NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = P.Schuck Found 216 matches. Showing 1 to 100. [Next]2023PA39 Eur.Phys.J. A 59, 241 (2023) Generic size dependences of pairing in ultrasmall systems: electronic nano-devices and atomic nuclei
doi: 10.1140/epja/s10050-023-01155-9
2023SC12 Eur.Phys.J. A 59, 164 (2023) Corrections to local-density approximation for superfluid trapped fermionic atoms from the Wigner-Kirkwood h-bar expansion
doi: 10.1140/epja/s10050-023-01077-6
2022BA09 Phys.Rev. C 105, 044323 (2022) E.B.Balbutsev, I.V.Molodtsova, A.V.Sushkov, N.Yu.Shirikova, P.Schuck Spin-isospin structure of the nuclear scissors mode NUCLEAR STRUCTURE 148,150Nd, 148,150,152,154Sm, 156,158,160Gd, 160,162,164Dy, 166,168,170Er, 172,174,176Yb, 176,178,180Hf, 182,184,186W, 190,192Os, 194,196Pt, 232Th, 236,238U; calculated levels, J, π, B(M1), scissor resonances fine structure features. 164Dy; calculated B(E2), strengths of currents. Calculations with the use of the Wigner function moments (WFM) and quasiparticle-phonon nuclear model (QPNM) methods. Comparison to experimental values obtained with NRF and photoneutron measurements methods.
doi: 10.1103/PhysRevC.105.044323
2022BL08 Eur.Phys.J. A 58, 236 (2022) D.Blaschke, H.Horiuchi, M.Kimura, G.Ropke, P.Schuck Topical collection on light clusters in nuclei and nuclear matter: nuclear structure and decay, heavy-ion collisions, and astrophysics
doi: 10.1140/epja/s10050-022-00867-8
2022LE04 Eur.Phys.J. A 58, 58 (2022) S.Lei, S.Li, Q.Zhao, N.Wan, M.Lyu, Z.Ren, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, B.Zhou Investigating the proton-halo structure of 8B via the extended THSR wave function NUCLEAR STRUCTURE 8B; calculated standard deviation of the ground state Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave function, contour maps of the energy surface, spatial matter density and valence density distribution, proton density distributions, rms radii and quadrupole moments; deduced proton halo structure in the ground state.
doi: 10.1140/epja/s10050-022-00705-x
2022ZH19 Phys.Rev. C 105, 044326 (2022) Y.Zhang, A.Bjelcic, T.Niksic, E.Litvinova, P.Ring, P.Schuck Many-body approach to superfluid nuclei in axial geometry NUCLEAR STRUCTURE 28Si; calculated single-particle energies, Nilsson diagram, strength of the neutron states, low-energy isoscalar strength functions for varying quadrupole deformation, deformation parameters. 250Cf; calculated deformation parameters. 249,251Cf; calculated single-quasiparticle neutron states. Finite amplitude quasiparticle random phase approximation method. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.044326
2021BH02 Phys.Rev. C 103, 024320 (2021) A.Bhagwat, M.Centelles, X.Vinas, P.Schuck Woods-Saxon type of mean-field potentials with effective mass derived from the D1S Gogny force NUCLEAR STRUCTURE 40Ca, 68Ni, 132Sn, 208Pb; calculated nucleon density distributions, neutron and proton mean fields for 132Sn and 208Pb, spin-orbit potentials and effective masses for 208Pb. 16O, 40,48Ca, 56,78Ni, 90Zr, 100,132Sn, 208Pb; calculated rms neutron and proton radii. Hartree-Fock, expectation value method (EVM), and ETF approaches, using D1S Gogny force.
doi: 10.1103/PhysRevC.103.024320
2021BH03 Phys.Rev. C 103, 024321 (2021) A.Bhagwat, M.Centelles, X.Vinas, P.Schuck Microscopic-macroscopic approach for ground-state energies based on the Gogny force with the Wigner-Kirkwood averaging scheme ATOMIC MASSES A=20-264, Z=10-108; calculated ground state energies of 551 spherical and deformed even-even nuclei. A=58-80, Z=30; A-114-148, Z=56; A=168-202, Z=78; A=196-216, Z=86; calculated binding energies; deduced differences from the evaluated data. 102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 146,148,150,152,154,156,158,160,162,164,166,168Dy, 180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated S(2n). 72Kr, 90,92,94Se, 98,100,102Ru, 124Xe, 186Pb; calculated potential-energy surfaces (PES) in (β, γ) plane. Wigner-Kirkwood Macroscopic-Microscopic model based on the Gogny D1S interaction, and by the Mic-Mac Gogny-based models. Comparison with evaluated data in AME-2012. Data for all the nuclei listed in the supplemental material of the article.
doi: 10.1103/PhysRevC.103.024321
2021LI57 Phys.Rev. C 104, 044330 (2021) Nuclear superfluidity at finite temperature NUCLEAR STRUCTURE 68Ni; calculated neutron pairing gap around the Fermi surface, temperature dependence of the pairing gaps. 44,46Ca, 68Ni; calculated pairing gaps for states around Fermi energy and the average pairing gaps as function of temperature; discussed effects of the dynamical kernel at finite temperature. Bardeen, Cooper, and Schrieffer (BCS), and BCS with particle-vibration coupling (PVC) calculations.
doi: 10.1103/PhysRevC.104.044330
2021LY02 Eur.Phys.J. A 57, 51 (2021) M.Lyu, Z.Ren, H.Horiuchi, B.Zhou, Y.Funaki, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Properties of 8-11Be sotopes with isospin-dependent spin-orbit potential in a cluster approach NUCLEAR STRUCTURE 8,9,10,11Be; calculated single nucleon wave functions, energy levels, J, π, one-neutron separation energies, root-mean-square radii and density distributions, spectroscopic factor. Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave functions.
doi: 10.1140/epja/s10050-021-00363-5
2021MI14 Phys.Rev. C 104, L031305 (2021) Symmetry projection to coupled-cluster singles plus doubles wave function through the Monte Carlo method
doi: 10.1103/PhysRevC.104.L031305
2020BA44 Phys.Atomic Nuclei 83, 212 (2020) E.B.Balbutsev, I.V.Molodtsova, P.Schuck Triplet of Nuclear Scissors Modes
doi: 10.1134/S1063778820020040
2020BA57 Phys.Rev. C 102, 061301 (2020) V.V.Baran, D.R.Nichita, D.Negrea, D.S.Delion, N.Sandulescu, P.Schuck Bridging the quartet and pair pictures of isovector proton-neutron pairing
doi: 10.1103/PhysRevC.102.061301
2020EB01 Phys.Rev. C 102, 014305 (2020) J.-P.Ebran, M.Girod, E.Khan, R.D.Lasseri, P.Schuck α-particle condensation: A nuclear quantum phase transition NUCLEAR STRUCTURE 16O; calculated binding energy as a function of deformation parameters β20, β30, β32, nucleon radial density for rms radii, neutron single particle levels, single-nucleon occupation numbers, Mott-like transition towards α-clusterized states using microscopic energy density functional (EDF) theory with the relativistic and the Gogny approaches. Discussed phase transition in nucleon density from Fermi gas to tetrahedral α-clustered configuration at critical density.
doi: 10.1103/PhysRevC.102.014305
2020JE05 Eur.Phys.J. A 56, 268 (2020) Symmetry conserving coupled cluster doubles wave function and the self-consistent odd particle number RPA
doi: 10.1140/epja/s10050-020-00276-9
2020LI36 Phys.Rev. C 102, 034310 (2020) Many-body correlations in nuclear superfluidity NUCLEAR STRUCTURE 44,46Ca, 66,68Ni, 112,114,116,120,124Sn; calculated state-dependent pairing gaps using static constant-gap approximation with a phenomenological kernel, and with dynamical particle-vibration coupling (PVC) effects. Discussed two-fermion two-time correlation function in the pairing channel within the equation of motion (EOM), in the form of Dyson Bethe-Salpeter equation.
doi: 10.1103/PhysRevC.102.034310
2020YA03 Phys.Rev. C 101, 024316 (2020) S.Yang, C.Xu, G.Ropke, P.Schuck, Z.Ren, Y.Funaki, H.Horiuchi, A.Tohsaki, T.Yamada, B.Zhou α decay to a doubly magic core in the quartetting wave function approach NUCLEAR STRUCTURE 102Sn, 102,104Te, 210Pb, 210,212Po; calculated single-particle wave functions of protons and neutrons in the quartet, effective potentials of the α cluster, normalized bound state wave functions, scattering wave functions for α-emitters, α-cluster preformation probabilities and α-decay half-lives. Microscopic calculation of α-cluster formation using the quartetting wave function approach. Comparison with experimental data. RADIOACTIVITY 102Sn, 102,104Te, 210Pb, 210,212Po(α); calculated α-cluster preformation probabilities and α-decay half-lives. Comparison with experimental half-lives.
doi: 10.1103/PhysRevC.101.024316
2019GU01 Phys.Rev. C 99, 014310 (2019) Medium-polarization effects in 3SD1 spin-triplet pairing
doi: 10.1103/PhysRevC.99.014310
2019JE02 Phys.Rev. C 100, 034311 (2019) Coupled self-consistent random-phase approximation equations for even and odd particle numbers: Tests with solvable models
doi: 10.1103/PhysRevC.100.034311
2019LI56 Phys.Rev. C 100, 064320 (2019), Erratum Phys.Rev. C 107, 029903 (2023) Toward an accurate strongly coupled many-body theory within the equation-of-motion framework NUCLEAR STRUCTURE 42,48Ca, 68Ni; calculated isoscalar dipole and giant dipole strength distributions, low-energy dipole E1 strength using relativistic quasiparticle random phase approximation (RQRPA), relativistic quasiparticle time blocking approximation (RQTBA), and equation of motion relativistic quasiparticle time blocking approximation (EOM/RQ-TBA3). Comparison with experimental data and with other theoretical models. Relevance to mechanisms of emergent collective phenomena, superfluidity and other dynamical aspects of strongly correlated many-body systems.
doi: 10.1103/PhysRevC.100.064320
2019SC16 Phys.Rev. C 100, 031301(R) (2019) Macroscopic manifestations of rotating triaxial superfluid nuclei NUCLEAR STRUCTURE 110Ru, 150Nd, 156Gd, 166,168Er, 172Yb, 182,184W, 186,188,190,192Os; calculated the three moments of inertia of triaxial superfluid nuclei from β and γ deformation parameters, pairing gaps for neutrons and protons from D1S Gogny force, and from nuclear masses using a five-point formula for triaxial nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.031301
2019SC22 Eur.Phys.J. A 55, 250 (2019) Mean-field theory for fermion pairs and the ab initio particle-vibration coupling approach
doi: 10.1140/epja/i2019-12798-x
2019TO07 Eur.Phys.J. A 55, 74 (2019) Truncation scheme of time-dependent density-matrix approach III
doi: 10.1140/epja/i2019-12746-x
2019ZH24 Phys.Rev. C 99, 051303 (2019) B.Zhou, Y.Funaki, H.Horiuchi, M.Kimura, Z.Ren, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Nonlocalized motion in a two-dimensional container of α particles in 3- and 4- states of 12C NUCLEAR STRUCTURE 12C; calculated level energies, Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave functions, energy curves and contours, and density profiles of the first 3- and 4- states in 12C using container model. Comparison with generator coordinate method (GCM).
doi: 10.1103/PhysRevC.99.051303
2019ZH33 Phys.Rev. C 100, 014306 (2019) Q.Zhao, Z.Ren, M.Lyu, H.Horiuchi, Y.Kanada-En'yo, Y.Funaki, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada, B.Zhou Investigation of isospin-triplet and isospin-singlet pairing in the A=10 nuclei 10B, 10Be, and 10C with an extension of the Tohsaki-Horiuchi-Schuck-Ropke wave function NUCLEAR STRUCTURE 10Be, 10B, 10C; calculated ground state energies, first 1+ energy in 10B, overlap between total wave function, molecular-orbit component, and pairing component, density distributions of valence nucleons, and average distance between nucleons, and optimized β parameters for the wave functions of ground states and first 1+ state in 10B. Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave function, with and without pairing effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014306
2018BA15 Phys.Rev. C 97, 044316 (2018) E.B.Balbutsev, I.V.Molodtsova, P.Schuck Experimental status of the nuclear spin scissors mode NUCLEAR STRUCTURE 232Th, 236,238U, 134Ba, 144,146,148,150Nd, 148,150,152,154Sm, 154,156,158,160Gd, 160,162,164Dy, 166,168,170Er, 172,174,176Yb, 176,178,180Hf, 182,184,186W, 190,192Os, 194,196Pt; calculated energy centroids, B(M1), nuclear spin and orbital scissors for 1+ states using Wigner function moments (WFM) method, and compared with experimental data. A=130-200; calculated (WFM) mean excitation energies and summed M1 strengths of scissors mode excitations, and compared with experimental data. NUCLEAR REACTIONS 232Th(d, d'), (d, p), E=12 MeV; 232Th(3He, 3He'), (3He, d), (3He, t), (3He, α), E=24 MeV; 238U(d, d'), (d, p), (d, t), E=15 MeV; compiled observed radiative strength functions (RSF) for scissors resonances by 2014Gu04. 232Th, 236,238U(γ, γ'), E=1.5-3.5 MeV; 134Ba, 144,146,148,150Nd, 148,150,152,154Sm, 154,156,158,160Gd, 160,162,164Dy, 166,168,170Er, 172,174,176Yb, 176,178,180Hf, 182,184,186W, 190,192Os, 194,196Pt(γ, γ'), E=2.0-4.0; compiled experimentally observed spectra of 1+ excitations and B(M1)(up) in various studies.
doi: 10.1103/PhysRevC.97.044316
2018BA48 Phys.Atomic Nuclei 81, 550 (2018) E.B.Balbutsev, I.V.Molodtsova, P.Schuck The Nuclear Spin Scissors Mode-Theory and Experiment
doi: 10.1134/S1063778818050034
2018ZH24 Phys.Rev. C 97, 054323 (2018) Q.Zhao, Z.Ren, M.Lyu, H.Horiuchi, Y.Funaki, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada, B.Zhou Investigation of the 9B nucleus and its cluster-nucleon correlations NUCLEAR STRUCTURE 9B; calculated levels, J, π, 3/2- rotational band levels, rms radii of six levels, density distributions of valence proton, energy of the 1/2+ excited state. New superposed Tohsaki-Horiuchi-Schuck-Ropke (THSR) wavefunction for cluster-correlated dynamics of valence nucleons. Comparison with experimental values and, with other theoretical predictions.
doi: 10.1103/PhysRevC.97.054323
2017BA03 Phys.Rev. C 95, 014318 (2017) M.Baldo, L.M.Robledo, P.Schuck, X.Vinas Barcelona-Catania-Paris-Madrid functional with a realistic effective mass NUCLEAR STRUCTURE Z=8-108, N=8-156; calculated binding energy differences of theoretical values computed with the HFB method and experimental values from AME-2012 for 620 even-even nuclei, rms charge deviations between experimental and theoretical values for the 315 even-even nuclei. 234U, 240,244Pu, 242,246Cm; calculated first and second fission barrier heights and the excitation energy of the fission isomers from Barcelona-Catania-Paris-Madrid (BCPM* and BCPM) functionals, and compared to experimental data. 90Zr, 106,110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 144Sm, 208Pb; calculated average excitation energy of the giant monopole resonance (GMR) and giant quadrupole resonance (GQR) including pairing correlations, and compared with experimental data. Proposed a variant of Barcelona-Catania-Paris-Madrid (BCPM) energy density functional, with bare mass replaced by a density dependent effective mass.
doi: 10.1103/PhysRevC.95.014318
2017TO10 Eur.Phys.J. A 53, 186 (2017) Truncation scheme of time-dependent density-matrix approach II
doi: 10.1140/epja/i2017-12377-3
2017XU03 Phys.Rev. C 95, 061306 (2017) C.Xu, G.Ropke, P.Schuck, Z.Ren, Y.Funaki, H.Horiuchi, A.Tohsaki, T.Yamada, B.Zhou a-cluster formation and decay in the quartetting wave function approach RADIOACTIVITY 190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 210Pb, 214Rn, 216Ra, 218Th, 260Sg, 264,268Hs, 270Ds, 286,288Fl, 290,292Lv, 294Og(α); calculated α-cluster preformation probabilities, comparison of experimental and theoretical half-lives. Microscopic calculations for α-cluster formation using quartetting wave function approach.
doi: 10.1103/PhysRevC.95.061306
2016LY03 Phys.Rev. C 93, 054308 (2016) M.Lyu, Z.Ren, B.Zhou, Y.Funaki, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Investigation of 10Be and its cluster dynamics with the nonlocalized clustering approach NUCLEAR STRUCTURE 10Be; calculated energies of the first two 0+ states, rms radii, rotational bands built on 0+ states, density distribution and correlations of two valence neutrons, dynamics of α clusters using Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.054308
2016SC21 Phys.Scr. 91, 123001 (2016) P.Schuck, Y.Funaki, H.Horiuchi, G.Ropke, A.Tohsaki, T.Yamada Alpha particle clusters and their condensation in nuclear systems
doi: 10.1088/0031-8949/91/12/123001
2016SC23 Eur.Phys.J. A 52, 307 (2016) Self-consistent RPA and the time-dependent density matrix approach
doi: 10.1140/epja/i2016-16307-7
2016XU01 Phys.Rev. C 93, 011306 (2016) C.Xu, Z.Ren, G.Ropke, P.Schuck, Y.Funaki, H.Horiuchi, A.Tohsaki, T.Yamada, B.Zhou α-decay width of 212Po from a quartetting wave function approach RADIOACTIVITY 212Po(α); calculated preformation probability and decay half-life using different sets of effective c.m. potentials and implementing four-nucleon correlations. Comparison of calculated α-decay width with experimental value.
doi: 10.1103/PhysRevC.93.011306
2016ZH15 Phys.Rev. C 93, 044329 (2016) S.S.Zhang, L.G.Cao, U.Lombardo, P.Schuck Medium polarization in asymmetric nuclear matter
doi: 10.1103/PhysRevC.93.044329
2015BA18 Phys.Rev. C 91, 064312 (2015) E.B.Balbutsev, I.V.Molodtsova, P.Schuck Orbital and spin scissors modes in superfluid nuclei NUCLEAR STRUCTURE 134Ba, 148,150Nd, 150,152,154Sm, 156,158,160Gd, 160,162,164Dy, 164,166,168,170Er, 172,174,176Yb, 178,180Hf, 182,184,186W, 190,192Os; calculated centroid energies and B(M1) of spin and orbital scissors. Wigner-function moments method generalized to include spin degrees of freedom and pair correlations simultaneously; deduced new phenomenon of opposite rotation of spin-up and spin-down nucleons, or the phenomenon of hidden angular momenta. Comparison with experimental values.
doi: 10.1103/PhysRevC.91.064312
2015LY01 Phys.Rev. C 91, 014313 (2015) M.Lyu, Z.Ren, B.Zhou, Y.Funaki, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Investigation of 9Be from a nonlocalized clustering concept NUCLEAR STRUCTURE 9Be; calculated levels, J, π, bands, contour maps of binding energy surface as function of β parameters, density distribution contour of the intrinsic ground state. Nonlocalized clustering calculations based on Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave function with a new phase factor. Comparison with available experimental results.
doi: 10.1103/PhysRevC.91.014313
2015PE17 Phys.Rev. C 92, 064316 (2015) J.C.Pei, N.Fei, Y.N.Zhang, P.Schuck Generalized second-order Thomas-Fermi method for superfluid Fermi systems NUCLEAR STRUCTURE 238U; calculated binding energies and neutron pairing density within a quasiparticle energy interval from 25 to 65 MeV by extending the second-order Thomas-Fermi approximation of the Hartree-Fock-Bogoliubov solutions for superfluid systems by including the effective mass and the spin-orbit potential.
doi: 10.1103/PhysRevC.92.064316
2015SC10 Rom.J.Phys. 60, 811 (2015) Theory for Quartet Condensation in Fermi Systems with Applications to Nuclear Matter NUCLEAR STRUCTURE 208Pb; calculated critical temperatures for α-particle and deuteron condensation in symmetric nuclear matter.
2015TO06 Phys.Rev. C 91, 034316 (2015) Extension of time-dependent Hartree-Fock-Bogoliubov equations NUCLEAR STRUCTURE 106,116,126Sn; calculated pairing energy as a function of an artificial factor f; deduced higher order effects of the pairing correlation. Extended time-dependent Hartree-Fock-Bogoliubov theory (ETDHFB) using a truncation scheme of the time-dependent density matrix theory.
doi: 10.1103/PhysRevC.91.034316
2015VI04 Phys.Scr. 90, 114001 (2015) X.Vinas, A.Bhagwat, M.Centelles, P.Schuck, R.Wyss Applications to nuclear properties of the microscopic-macroscopic model based on the semiclassical Wigner-Kirkwood method NUCLEAR STRUCTURE Zn, Ba, Pt, Rn; calculated 2 neutron separation energies. Comparison with experimental data. RADIOACTIVITY 112,114,116Te, 116,118,120,122,124Ba, 114,116,118,120Xe, No, Rf, Sg, Hs, Ds(α); calculated Q-value, T1/2. Comparison with experimental data.
doi: 10.1088/0031-8949/90/11/114001
2014RO20 Phys.Rev. C 90, 034304 (2014) G.Ropke, P.Schuck, Y.Funaki, H.Horiuchi, Z.Ren, A.Tohsaki, C.Xu, T.Yamada, B.Zhou Nuclear clusters bound to doubly magic nuclei: The case of 212Po NUCLEAR STRUCTURE 212Po; calculated internal four-nucleon energy, Coulomb and isospin-dependent Woods-Saxon potentials, Thomas-Fermi density, Fermi energy, E(α). Shell model calculations with cluster formation in inhomogeneous nuclear systems, four-particle (α-like) correlations in doubly-magic 208Pb core. Tohsaki-Horiuchi-Schuck-Ropke wave function approach in shell-model calculations. Discussed different physics behavior of an α-like cluster as compared to a deuteron-like cluster.
doi: 10.1103/PhysRevC.90.034304
2014TO06 Eur.Phys.J. A 50, 77 (2014) Truncation scheme of time-dependent density-matrix approach
doi: 10.1140/epja/i2014-14077-x
2014ZH10 Phys.Rev. C 89, 034319 (2014) B.Zhou, Y.Funaki, H.Horiuchi, Z.Ren, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Nonlocalized cluster dynamics and nuclear molecular structure NUCLEAR STRUCTURE 8Be, 12C, 20Ne; calculated levels, J, π, energy surfaces, density distributions, quadrupole moments using Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave function. Container model. Nonlocalized cluster dynamics for 2α, 3α, and 16O+α cluster systems.
doi: 10.1103/PhysRevC.89.034319
2013BA33 Phys.Rev. C 87, 064305 (2013) M.Baldo, L.M.Robledo, P.Schuck, X.Vinas New Kohn-Sham density functional based on microscopic nuclear and neutron matter equations of state NUCLEAR STRUCTURE Z=8-116, N=4-154; calculated binding energies; analyzed differences between the calculated and experimental values from AME-2003 for 579 nuclei; deduced energy rms value. N=4-154; calculated rms charge radii for even-even nuclei and compared with evaluated experimental values. Quadrupole and octupole deformations calculated for 818 nuclei. 240Pu, 262Sg; calculated spontaneous fission barrier heights, SF half-lives, quadrupole, octupole and hexadecapole moments. Comparison with experimental data. 90Zr, 144Sm, 208Pb, 106,110,112,114,116Cd, 112,114,116,118,120,122,124Sn; calculated energies of isoscalar giant monopole and quadrupole (ISGMR, ISGQR) resonances with and without pairing. Comparison with experimental data. A new version of Barcelona-Catania-Paris energy functional based on calculated ab initio nuclear and neutron matter equations of state. Comparison with other mean-field theories.
doi: 10.1103/PhysRevC.87.064305
2013BA36 Phys.Rev. C 88, 014306 (2013) E.B.Balbutsev, I.V.Molodtsova, P.Schuck New type of nuclear collective motion: The spin scissors mode NUCLEAR STRUCTURE 164Er; calculated isovector and isoscalar energies B(M1), B(E2) using the Wigner function moments method on the basis of time-dependent Hartree-Fock equations. Spin-spin interaction. Spin scissors excitation mode.
doi: 10.1103/PhysRevC.88.014306
2013GI05 Phys.Rev.Lett. 111, 132503 (2013) α-Particle Clustering from Expanding Self-Conjugate Nuclei within the Hartree-Fock-Bogoliubov Approach NUCLEAR STRUCTURE 16O, 24Mg, 32S, 40Ca; calculated total energy as a function of the radius, threshold energies as a function of the number n of α particles; deduced nuclear equation of state implications. HFB approach for self-conjugate nuclei.
doi: 10.1103/PhysRevLett.111.132503
2013JE05 Phys.Rev. C 88, 044004 (2013) Self-consistent random-phase approximation from a coupled-cluster wave function perspective
doi: 10.1103/PhysRevC.88.044004
2013PA25 Phys.Rev. C 88, 034314 (2013) A.Pastore, J.Margueron, P.Schuck, X.Vinas Pairing in exotic neutron-rich nuclei near the drip line and in the crust of neutron stars NUCLEAR STRUCTURE Z=20, A=36-120; Z=28, A=52-128; Z=40, A=80-240; Z=42, A=82-162; Z=50, A=100-250; Z=82, A=178-342; 66,68,70Ca; 122,124,126,128,130,166,250,500Zr; calculated pairing energies, neutron pairing gaps, single-particle energies and other properties for neutron drip line nuclei immersed in low-density gas of neutrons in outer crust of neutron stars. Skyrme energy density functional theory with density-dependent contact interaction, and Gogny finite range pairing functionals interactions. Hartree-Fock-Bogoliubov and BCS approaches compared. Strong impact of resonances in the continuum on pairing properties of drip line nuclei.
doi: 10.1103/PhysRevC.88.034314
2013TO06 Phys.Rev. C 87, 044316 (2013) Odd particle number random-phase approximation and extensions: Applications to particle and hole states around 16O NUCLEAR STRUCTURE 15N, 17F; calculated proton-hole and proton-particle state spectral functions S(E), spectroscopic factors, strength distributions using the hole-state and the particle-state random-phase approximation with a 16O core. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.044316
2013ZH25 Phys.Rev.Lett. 110, 262501 (2013) B.Zhou, Y.Funaki, H.Horiuchi, Z.Ren, G.Ropke, P.Schuck, A.Tohsaki, C.Xu, T.Yamada Nonlocalized Clustering: A New Concept in Nuclear Cluster Structure Physics NUCLEAR STRUCTURE 20Ne; calculated energy surfaces, levels, J, π. The Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave function, α+16O resonating group method.
doi: 10.1103/PhysRevLett.110.262501
2012BH10 Phys.Rev. C 86, 044316 (2012) A.Bhagwat, X.Vinas, M.Centelles, P.Schuck, R.Wyss Microscopic-macroscopic approach for binding energies with the Wigner-Kirkwood method. II. Deformed nuclei NUCLEAR STRUCTURE 63Ge, 65As, 67Se, 71,80,82,84,86,88,90,92,94,96,98,100,102,104Kr, 76,78,80,82,84,86,88,90,92,94,96,98,100,102Sr, 84,86,88,90,92,94,96,98,100,102,104,106,108Zr, 86,88,90,92,94,96,98,100,102,104,106,108,110Mo, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 140,142,144,146,148,150,152,154,156,158,160,162Gd, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Po; calculated S2n, β2, Sp, binding energy using Microscopic-macroscopic model with Wigner-Kirkwood expansion. Comparison with experimental data. Z, N>7; deduced difference between the calculated and the corresponding experimental binding energies for 561 nuclides. RADIOACTIVITY 279,280Rg, 282,283Nh, 287,288,289Fl, 287,288Mc, 291,292,293Lv, 294Og(α); calculated Q values and half-lives. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044316
2012DE10 Phys.Rev. C 85, 064306 (2012) D.S.Delion, R.J.Liotta, P.Schuck, A.Astier, M.-G.Porquet Shell model plus cluster description of negative parity states in 212Po NUCLEAR STRUCTURE 212Po; calculated negative-parity levels, J, π, B(E1), B(E2), octupole TDA amplitudes, α-decay widths. 208,210Pb, 210Po; calculated interaction energies, B(E2). Shell-model with α cluster approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.064306
2012FU10 Prog.Theor.Phys.(Kyoto), Suppl. 196, 439 (2012) Y.Funaki, T.Yamada, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki Alpha Cluster States and Condensation in 16O NUCLEAR STRUCTURE 16O, 12C, 20Ne; calculated energy spectra, J, π, rotational band of the α+Hoyle state. Orthogonality condition model and Gauss expansion method calculations.
doi: 10.1143/PTPS.196.439
2012SC14 Prog.Theor.Phys.(Kyoto), Suppl. 196, 56 (2012) Quartetting in Nuclear Matter
doi: 10.1143/PTPS.196.56
2012YA02 Phys.Rev. C 85, 034315 (2012) T.Yamada, Y.Funaki, T.Myo, H.Horiuchi, K.Ikeda, G.Ropke, P.Schuck, A.Tohsaki Isoscalar monopole excitations in 16O: α-cluster states at low energy and mean-field-type states at higher energy NUCLEAR STRUCTURE 16O; calculated energies of 0+ levels, rms charge radii, E0 transition matrix elements, particle decay widths, spectroscopic factors, isoscalar monopole strength functions using four α cluster model and α+12C orthogonality condition model (OCM) model. Discussed dual nature of 16O ground state. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034315
2012ZH29 Phys.Rev. C 86, 014301 (2012) B.Zhou, Z.-z.Ren, C.Xu, Y.Funaki, T.Yamada, A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke New concept for the ground-state band in 20Ne within a microscopic cluster model NUCLEAR STRUCTURE 20Ne; calculated energy surface contour maps of ground-state and first 2+ states, wave function overlaps, minimum energies and distances between α cluster and 16O cluster with respect to different spin-projected states for the ground-state band members up to 8+. Brink microscopic cluster model based on generalized Tohsaki, Horiuchi, Schuck, Ropke (THSR) wave functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.014301
2011AS06 Int.J.Mod.Phys. E20, 785 (2011) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Pure α-208Pb states in 212Po revealed by their enhanced E1 decays, A novel α clustering NUCLEAR REACTIONS 208Pb(18O, 14C)212Po, E=85 MeV; measured reaction products, Eγ, Iγ, γ-γ-γ-coin.; deduced energies, states, J, π, yrast states, B(E1), α-208Pb states.
doi: 10.1142/S0218301311018678
2011AS09 J.Phys.:Conf.Ser. 312, 092014 (2011) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck A novel manifestation of α clustering in 212Po: Pure α-208Pb states revealed by their enhanced E1 decays NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured Eγ, Iγ(θ), γγ-coin using Eurobal array of Ge crystals. 212Po deduced γ yrast transitions angular distribution, T1/2 using Doppler shift, B(E1), α-core.
doi: 10.1088/1742-6596/312/9/092014
2011BA42 Nucl.Phys. A872, 42 (2011) E.B.Balbutsev, I.V.Molodtsova, P.Schuck Spin scissors mode and the fine structure of M1 states in nuclei NUCLEAR STRUCTURE 164Er; calculated B(M1), B(E2), energies of states, giant quadrupole resonances, quantum numbers of excited states using coupled dynamics; deduced spin-orbit interaction constant ETA for scissors mode and IVGQR.
doi: 10.1016/j.nuclphysa.2011.09.013
2011BA44 Phys.Atomic Nuclei 74, 1651 (2011) E.B.Balbutsev, L.A.Malov, P.Schuck Spatial dependence of pairing in deformed nuclei NUCLEAR STRUCTURE 134Ba, 174Yb; calculated pairing gaps, coherence lengths. Time-dependent HFB equations.
doi: 10.1134/S1063778811110020
2011FU08 Int.J.Mod.Phys. E20, 874 (2011) Y.Funaki, T.Yamada, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki Alpha clustering and condensation in nuclei NUCLEAR STRUCTURE 16O; calculated energy levels, J, π, rms radii, occupation of the single-α orbitals. OCM and THSR calculations, comparison with experimental data.
doi: 10.1142/S0218301311018873
2011RO50 Phys.Rev. C 84, 054309 (2011); Erratum Phys.Rev. C 93, 069905 (2016) X.Roca-Maza, X.Vinas, M.Centelles, P.Ring, P.Schuck Relativistic mean-field interaction with density-dependent meson-nucleon vertices based on microscopical calculations NUCLEAR STRUCTURE 16,18,26,28,30Ne, 20,32Mg, 34,36Si, 36S, 38,40Ar, 36,38,40,42,44,46,48,50,52Ca, 40,42,44,48,50,52,54Ti, 46,52Cr, 54,64,66,68Fe, 54,56,58,66,68,70,72Ni, 58,70,72Zn, 82Ge, 84,86Se, 86,88Kr, 86,88,90Sr, 86,88,90,92Zr, 86,88,90,92,94Mo, 94,96Ru, 96,98Pd, 98,100Cd, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 126,128,130,132,134,136Te, 134,136,138Xe, 136,138,140Ba, 138,140,142,144Ce, 140,142,144Nd, 142,144,146Sm, 146Gd, 148Dy, 150Er, 152Yb, 170,172Pt, 172,174,176,204,206Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 204,206,208,210,212,214,216Po, 208,210,212,214,216Rn, 210,212,214,216,218Ra, 212,214,216,218,220Th, 224U; analyzed binding energies, and charge radii. 100,132,176Sn; calculated isoscalar, isovector parts of the spin-orbit potential, spin orbit splitting. Relativistic Brueckner theory, high-precision density functional DD-MEδ with density-dependent meson-nucleon couplings. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.054309
2011SC14 Int.J.Mod.Phys. E20, 889 (2011) Critical temperature for α-condensation in asymmetric nuclear matter: The astrophysical context
doi: 10.1142/S0218301311018903
2011VI01 Int.J.Mod.Phys. E20, 399 (2011) Semiclassical description of average pairing properties in nuclei NUCLEAR STRUCTURE 116Sn; calculated level density, neutron effective mass, pairing gap.
doi: 10.1142/S0218301311017788
2010AS01 Phys.Rev.Lett. 104, 042701 (2010) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Novel Manifestation of α-Clustering Structures: New "α+ 208Pb" States in 212Po Revealed by Their Enhanced E1 Decays NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured Eγ, Iγ; deduced 212Po level scheme, yrast state, lifetimes, B(E1). Doppler-shift attenuation method.
doi: 10.1103/PhysRevLett.104.042701
2010AS03 Eur.Phys.J. A 46, 165 (2010) A.Astier, P.Petkov, M.-G.Porquet, D.S.Delion, P.Schuck Coexistence of "a + 208Pb" cluster structures and single-particle excitations in 21284Po128 NUCLEAR REACTIONS 208Pb(18O, 14C), E=85 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin. 212Po; deduced level scheme, transition energies, γ-ray intensities, J, π, angular-distribution coefficients, internal conversion coefficients, yrast states, lifetimes, B(E1), B(E2), B(E3). EUROBALL project, DSAM method, comparison with low-lying cluster structure models. RADIOACTIVITY 212Po(α); measured decay products, Eγ, Iγ, alpha spectrum; deduced branching ratios, partial T1/2 for yrast states.
doi: 10.1140/epja/i2010-11053-6
2010BH05 Phys.Rev. C 81, 044321 (2010) A.Bhagwat, X.Vinas, M.Centelles, P.Schuck, R.Wyss Microscopic-macroscopic approach for binding energies with the Wigner-Kirkwood method NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated coulomb potential, Wigner-Kirkwood energies and ground state energies as function of quadrupole deformation. 136,138,140,142,144,146,148,150,152,154,156Gd, 138,140,142,144,146,148,150,152,154,156,158Dy, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated Strutinsky shell corrections. 38,40,42,44,46,48,50,52Ca, 40,42,44,46,48,50,52Sc, 40,42,44,46,48,50,52,54Ti, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated binding energies, one-neutron and two-neutron separation energies. A=40-152, A=18-220; calculated binding energies for a set of 367 spherical nuclei. Classical Wigner-Kirkwood expansion method for spherical and deformed nuclei. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044321
2010BH06 Int.J.Mod.Phys. E19, 747 (2010) A.Bhagwat, X.Vinas, R.Wyss, P.Schuck Wigner-Kirkwood method for microscopic-macroscopic calculation of binding energies NUCLEAR STRUCTURE 188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 134,136,138,140,142,144,146,148,150,152,154,156,158Dy; calculated Coulomb potential, deformation parameters, shell corrections, binding energies.
doi: 10.1142/S0218301310015187
2010FU06 Phys.Rev. C 82, 024312 (2010) Y.Funaki, T.Yamada, A.Tohsaki, H.Horiuchi, G.Ropke, P.Schuck Microscopic study of 4α-particle condensation with inclusion of resonances NUCLEAR STRUCTURE 16O; calculated binding energies, energy spectra, rms radii, monopole M(E0) matrix elements, α-decay widths, nucleon density distributions, occupation probabilities, and momentum distributions of four 0+ states in 4α-particle condensate using Tohsaki-Horiuchi- Schuck-Ropke (THSR) wave function. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.024312
2010HA10 J.Phys.(London) G37, 064040 (2010) Cooper pair sizes in 11Li and in superfluid nuclei: a puzzle? NUCLEAR STRUCTURE 11Li, 18O; calculated neutron Cooper pairs, two-particle densities and wavefunctions, radii.
doi: 10.1088/0954-3899/37/6/064040
2010JI10 Phys.Rev. C 82, 024911 (2010) BEC-BCS crossover and the liquid-gas phase transition in hot and dense nuclear matter
doi: 10.1103/PhysRevC.82.024911
2010PI02 Phys.Rev. C 81, 034307 (2010) N.Pillet, N.Sandulescu, P.Schuck, J.-F.Berger Two-particle spatial correlations in superfluid nuclei NUCLEAR STRUCTURE 102Sr, 152Sm, 238U; calculated local and nonlocal parts of the pairing tensor, and coherence lengths. 60Ni, 120,136Sn, 212Pb; calculated pairing correlation energies and average pairing fields, and coherence lengths. Effect of pairing on two-neutron spatial correlations in deformed nuclei. Hartree-Fock Bogoliubov calculations with D1S Gogny force.
doi: 10.1103/PhysRevC.81.034307
2010RO08 Phys.Rev. C 81, 034315 (2010) L.M.Robledo, M.Baldo, P.Schuck, X.Vinas Octupole deformation properties of the Barcelona-Catania-Paris energy density functionals NUCLEAR STRUCTURE 216,218,220,222,224,226,228,230,232Ra, 140,142,144,146,148,150Ba; calculated HFB mean-field energies and octupole collective inertial parameters as function of octupole moment, particle-particle correlation energies, B(E1) and B(E3) probabilities, and dipole moments. 144Ba, 224Ra; calculated single-particle neutron and proton energies with energy density functional and the Gogny D1S force as function of quadrupole and octupole moments. 240Pu; calculated mean-field energy, octupole and hexadecapole moments as function of axial quadrupole moment. Hartree-Fock-Bogoliubov approximation calculations for octupole deformation properties of the Barcelona-Catania-Paris (BCP) energy density functionals.
doi: 10.1103/PhysRevC.81.034315
2010SO11 Phys.Rev. C 81, 064310 (2010) Many-body approach for quartet condensation in strong coupling
doi: 10.1103/PhysRevC.81.064310
2010SO17 Phys.Rev. C 82, 034322 (2010) Critical temperature for α-particle condensation in asymmetric nuclear matter
doi: 10.1103/PhysRevC.82.034322
2010TO15 Eur.Phys.J. A 45, 257 (2010) Density-matrix formalism with three-body ground-state correlations
doi: 10.1140/epja/i2010-11002-5
2010VI05 Phys.Rev. C 82, 034314 (2010) X.Vinas, P.Schuck, and N.Pillet Cooper pair sizes in superfluid nuclei in a simplified model NUCLEAR STRUCTURE A=1-320; calculated pairing gap at the Fermi energy using the Gogny D1S force. A=12, 28, 120, 8000 120Sn; calculated coherence lengths as a function of the radial distance, and density matrices; evaluated Cooper pair sizes in a simple harmonic oscillator model.
doi: 10.1103/PhysRevC.82.034314
2009CA34 Chin.Phys.C 33, Supplement 1, 33 (2009) L.-G.Cao, U.Lombardo, P.Schuck Superfluid nuclear matter in BCS theory and beyond
doi: 10.1088/1674-1137/33/S1/011
2009FU14 Int.J.Mod.Phys. E18, 2083 (2009) Y.Funaki, T.Yamada, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki α-particle condensed state in 16O NUCLEAR STRUCTURE 16O; calculated energy spectra, J, π, rms radii, monopole transition matrix elements, single-α orbits.
doi: 10.1142/S0218301309014330
2009FU16 Phys.Rev. C 80, 064326 (2009) Y.Funaki, H.Horiuchi, W.von Oertzen, G.Ropke, P.Schuck, A.Tohsaki, T.Yamada Concepts of nuclear α-particle condensation NUCLEAR STRUCTURE 12C, 16O; calculated occupation of single-α orbitals, binding energies, and momentum distribution of Hoyle states in 12C and 16O using antisymmetrized α-particle product state wave functions or THSR (Tohsaki-Horiuchi-Schuck-Roepke) α-cluster wave functions. Discussed α-cluster phenomenon in connection with experimental αγ-coin spectra for 24Mg(28Si, 3α)40Ca and 24Mg(28Si, 12C)40Ca reactions.
doi: 10.1103/PhysRevC.80.064326
2009HA37 Int.J.Mod.Phys. E18, 2045 (2009) Di-neutron correlation in light neutron-rich nuclei NUCLEAR STRUCTURE 11Li, 8He; analyzed root mean square distance between the two valence neutrons in 11Li, di-neutron structure in 8He.
doi: 10.1142/S0218301309014263
2009KA17 Phys.Rev. C 79, 054305 (2009) Y.Kanada-Enyo, N.Hinohara, T.Suhara, P.Schuck Dineutron correlations in quasi-two-dimensional systems in a simplified model, and possible relation to neutron-rich nuclei
doi: 10.1103/PhysRevC.79.054305
2009SO06 Phys.Rev. C 79, 051301 (2009) T.Sogo, R.Lazauskas, G.Ropke, P.Schuck Critical temperature for α-particle condensation within a momentum-projected mean-field approach
doi: 10.1103/PhysRevC.79.051301
2009VI04 Int.J.Mod.Phys. E18, 935 (2009) X.Vinas, L.M.Robledo, M.Baldo, P.Schuck Deformed nuclei using the Barcelona-Catania-Paris energy density functional
doi: 10.1142/S0218301309013075
2009YA05 Phys.Rev. C 79, 054314 (2009) T.Yamada, Y.Funaki, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki Internal one-particle density matrix for Bose-Einstein condensates with finite number of particles in a harmonic potential
doi: 10.1103/PhysRevC.79.054314
2008FU06 Phys.Rev. C 77, 064312 (2008) Y.Funaki, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki, T.Yamada Density-induced suppression of the α-particle condensate in nuclear matter and the structure of α-cluster states in nuclei NUCLEAR STRUCTURE 12C, 16O; calculated condensation fraction for alpha-matter and its dependence on baryon density. Jastrow-Feenberg approach.
doi: 10.1103/PhysRevC.77.064312
2008FU11 Phys.Rev.Lett. 101, 082502 (2008) Y.Funaki, T.Yamada, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki α-Particle Condensation in 16O Studied with a Full Four-Body Orthogonality Condition Model Calculation NUCLEAR STRUCTURE 16O; calculated energy and rms radii of ground and excited 0+ states and monopole transition matrix elements, M(E0) to ground state; comparison with experiments; semi-microscopic cluster model.
doi: 10.1103/PhysRevLett.101.082502
2008FU14 Int.J.Mod.Phys. E17, 2087 (2008) Y.Funaki, T.Yamada, H.Horiuchi, G.Ropke, P.Schuck, A.Tohsaki Present status of alpha-particle condensate states in self-conjugate 4n nuclei NUCLEAR STRUCTURE 12C, 16O; calculated low density states near the 3α and 4α breakup threshold, energy levels, J, π. OCM and THSR approaches.
doi: 10.1142/S0218301308011148
2008MA20 Phys.Rev. C 77, 064306 (2008) J.Margueron, J.Navarro, Nguyen Van Giai, P.Schuck Continued fraction approximation for the nuclear matter response function
doi: 10.1103/PhysRevC.77.064306
2008RO11 Phys.Rev. C 77, 051301 (2008) L.M.Robledo, M.Baldo, P.Schuck, X.Vinas Deformation properties of the Barcelona-Catania-Paris (BCP) energy density functional NUCLEAR STRUCTURE 26,32,38Mg, 144,154,160,164Dy, 218,228,236Ra, 240Pu; calculated potential energy surfaces, neutron separation energies, deformation energies; deduced levels, configurations. Barcelona-Catania-Paris (BCP) energy density functions. 240Pu; calculated fission barrier. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.051301
2008SC21 Int.J.Mod.Phys. E17, 2136 (2008) Formulation of alpha-particle condensation in the macroscopic limit
doi: 10.1142/S0218301308011227
2008TO09 Eur.Phys.J. A 36, 349 (2008) Extended random-phase approximation with three-body ground-state correlations
doi: 10.1140/epja/i2008-10596-3
2007BA03 Ann.Phys.(New York) 322, 489 (2007) The nuclear scissors mode from various aspects
doi: 10.1016/j.aop.2006.04.014
2007CE01 Ann.Phys.(New York) 322, 363 (2007) M.Centelles, P.Schuck, X.Vinas Thomas-Fermi theory for atomic nuclei revisited NUCLEAR STRUCTURE A=8-200; calculated binding energies, shell correction energies. Semiclassical approach, Thomas-Fermi theory, Wigner-Kirkwood expansion.
doi: 10.1002/andp.2006.07.009
2007HA21 Phys.Rev.Lett. 99, 022506 (2007) K.Hagino, H.Sagawa, J.Carbonell, P.Schuck Coexistence of BCS- and BEC-Like Pair Structures in Halo Nuclei
doi: 10.1103/PhysRevLett.99.022506
2007PI11 Phys.Rev. C 76, 024310 (2007) N.Pillet, N.Sandulescu, P.Schuck Generic strong coupling behavior of Cooper pairs on the surface of superfluid nuclei
doi: 10.1103/PhysRevC.76.024310
2007SC21 Prog.Part.Nucl.Phys. 59, 285 (2007) P.Schuck, Y.Funaki, H.Horiuchi, G.Ropke, A.Tohsaki, T.Yamada Quartetting in fermionic matter and α-particle condensation in nuclear systems
doi: 10.1016/j.ppnp.2006.12.003
2007SC38 Nucl.Phys. A788, 293c (2007) P.Schuck, Y.Funaki, H.Horiuchi, G.Ropke, A.Tohsaki, T.Yamada α-Particle Condensation in Nuclear Systems NUCLEAR STRUCTURE 12C; calculated binding energy, radii, monopole matrix elements and inelastic form factor. 16O; calculated 0+ state energies. Hoyle state discussed.
doi: 10.1016/j.nuclphysa.2007.01.015
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