NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = A.Tohsaki Found 62 matches. 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
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
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
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
2018IT02 Phys.Rev. C 97, 014304 (2018) Improved version of a simplified method for including tensor effects in cluster models NUCLEAR STRUCTURE 4He; calculated energy convergence for the ground state, energies of the (0s)4 configuration, amplitude for the linear combination of basis states, expectation values of principal quantum number, one-body spin-orbit operator, and the component of (0s)4 configuration. 16O; calculated energy curve for 0+ state with a tetrahedral configuration of four-α clusters, and expectation value of the one-body spin-orbit operator, principal quantum number of harmonic oscillator, and squared overlap between the result of iSMT and tetrahedron configuration of four α clusters as a function of the α-α distance. Conventional cluster model with tensor contribution (SMT), and improved SMT (iSMT).
doi: 10.1103/PhysRevC.97.014304
2018IT03 Phys.Rev. C 97, 014307 (2018) Nontrivial origin for the large nuclear radii of dripline oxygen isotopes NUCLEAR STRUCTURE 16O, 22,24O; calculated principal quantum number, expectation values of one-body spin-orbit operator and rms radii for 22,24O, energies of 0+ states for 16O, 22,24O, size parameter dependence for the 0+ energy of 24O as function of α-α distance for the four α clusters. Cluster model.
doi: 10.1103/PhysRevC.97.014307
2018IT07 Phys.Rev. C 98, 044306 (2018) N.Itagaki, H.Matsuno, A.Tohsaki Explicit inclusion of the spin-orbit contribution in the Tohsaki-Horiuchi-Schuck-Ropke wave function NUCLEAR STRUCTURE 12C; calculated energy of the 0+ state, rms matter radius, energy curve for 0+ state, spin-orbit energy, contribution of the three-body interaction terms, and the elastic form factor versus momentum transfer of the 0+ state using Monte Carlo Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave functions combined with antisymmetrized quasi-cluster model (AQCM). Comparison with experimental values.
doi: 10.1103/PhysRevC.98.044306
2018TO01 Phys.Rev. C 97, 011301 (2018) α clustering with a hollow structure: Geometrical structure of α clusters from platonic solids to fullerene shape NUCLEAR STRUCTURE 16O, 24Mg, 32S, 48Cr, 56Ni, 80Zr, 128Gd, 240120; calculated α-cluster structures based on the geometric configurations and fullerene-shaped polyhedrons with microscopic α-cluster models.
doi: 10.1103/PhysRevC.97.011301
2018TO05 Phys.Rev. C 98, 014302 (2018) Coulomb energy of α-particle aggregates distributed on Archimedean solids NUCLEAR STRUCTURE A=120-162, Z=60; A=128-173, Z=64; A=168-227, Z=84; A=240-324, Z=120; calculated Coulomb energy for one α cluster in Archimedean solids within a microscopic framework. Discussed geometric configurations.
doi: 10.1103/PhysRevC.98.014302
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
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
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
2016ZH43 Phys.Rev. C 94, 044319 (2016) B.Zhou, A.Tohsaki, H.Horiuchi, Z.Ren Breathing-like excited state of the Hoyle state in 12C NUCLEAR STRUCTURE 12C; calculated energies of the first four 0+ states, rms radii for the mass distributions, monopole transition strengths, contour plot for the third 0+ state in the spherical β1 and β2 parameter space, α reduced width amplitudes of four 0+ states; deduced third 0+ state as a breathing-like excited state of the Hoyle state, and the fourth 0+ state as a bent-arm 3α structure. Generator coordinate method (GCM), and optimized 2α+α Tohsaki-Horiuchi-Schuck-Ropke (THSR) wave functions.
doi: 10.1103/PhysRevC.94.044319
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
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
2014su04 Phys.Rev.Lett. 112, 062501 (2014) T.Suhara, Y.Funaki, B.Zhou, H.Horiuchi, A.Tohsaki One-Dimensional α Condensation of α-Linear-Chain States in 12C and 16O NUCLEAR STRUCTURE 12C, 16O; calculated energy curves for excited states, α linear chain wave functions, α clusters. Brink and Tohsaki-Horiuchi-Schuck-Ropke wave functions.
doi: 10.1103/PhysRevLett.112.062501
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
2014ZH33 Prog.Theor.Exp.Phys. 2014, 101D01 (2014) B.Zhou, Y.Funaki, A.Tohsaki, H.Horiuchi, Z.Ren The container picture with two-alpha correlation for the ground state of 12C NUCLEAR STRUCTURE 12C; calculated ground state energies, energy surfaces. THSR (Tohsaki-Horiuchi-Schuck-Ropke) wavefunctions.
doi: 10.1093/ptep/ptu127
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
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
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
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
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
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
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
2008TO18 Int.J.Mod.Phys. E17, 2106 (2008) The interaction of a nucleon and alpha condensate NUCLEAR STRUCTURE 13C; calculated energy curves for a neutron and 3α-clusters. THSR wave function.
doi: 10.1142/S0218301308011173
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
2007WA32 Phys.Lett. B 653, 173 (2007) T.Wakasa, E.Ihara, K.Fujita, Y.Funaki, K.Hatanaka, H.Horiuchi, M.Itoh, J.Kamiya, G.Ropke, H.Sakaguchi, N.Sakamoto, Y.Sakemi, P.Schuck, Y.Shimizu, M.Takashina, S.Terashima, A.Tohsaki, M.Uchida, H.P.Yoshida, M.Yosoi New candidate for an alpha cluster condensed state in 16O(α, α') at 400 MeV NUCLEAR REACTIONS 16O(α, α'), E=400 MeV; analyzed elastic and inelastic σ(θ). Comparison with model calculations. Evidence for cluster structure.
doi: 10.1016/j.physletb.2007.08.016
2006FU02 Prog.Theor.Phys.(Kyoto) 115, 115 (2006) Y.Funaki, H.Horiuchi, A.Tohsaki New Treatment of Resonances with a Bound State Approximation Using a Pseudo-Potential NUCLEAR STRUCTURE 12C; calculated wave function, resonance parameters for second 2+ state. Analytic continuation in the coupling constant.
doi: 10.1143/PTP.115.115
2006FU09 Eur.Phys.J. A 28, 259 (2006) Y.Funaki, A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke Inelastic form factors to alpha-particle condensate states in 12C and 16O: What can we learn? NUCLEAR STRUCTURE 12C, 16O; calculated inelastic and elastic form factors, α-cluster states energies, related features. Hoyle state discussed, comparison with data.
doi: 10.1140/epja/i2006-10061-5
2006MA72 Phys.Rev. C 74, 044311 (2006) J.A.Maruhn, M.Kimura, S.Schramm, P.-G.Reinhard, H.Horiuchi, A.Tohsaki α-cluster structure and exotic states in a self-consistent model for light nuclei NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated binding energies, deformation, cluster configurations. 28Si, 32S, 36Ar, 40Ca; calculated superdeformed states features.
doi: 10.1103/PhysRevC.74.044311
2005FU02 Eur.Phys.J. A 24, 321 (2005) Y.Funaki, A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke Resonance states in 12C and α-particle condensation NUCLEAR STRUCTURE 12C; calculated resonance levels J, π, α-decay widths, α-cluster structure. Analytic continuation in the coupling constant.
doi: 10.1140/epja/i2004-10238-x
2004SC27 Nucl.Phys. A738, 94 (2004) P.Schuck, Y.Funaki, H.Horiuchi, G.Ropke, A.Tohsaki, T.Yamada Alpha-particle condensation in nuclei NUCLEAR STRUCTURE 12C; calculated α-cluster states energies, radii. Other nuclides discussed.
doi: 10.1016/j.nuclphysa.2004.04.075
2004TA07 Phys.Rev. C 69, 035802 (2004) H.Takemoto, M.Fukushima, S.Chiba, H.Horiuchi, Y.Akaishi, A.Tohsaki Clustering phenomena in nuclear matter below the saturation density
doi: 10.1103/PhysRevC.69.035802
2004TA20 Nucl.Phys. A738, 278 (2004) Dimensional dependency of Coulomb energy in an infinite aggregate with periodicity neutralized by a uniform background
doi: 10.1016/j.nuclphysa.2004.04.045
2004TO15 Nucl.Phys. A738, 259 (2004) A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke Wide perspective of alpha condensation in light 4N Nuclei NUCLEAR STRUCTURE 8Be, 12C, 16O, 20Ne; calculated α-cluster states energies, radii, α condensation features.
doi: 10.1016/j.nuclphysa.2004.04.042
2003FU06 Phys.Rev. C 67, 051306 (2003) Y.Funaki, A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke Analysis of previous microscopic calculations for the second 0+ state in 12C in terms of 3-α particle Bose-condensed state NUCLEAR STRUCTURE 12C; calculated 0+ state wave function, radius, related features. Comparison of microscopic cluster model and condensed state results.
doi: 10.1103/PhysRevC.67.051306
2003FU21 Mod.Phys.Lett. A 18, 170 (2003) Y.Funaki, H.Horiuchi, A.Tohsaki, P.Schuck, G.Ropke Description of 8Be as deformed gas- Like two-alpha-particle states NUCLEAR STRUCTURE 8Be; calculated level energies, widths, deformation. Deformed α-cluster condensate.
doi: 10.1142/S0217732303010181
2003SC43 Acta Phys.Hung.N.S. 18, 241 (2003) P.Schuck, H.Horiuchi, G.Ropke, A.Tohsaki Alpha-Particle Condensation in Nuclei
doi: 10.1556/APH.18.2003.2-4.19
2003SC44 C.R.Physique 4, 537 (2003) P.Schuck, H.Horiuchi, G.Ropke, A.Tohsaki Alpha-particle condensation in nuclei
doi: 10.1016/S1631-0705(03)00056-2
2002FU19 Prog.Theor.Phys.(Kyoto) 108, 297 (2002) Y.Funaki, H.Horiuchi, A.Tohsaki, P.Schuck, G.Ropke Description of 8Be as Deformed Gas-Like Two-Alpha-Particle States NUCLEAR STRUCTURE 8Be; calculated level energies, widths, deformation. Deformed α-cluster condensate.
doi: 10.1143/PTP.108.297
2001TO23 Phys.Rev.Lett. 87, 192501 (2001) A.Tohsaki, H.Horiuchi, P.Schuck, G.Ropke Alpha Cluster Condensation in 12C and 16O NUCLEAR STRUCTURE 12C, 16O; calculated α-cluster states energies, widths.
doi: 10.1103/PhysRevLett.87.192501
1998TO30 Prog.Theor.Phys.(Kyoto), Suppl. 132, 213 (1998) Microscopic Study of α-Cluster Matter - New Treatment for Aggregation of Nucleons -
doi: 10.1143/PTPS.132.213
1996TO03 Phys.Rev.Lett. 76, 3518 (1996) Energy Properties of α-Cluster Matter in a Microscopic Description
doi: 10.1103/PhysRevLett.76.3518
1994IS11 Prog.Theor.Phys.(Kyoto) 92, 111 (1994) M.Ishii, R.Tamagaki, A.Tohsaki Energy Properties of Strange Quark Matter Studied in Consitituent Quark Model
doi: 10.1143/ptp/92.1.111
1994TO04 Phys.Rev. C49, 1814 (1994) New Effective Internucleon Forces in Microscopic α-Cluster Model NUCLEAR REACTIONS 4He(α, α), E(cm) ≤ 50 MeV; calculated phase shifts vs E. Microscopic α-cluster model, effective interactions. NUCLEAR STRUCTURE 12C, 20Ne; calculated binding energies. Microscopic α-cluster model, effective interactions.
doi: 10.1103/PhysRevC.49.1814
1992TO09 Prog.Theor.Phys.(Kyoto) 88, 1119 (1992) Microscopic Representation of α-Cluster Matter. I - Formulation -
doi: 10.1143/ptp/88.6.1119
1983TO03 Prog.Theor.Phys.(Kyoto) 69, 113 (1983) Microscopic Study on Di-Nucleus States of 16O + 40Ca and 40Ca + 40Ca. I NUCLEAR REACTIONS 40Ca(16O, 16O), (40Ca, 40Ca), E not given; calculated energy surfaces. Generator coordinate method. NUCLEAR STRUCTURE 56Ni, 80Zr; calculated dinuclear state rotational band characteristics. Generator coordinate method, 16O, 40Ca clusters.
1980AN30 Prog.Theor.Phys.(Kyoto) 64, 1608 (1980) T.Ando, K.Ikeda, A.Tohsaki-Suzuki Nucleus-Nucleus Interaction and Nuclear Saturation Property NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=10-40 MeV; calculated phase shifts vs E, resonance energies; deduced nucleus-nucleus interaction properties. Resonating group method, effective nuclear forces. NUCLEAR STRUCTURE 32S; calculated potential energy surfaces, energy levels, resonances.Resonating group method, effective nuclear forces.
doi: 10.1143/PTP.64.1608
1979AN11 Prog.Theor.Phys. 61, 101 (1979) T.Ando, K.Ikeda, A.Tohsaki-Suzuki Microscopic Study of 16O + 16O Interaction NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=6-60 MeV; calculated phase shifts, energy surfaces for compound system, σ(E, θ). Microscopic approach, generator coordinate method.
doi: 10.1143/PTP.61.101
1978AN24 Prog.Theor.Phys. 59, 2168 (1978) T.Ando, K.Ikeda, A.Tohsaki-Suzuki Nucleus-Nucleus Interaction and Nuclear Saturation Properties. Microscopic Study of 16O + 16O Case NUCLEAR REACTIONS 16O(16O, 16O), E(cm)=15-30 MeV; calculated σ(E, θ). Nuclear saturation effects considered for 32S, 16O systems.
doi: 10.1143/PTP.59.2168
1978TO12 Prog.Theor.Phys. 60, 1013 (1978) Dynamical Structural Change of 12C + 12C System during Scattering Process and Molecular Resonances. I. Microscopic Study of 24-Nucleon System NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), (12C, 8Be), (12C, α), E not given; calculated channel coupling strengths. 24Mg molecular resonances deduced roles of various channels. Coupled-channel generator coordinate method, inelastic excitation of 12C as intermediate path.
1971TO11 Progr.Theor.Phys. 45, 980 (1971) A.Tohsaki, F.Tanabe, R.Tamagaki Quasimolecular Rotational Levels of the 16O+16O System NUCLEAR REACTIONS 16O(16O, 16O), E=0-40 MeV cms; analyzed σ(E). 32S deduced quasimolecular rotational levels.
doi: 10.1143/PTP.45.980
Back to query form |