sarazin, P.Walden, B.R.Fulton, J.E.Pearson, B.A.Brown Level structure of 21Mg: Nuclear and astrophysical implications NUCLEAR REACTIONS 1H(20Na, p), E=1.25, 1.60 MeV/nucleon; measured recoil proton spectra, σ(θ). 21Mg deduced resonance energies, widths. 20Na(p, γ), E=low; calculated astrophysical reaction rate.
doi: 10.1103/PhysRevC.73.034320
2006PE41 Nucl.Phys. A777, 623 (2006) Nuclear mass formulas for astrophysics
doi: 10.1016/j.nuclphysa.2004.06.005
2006RU09 Phys.Rev.Lett. 96, 252501 (2006) C.Ruiz, A.Parikh, J.Jose, L.Buchmann, J.A.Caggiano, A.A.Chen, J.A.Clark, H.Crawford, B.Davids, J.M.D'Auria, C.Davis, C.Deibel, L.Erikson, L.Fogarty, D.Frekers, U.Greife, A.Hussein, D.A.Hutcheon, M.Huyse, C.Jewett, A.M.Laird, R.Lewis, P.Mumby-Croft, A.Olin, D.F.Ottewell, C.V.Ouellet, P.Parker, J.Pearson, G.Ruprecht, M.Trinczek, C.Vockenhuber, C.Wrede Measurement of the Ec.m. = 184 keV Resonance Strength in the 26gAl(p, γ)27Si Reaction NUCLEAR REACTIONS 1H(26Al, γ), E=5.122, 5.226, 5.850 MeV; measured Eγ, (recoil)γ-coin. 26Al(p, γ), E(cm) ≈ 184 keV; deduced resonance strength. Astrophysical implications discussed.
doi: 10.1103/PhysRevLett.96.252501
2006RU12 Eur.Phys.J. A 27, Supplement 1, 315 (2006) G.Ruprecht, D.Gigliotti, P.Amaudruz, L.Buchmann, S.P.Fox, B.R.Fulton, T.Kirchner, A.M.Laird, P.D.Mumby-Croft, R.Openshaw, M.M.Pavan, J.Pearson, G.Sheffer, P.Walden Status of the TRIUMF annular chamber for the tracking and identification of charged particles (TACTIC)
doi: 10.1140/epja/i2006-08-048-y
2005BU39 Phys.Rev. C 72, 057305 (2005) Charge radii in macroscopic-microscopic mass models NUCLEAR STRUCTURE 108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125Sn; calculated charge radii. Finite-range droplet model and finite-range liquid drop model compared with data.
doi: 10.1103/PhysRevC.72.057305
2005EN07 Nucl.Instrum.Methods Phys.Res. A 553, 491 (2005) S.Engel, D.Hutcheon, S.Bishop, L.Buchmann, J.Caggiano, M.L.Chatterjee, A.A.Chen, J.D'auria, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, C.C.Jewett, A.M.Laird, M.Lamey, W.Liu, A.Olin, D.Ottewell, J.Pearson, C.Ruiz, G.Ruprecht, M.Trinczek, C.Vockenhuber, C.Wrede Commissioning the DRAGON facility at ISAC NUCLEAR REACTIONS 20Ne(p, γ), 21Ne(p, γ), 24Mg(p, γ), E=214 keV-1.1 MeV; measured products, Eγ, Iγ; deduced resonance parameters. Data were imported from EXFOR entry C1403.
doi: 10.1016/j.nima.2005.07.029
2005GO07 Nucl.Phys. A750, 425 (2005) S.Goriely, M.Samyn, J.M.Pearson, M.Onsi Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. IV: Neutron-matter constraint
doi: 10.1016/j.nuclphysa.2005.01.009
2005GO32 Nucl.Phys. A758, 587c (2005) S.Goriely, P.Demetriou, H.-Th.Janka, J.M.Pearson, M.Samyn The r-process nucleosynthesis: a continued challenge for nuclear physics and astrophysics
doi: 10.1016/j.nuclphysa.2005.05.107
2005GO39 Eur.Phys.J. A 25, Supplement 1, 71 (2005) S.Goriely, M.Samyn, J.M.Pearson, E.Khan Recent progress in mass predictions NUCLEAR STRUCTURE Z=8-120; A=16-340; analyzed atomic masses. Nuclear matter properties discussed. Skyrme-Hartree-Fock-Bogoliubov approach, comparison with data.
doi: 10.1140/epjad/i2005-06-022-4
2005JE03 Phys.Rev. C 71, 041301 (2005) D.G.Jenkins, B.R.Fulton, J.Pearson, C.J.Lister, M.P.Carpenter, S.J.Freeman, N.J.Hammond, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, A.H.Wuosmaa, P.Fallon, A.Gorgen, A.O.Macchiavelli, M.McMahan, M.Freer, F.Haas Doorway states as a principal decay pathway in 12C(12C, γ) radiative capture NUCLEAR REACTIONS 12C(12C, γ), E(cm) ≈ 8 MeV; measured Eγ, Iγ, σ; deduced role of doorway states. Gammasphere array.
doi: 10.1103/PhysRevC.71.041301
2005PE17 Nucl.Phys. A758, 651c (2005) J.M.Pearson, M.Onsi, S.Goriely, M.Samyn Hartree-Fock-Bogoliubov mass formulas and the equation of state of neutron-star matter
doi: 10.1016/j.nuclphysa.2005.05.117
2005RU01 Phys.Rev. C 71, 025802 (2005) C.Ruiz, T.Davinson, F.Sarazin, I.Roberts, A.Robinson, P.J.Woods, L.Buchmann, A.C.Shotter, P.Walden, N.M.Clarke, A.A.Chen, B.R.Fulton, D.Groombridge, J.Pearson, A.S.Murphy Multichannel R-matrix analysis of elastic and inelastic resonances in the 21Na + p compound system NUCLEAR REACTIONS 1H(21Na, p), E=580-1560 keV/nucleon; measured elastic and inelastic recoil proton spectra, σ(θ). 22Mg deduced resonance energies, widths, J, π, analog states. 21Na(p, γ), E=low; calculated reaction rate. R-matrix analysis.
doi: 10.1103/PhysRevC.71.025802
2005RU15 Nucl.Phys. A758, 166c (2005) C.Ruiz, M.Aliotta, R.E.Azuma, R.N.Boyd, L.Buchmann, A.Chen, N.M.Clarke, J.M.D'Auria, T.Davinson, B.R.Fulton, D.Groombridge, D.Hutcheon, A.M.Laird, A.S.Murphy, J.Pearson, I.Roberts, A.Robinson, F.Sarazin, A.C.Shotter, P.Walden, P.J.Woods Multichannel R-matrix analysis of elastic and inelastic resonances in the 20, 21Na+p compound systems NUCLEAR REACTIONS 1H(20Na, p), (21Na, p), E(cm) ≈ 500-1600 keV; measured recoil proton spectra; deduced excitation functions. 22Ne deduced resonance energies, widths.
doi: 10.1016/j.nuclphysa.2005.05.171
2005SA56 Phys.Rev. C 72, 044316 (2005) M.Samyn, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. V. Extension to fission barriers NUCLEAR STRUCTURE Z=80-130; A=198-314; calculated deformation and fission barrier parameters. Skyrme-Hartree-Fock-Bogoliubov approach, comparisons with data.
doi: 10.1103/PhysRevC.72.044316
2005TR11 Nucl.Phys. A758, 729c (2005) M.Trinczek, C.C.Jewett, J.M.D'Auria, S.Bishop, L.Buchmann, A.A.Chen, S.Engel, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, D.Hutcheon, J.Jose, A.M.Laird, M.Lamey, R.Lewis, A.Olin, D.Ottewell, P.Parker, M.M.Pavan, J.E.Pearson, J.Rogers, C.Ruiz, C.Wrede Direct Measurement of the 21Na(p, γ)22Mg Reaction: Resonance Strengths and Gamma-Gamma Analysis NUCLEAR REACTIONS 1H(21Na, γ), E(cm)=200-1135 keV; measured Eγ, Iγ, γγ-coin. 22Mg deduced levels, J, π, resonance strengths.
doi: 10.1016/j.nuclphysa.2005.05.131
2004DU13 Phys.Rev. C 69, 052801 (2004) A.K.Dutta, M.Onsi, J.M.Pearson Proton-shell effects in neutron-star matter
doi: 10.1103/PhysRevC.69.052801
2004SA55 Phys.Rev. C 70, 044309 (2004) M.Samyn, S.Goriely, M.Bender, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. III. Role of particle-number projection NUCLEAR STRUCTURE Z=8-120; calculated masses. 230,231,233Th, 235,236,237,238,239U, 237,238Np, 235,237,238,239,240,241,243,244Pu, 239,240,241,242,243,244Am, 241,242,243,244,245Cm, 244Bk; analyzed shape isomer energies. 32S, 208Pb; calculated charge density distributions. Skyrme-Hartree-Fock-Bogoliubov mass formulas.
doi: 10.1103/PhysRevC.70.044309
2003AZ05 Nucl.Phys. A718, 119c (2003) R.E.Azuma, S.Bishop, L.Buchmann, M.L.Chatterjee, A.A.Chen, J.M.D'Auria, T.Davinson, S.Engel, B.R.Fulton, D.Gigliotti, U.Greife, D.Groombridge, D.Hunter, A.Hussein, D.Hutcheon, C.Jewett, J.D.King, N.Khan, S.Kubono, A.M.Laird, M.Lamey, R.Lewis, L.Ling, W.Liu, S.Michimasa, A.S.Murphy, A.Olin, D.Ottewell, P.Parker, J.Pearson, I.Roberts, A.Robinson, J.G.Rogers, G.Roy, C.Ruiz, F.Sarazin, A.C.Shotter, H.Sprenger, F.Strieder, P.Walden, P.J.Woods, C.Wrede Results of 21Na + p Experiments at ISAC NUCLEAR REACTIONS 1H(21Na, 21Na), E=0.45-1.4 MeV; measured recoil proton spectra; deduced excitation function. 1H(21Na, γ), E=220, 855 keV/nucleon; measured Eγ, (particle)γ-coin. 22Mg deduced resonance features.
doi: 10.1016/S0375-9474(03)00688-2
2003GO31 Phys.Rev. C 68, 054325 (2003) S.Goriely, M.Samyn, M.Bender, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. II. Role of the effective mass NUCLEAR STRUCTURE Z=8-120; calculated masses; deduced role of effective mass. 16O, 132Sn, 208Pb; calculated single-particle energy levels. Skyrme-Hartree-Fock-Bogoliubov approach, comparisons with data.
doi: 10.1103/PhysRevC.68.054325
2003LU10 Rev.Mod.Phys. 75, 1021 (2003) D.Lunney, J.M.Pearson, C.Thibault Recent trends in the determination of nuclear masses
doi: 10.1103/RevModPhys.75.1021
2003SA26 Nucl.Phys. A725, 69 (2003) M.Samyn, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas I: Role of density dependence in pairing force
doi: 10.1016/S0375-9474(03)01578-1
2003SA34 Nucl.Phys. A718, 653c (2003) M.Samyn, S.Goriely, J.M.Pearson Nuclear Mass Predictions Within The Skyrme HFB Theory NUCLEAR STRUCTURE A=2-270; calculated masses. Z=34-70; calculated shell gaps. Self-consistent Skyrme HFB approach.
doi: 10.1016/S0375-9474(03)00877-7
2002GO26 Phys.Rev. C66, 024326 (2002) S.Goriely, M.Samyn, P.H.Heenen, J.M.Pearson, F.Tondeur Hartree-Fock mass formulas and extrapolation to new mass data NUCLEAR STRUCTURE Z=8-120; analyzed masses, mass formulas; deduced parameters. ATOMIC MASSES Z=8-120; analyzed masses, mass formulas; deduced parameters.
doi: 10.1103/PhysRevC.66.024326
2002ON01 Phys.Rev. C65, 047302 (2002) Equation of State of Stellar Nuclear Matter and the Effective Nucleon Mass
doi: 10.1103/PhysRevC.65.047302
2002PE19 Eur.Phys.J. A 15, 13 (2002) J.M.Pearson, S.Goriely, M.Samyn A Hartree-Fock nuclear mass formula
doi: 10.1140/epja/i2001-10215-y
2002RU03 Phys.Rev. C65, 042801 (2002) C.Ruiz, F.Sarazin, L.Buchmann, T.Davinson, R.E.Azuma, A.A.Chen, B.R.Fulton, D.Groombridge, L.Ling, A.Murphy, J.Pearson, I.Roberts, A.Robinson, A.C.Shotter, P.Walden, P.J.Woods Strong Resonances in Elastic Scattering of Radioactive 21Na on Protons NUCLEAR REACTIONS 1H(21Na, 21Na'), E(cm)=0.45-1.4 MeV; measured σ(θ), recoil proton spectra. 22Mg deduced resonance features.
doi: 10.1103/PhysRevC.65.042801
2002SA14 Nucl.Phys. A700, 142 (2002) M.Samyn, S.Goriely, P.-H.Heenen, J.M.Pearson, F.Tondeur A Hartree-Fock-Bogoliubov Mass Formula NUCLEAR STRUCTURE Z=8-120; calculated masses, binding energies. Hartree-Fock-Bogoliubov method.
doi: 10.1016/S0375-9474(01)01316-1
2001BU30 Phys.Rev. C64, 067303 (2001) F.Buchinger, J.M.Pearson, S.Goriely Nuclear Charge Radii in Modern Mass Formulas: An update NUCLEAR STRUCTURE Z=11-95; calculated radii. Comparison with data, two mass formulas compared.
doi: 10.1103/PhysRevC.64.067303
2001FA22 Nucl.Phys. A696, 396 (2001) M.Farine, J.M.Pearson, F.Tondeur Skyrme Force with Surface-Peaked Effective Mass NUCLEAR STRUCTURE 84Ni, 122Zr, 190Gd, 266Pb, 276U; calculated mass, neutron separation energy, Qβ. 16O, 90Zr, 208Pb; calculated single-particle levels. Skyrme force with effective mass.
doi: 10.1016/S0375-9474(01)01136-8
2001GE11 Astrophys.J. 551, L193 (2001) M.Gerin, J.C.Pearson, E.Roueff, E.Falgarone, T.G.Phillips Determination of the Hyperfine Structure of N2D+ NUCLEAR MOMENTS 1,2H, N; measured hfs of N2H+ and N2D+. Astrophysical implications discussed.
doi: 10.1086/320029
2001GO20 At.Data Nucl.Data Tables 77, 311 (2001) S.Goriely, F.Tondeur, J.M.Pearson A Hartree-Fock Nuclear Mass Table ATOMIC MASSES Z=8-120; calculated masses, deformation parameters. Hartree-Fock-BCS approach, Skyrme force, pairing force, Wigner term. NUCLEAR STRUCTURE Z=8-120; calculated masses, deformation parameters. Hartree-Fock-BCS approach, Skyrme force, pairing force, Wigner term.
doi: 10.1006/adnd.2000.0857
2001MA04 Nucl.Phys. A679, 337 (2001) A.Mamdouh, J.M.Pearson, M.Rayet, F.Tondeur Fission Barriers of Neutron-Rich and Superheavy Nuclei Calculated with the ETFSI Method NUCLEAR STRUCTURE Z=84-120; A=214-318; calculated fission barrier heights. Extended Thomas-Fermi plus Strutinsky integral method.
doi: 10.1016/S0375-9474(00)00358-4
2001PE13 Phys.Rev. C64, 027301 (2001) Isovector Effective Mass in the Skyrme-Hartree-Fock Method NUCLEAR STRUCTURE 84Ni, 122Zr, 154Sn, 190Gd, 266Pb, 276U, 300Cm; calculated mass, neutron separation energies, Qβ, level densities. Skyrme-Hartree-Fock method.
doi: 10.1103/PhysRevC.64.027301
2001PE15 Phys.Lett. 513B, 319 (2001) Skyrme Hartree-Fock Method and the Spin-Orbit Term of the Relativistic Mean Field NUCLEAR STRUCTURE 114,116,118,120,122,124,126Zr; calculated total energy. 84Ni, 122Zr, 154Sn, 190Gd, 266Pb, 276U, 300Cm; calculated masses, one-neutron separation energies, Qβ. 40,60Ca, 208,266Pb; calculated neutron spin-orbit field. 36Ne, 38Mg, 124Zr; calculated neutron spin-orbit splitting. Comparison of Skyrme-Hartree-Fock and relativistic mean-field calculations.
doi: 10.1016/S0370-2693(01)00375-6
2001PE26 Hyperfine Interactions 132, 59 (2001) The Quest for a Microscopic Nuclear Mass Formula
doi: 10.1023/A:1011973100463
2000DU06 Phys.Rev. C61, 054303 (2000) A.K.Dutta, J.M.Pearson, F.Tondeur Triaxial Nuclei Calculated with the Extended Thomas-Fermi plus Strutinsky Integral (ETFSI) Method NUCLEAR STRUCTURE 62Zn, 74Ge, 110,111,112,113,114,115,116,117,118Zr, 132Ba, 134Ce, 138Sm, 168Er, 186W, 188,192Os, 222Ra, 233Th, 236,262U, 271Np, 240Pu, 244Cm, 287Bk, 252Cf, 255,286Fm, 259,292Rf, 294Hs, 288,294Cn, 298Fl; calculated ground state energy shift due to triaxial deformation. 233Th, 236,262U, 240Pu, 244Cm, 287Bk, 252Cf, 255,286Fm, 292Rf, 294Hs, 288,294Cn, 298Fl; calculated fission barrier energy shift due to triaxial deformation. Extended Thomas-Fermi plus Strutinsky integral method.
doi: 10.1103/PhysRevC.61.054303
2000PE08 Nucl.Phys. A668, 163 (2000) Nuclear-Matter Symmetry Coefficient and Nuclear Masses NUCLEAR STRUCTURE 60Ca, 101As, 136Ru, 153Sn, 184Ce, 202Dy, 218Ta, 266Pb, 274Th, 300Cf; calculated masses, neutron separation energies, Qβ; deduced constraint on nuclear matter symmetry coefficient. Extended Thomas-Fermi plus Strutinsky integral, several force parameterizations compared. ATOMIC MASSES 60Ca, 101As, 136Ru, 153Sn, 184Ce, 202Dy, 218Ta, 266Pb, 274Th, 300Cf; calculated masses, neutron separation energies, Qβ; deduced constraint on nuclear matter symmetry coefficient. Extended Thomas-Fermi plus Strutinsky integral, several force parameterizations compared.
doi: 10.1016/S0375-9474(99)00431-5
2000TO06 Phys.Rev. C62, 024308 (2000) F.Tondeur, S.Goriely, J.M.Pearson, M.Onsi Towards a Hartree-Fock Mass Formula
doi: 10.1103/PhysRevC.62.024308
1999PE22 Acta Phys.Hung.N.S. 10, 159 (1999) J.M.Pearson, F.Tondeur, A.Mamdouh, M.Rayet Nuclear Masses and Fission Barriers via the ETFSI Method NUCLEAR STRUCTURE Z=92; calculated fission barriers for N ≈ 140-190. ETFSI method, Skyrme force.
1998MA86 Nucl.Phys. A644, 389 (1998); Erratum Nucl.Phys. A648, 282 (1999) A.Mamdouh, J.M.Pearson, M.Rayet, F.Tondeur Large-Scale Fission-Barrier Calculations with the ETFSI Method NUCLEAR STRUCTURE Z=80-100; calculated fission barrier heights. Extended Thomas-Fermi plus Strutinsky Integral method. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(98)00576-4
1998NA21 Phys.Rev. C58, 878 (1998) Spin-Orbit Field and Extrapolated Properties of Exotic Nuclei NUCLEAR STRUCTURE 132Sn, 208,266Pb; calculated single-particle levels. 60Ca, 118Kr, 136Ru, 154Sn, 184Ce, 202Dy, 228W, 266Pb, 274Th, 300Cf; calculated masses, beta-decay energy, neutron separation energy. Several force parameter sets compared.
doi: 10.1103/PhysRevC.58.878
1997BO24 Nucl.Phys. A621, 307c (1997) I.N.Borzov, S.Goriely, J.M.Pearson Microscopic Calculations of β-Decay Characteristics Near the A = 130 r-Process Peak RADIOACTIVITY 125,126,127,128,129,130,131,132,133,134,135Cd(β-); calculated T1/2. 114,115,116,117,118,119,120,121,122,123,124,125,126,127,128Ru, 117,118,119,120,121,122,123,124,125,126,127,128,129,130,131Rh, 118,119,120,121,122,123,124,125,126,127,128,129,130,131,132Pd, 119,120,121,122,123,124,125,126,127,128,129,130,131,132,133Ag, 125,126,127,128,129,130,131,132,133,134Cd, 131In; calculated β-decay yield ratios for various models.
doi: 10.1016/S0375-9474(97)00260-1
1997FA06 Nucl.Phys. A615, 135 (1997) M.Farine, J.M.Pearson, F.Tondeur Nuclear-Matter Incompressibility from Fits of Generalized Skyrme Force to Breathing-Mode Energies NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 112,114,116,120,124,132Sn, 144Sm, 208Pb; calculated internal energy, rms charge radius. Breathing modes, generalized Skyrme forces.
doi: 10.1016/S0375-9474(96)00453-8
1997ON01 Phys.Rev. C55, 3139 (1997) M.Onsi, H.Przysiezniak, J.M.Pearson Equation of State of Stellar Nuclear Matter in the Temperature-Dependent Extended Thomas-Fermi Formalism
doi: 10.1103/PhysRevC.55.3139
1997ON02 Phys.Rev. C55, 3166 (1997) M.Onsi, R.C.Nayak, J.M.Pearson, H.Freyer, W.Stocker Skyrme Representation of a Relativistic Spin-Orbit Field
doi: 10.1103/PhysRevC.55.3166
1996PE22 Phys.Lett. 387B, 455 (1996) J.M.Pearson, R.C.Nayak, S.Goriely Nuclear Mass Formula with Bogolyubov-Enchanced Shell-Quenching: Application to r-process NUCLEAR STRUCTURE Z=55-80; calculated magic neutron gaps. N=55-90; calculated two-neutron separation energies. A=80-200; calculated abundances, masses from different models; deduced r-process implications. Mass formula with Bogolyubov-enhanced self-quenching.
doi: 10.1016/0370-2693(96)01071-4
1995AB38 At.Data Nucl.Data Tables 61, 127 (1995) Y.Aboussir, J.M.Pearson, A.K.Dutta, F.Tondeur Nuclear Mass Formula via an Approximation to the Hartree-Fock Method NUCLEAR STRUCTURE A=36-300; calculated masses, n-, p-separation, β-decay energies. Extended Thomas-Fermi, plus Strutinsky integral method.
doi: 10.1016/S0092-640X(95)90014-4
1995NA17 Phys.Rev. C52, 2254 (1995) Even-Odd Staggering of Pairing-Force Strength NUCLEAR STRUCTURE Z=30-100; N=30-144; analyzed mass data; deduced fourth-order even-odd mass difference rms errors. A=80-235; analyzed Q(β) data; deduced rms errors. High speed Hartree-Fock approximation, Skyrme force.
doi: 10.1103/PhysRevC.52.2254
1994BU06 Phys.Rev. C49, 1402 (1994) F.Buchinger, J.E.Crawford, A.K.Dutta, J.M.Pearson, F.Tondeur Nuclear Charge Radii in Modern Mass Formulas NUCLEAR STRUCTURE 78,80,82,84,86,88,90,92,94,96,98,100Sr; calculated β2 deformation parameter. A=36-238; calculated absolute rms charge radii. Extended Thomas-Fermi, finite-range droplet models mass formula.
doi: 10.1103/PhysRevC.49.1402
1994ON01 Phys.Rev. C50, 460 (1994) M.Onsi, H.Przysiezniak, J.M.Pearson Equation of State of Homogeneous Nuclear Matter and the Symmetry Coefficient
doi: 10.1103/PhysRevC.50.460
1994ON02 Z.Phys. A348, 255 (1994) M.Onsi, A.M.Chaara, J.M.Pearson On the Fermi Functions I(-)(n+(1/2))
doi: 10.1007/BF01305881
1994PE12 Phys.Rev. C50, 185 (1994) Relativistic Mean-Field Theory and a Density-Dependent Spin-Orbit Skyrme Force
doi: 10.1103/PhysRevC.50.185
1994VO07 Phys.Lett. 324B, 279 (1994) D.Von-Eiff, J.M.Pearson, W.Stocker, M.K.Weigel Relativistic Semi-Classical Analysis of Nuclear Surface-Symmetry Properties
doi: 10.1016/0370-2693(94)90194-5
1994VO11 Phys.Rev. C50, 831 (1994) D.Von-Eiff, J.M.Pearson, W.Stocker, M.K.Weigel Relativistic Hartree Calculations of Nuclear Compressional Properties NUCLEAR STRUCTURE 90Zr, 112,114,116,120,124Sn, 144Sm, 208Pb; calculated compressibilities, breathing mode energies. Relativistic Hartree theory.
doi: 10.1103/PhysRevC.50.831
1992AB08 Nucl.Phys. A549, 155 (1992) Y.Aboussir, J.M.Pearson, A.K.Dutta, F.Tondeur Thomas-Fermi Approach to Nuclear-Mass Formula (IV). The ETFSI-1 Mass Formula NUCLEAR STRUCTURE A=36-300; analyzed mass data; calculated equilibrium deformations, fission barriers; deduced Skyrme, δ-function pairing forces parameters. Hartree-Fock, BCS method, semi-classical approximations.
doi: 10.1016/0375-9474(92)90038-L
1991PE03 Nucl.Phys. A528, 1 (1991) J.M.Pearson, Y.Aboussir, A.K.Dutta, R.C.Nayak, M.Farine, F.Tondeur Thomas-Fermi Approach to Nuclear Mass Formula (III). Force Fitting and Construction of Mass Table NUCLEAR STRUCTURE A=100-260; calculated energies, equilibrium deformation parameters. 186Os, 210Po, 240Pu, 250Cm, 262U; calculated fission barriers. Thomas-Fermi approach to mass formula.
doi: 10.1016/0375-9474(91)90418-6
1991PE15 Phys.Lett. 271B, 12 (1991) The Incompressibility of Nuclear Matter and the Breathing Mode NUCLEAR STRUCTURE 112,114,116,120,124Sn, 144Sm, 208Pb; analyzed breathing mode; deduced unique nuclear matter incompressibility value nonderivability.
doi: 10.1016/0370-2693(91)91269-2
1990NA21 Nucl.Phys. A516, 62 (1990) R.C.Nayak, J.M.Pearson, M.Farine, P.Gleissl, M.Brack Leptodermous Expansion of Finite-Nucleus Incompressibility NUCLEAR STRUCTURE A ≤ 250; 16O, 40,48Ca, 56Ni, 90Zr, 112,132Sn, 140Ce, 208Pb; calculated compressibility vs mass. Leptodermous expansion.
doi: 10.1016/0375-9474(90)90049-R
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