Ab initio symplectic no-core shell model
暂无分享,去创建一个
Jerry P. Draayer | Tomas Dytrych | James P. Vary | K. D. Sviratcheva | J. Draayer | J. Vary | T. Dytrych | C. Bahri | Kristina D. Sviratcheva | C. Bahri
[1] K. Hecht. Relation between cluster and shell-model wave functions , 1977 .
[2] E. Salpeter. Nuclear Reactions in Stars Without Hydrogen. , 1952 .
[3] S. Avancini,et al. The physical content of the Sp(1,R) model , 1993 .
[4] E. Burtin,et al. Parity-violating electron scattering from 4He and the strange electric form factor of the nucleon. , 2005, Physical review letters.
[5] B. J. Verhaar,et al. A method for the elimination of spurious states in the nuclear harmonic oscillator shell model , 1960 .
[6] W. Glöckle,et al. Three-body interactions and on-shell equivalent two-body interactions , 1990 .
[7] Glenn Starkman,et al. Differentiating between modified gravity and dark energy , 2004 .
[8] M. Harvey,et al. Collective motion in the nuclear shell model III. The calculation of spectra , 1963, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[9] Partial Dynamical Symmetry in the Symplectic Shell Model , 2001, nucl-th/0110030.
[10] R. Wiringa,et al. Accurate nucleon-nucleon potential with charge-independence breaking. , 1995, Physical review. C, Nuclear physics.
[11] S. C. Pieper,et al. Realistic models of pion-exchange three-nucleon interactions , 2001 .
[12] K. Hecht,et al. Vector coherent state theory and its application to the orthogonal groups , 1988 .
[13] The High precision, charge dependent Bonn nucleon-nucleon potential (CD-Bonn) , 2000, nucl-th/0006014.
[14] J. Draayer,et al. Monopole-pairing and deformation in atomic nuclei , 1995 .
[15] W. Gerace,et al. The effect of deformed states in the Ca isotopes , 1967 .
[16] D. R. Entem,et al. Accurate charge dependent nucleon nucleon potential at fourth order of chiral perturbation theory , 2003 .
[17] D. Rowe. Analytical expressions for the matrix elements of the non-compact symplectic algebra , 1984 .
[18] Modern nuclear force predictions for the alpha particle , 2000, Physical review letters.
[19] R. Wiringa,et al. Three-nucleon interaction in 3-, 4- and ∞-body systems☆ , 1983 .
[20] W. Plessas,et al. Nonlocality in the nucleon-nucleon interaction and three-nucleon bound states , 2003 .
[21] K. Hecht,et al. Sp(6, R) symmetry and α-breakup amplitudes of giant E2 excitations in light nuclei , 1978 .
[22] P. Navrátil,et al. Spectra and Binding Energy Predictions of Chiral Interactions for 7Li , 2005, nucl-th/0511082.
[23] G. E. Brown,et al. Even parity states of 16O and 17O , 1966 .
[24] Johnson,et al. Weak-interaction rates in 16O. , 1990, Physical review letters.
[25] N. Barnea,et al. Wave function for no-core effective interaction approaches , 2004 .
[26] W. Gloeckle,et al. Two-pion-exchange three-nucleon potential: Partial wave analysis in momentum space , 1981 .
[27] E. Sheldon,et al. Unified Theory of the Nucleus , 1977 .
[28] A. Miyazaki,et al. Acoustic Phonon Softening and Spontaneous Strains in KD3(SeO3)2 , 1978 .
[29] Construction of high-quality NN potential models. , 1994, Physical review. C, Nuclear physics.
[30] R. Young,et al. Testing the standard model by precision measurement of the weak charges of quarks. , 2007, Physical review letters.
[31] J. Broeckhove,et al. The Sp(2,R) nuclear model of 12C , 1982 .
[32] Song,et al. Nonlocal nature of the nuclear force and its impact on nuclear structure. , 1996, Physical review. C, Nuclear physics.
[33] Jerry P. Draayer,et al. Dominant role of symplectic symmetry in ab initio no-core shell model results for light nuclei , 2007 .
[34] T. Skyrme,et al. Centre-of-mass effects in the nuclear shell-model , 1955, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[35] J. Wilson,et al. Superdeformation in the Doubly Magic Nucleus 40Ca , 2001 .
[36] J. Draayer,et al. Highly deformed modes in the ab initio symplectic no-core shell model , 2008 .
[37] T. W. Donnelly,et al. The interpretation of parity-violating electron-scattering experiments , 1992 .
[38] G. Stephenson,et al. SHAPE OF THE FOUR-PARTICLE, FOUR-HOLE STATE OF ¹⁶O. , 1967 .
[39] Ab initio shell model with a genuine three-nucleon force for the p-shell nuclei , 2003, nucl-th/0305090.
[40] J. Broeckhove,et al. The Sp(2, R) model applied to 8Be , 1979 .
[41] K. Ikeda,et al. Chapter II. Comprehensive Study of Alpha-Nuclei , 1980 .
[42] Y. Suzuki. Cluster and symplectic excitations in nuclei , 1986 .
[43] Y. Suzuki,et al. Structure Study of T = 0 States in 16O by 12C + α Cluster-Coupling Model. II , 1976 .
[44] Wilson,et al. Renormalization of Hamiltonians. , 1993, Physical review. D, Particles and fields.
[45] E. Verlinde,et al. Elliptic de Sitter space: dS/Z(2) , 2002, hep-th/0209120.
[46] Kenji Suzuki,et al. Convergent Theory for Effective Interaction in Nuclei , 1980 .
[47] Kenji Suzuki. Unitary-Model-Operator Approach to Nuclear Effective Interaction. II : Effects of Three-Body Cluster Term , 1982 .
[48] Steven Weinberg,et al. Nuclear forces from chiral Lagrangians , 1990 .
[49] J. Draayer,et al. Pairing-plus-quadrupole model and nuclear deformation: A look at the spin-orbit interaction , 1998 .
[50] David J Rowe,et al. Nuclear Sp(3,R) model , 1977 .
[51] D. R. Entem,et al. Towards a consistent approach to nuclear structure: EFT of two- and many-body forces , 2005, nucl-th/0503025.
[52] J. Wood,et al. Implications of deformation and shape coexistence for the nuclear shell model. , 2006, Physical review letters.
[53] J. Draayer,et al. Fermion realization of the nuclear Sp(6,R) model , 1998 .
[54] Effective Operators Within the Ab Initio No-Core Shell Model , 2004, nucl-th/0412004.
[55] K. Hecht. The use of SU(3) in the elimination of spurious center of mass states , 1971 .
[56] L. Biedenharn,et al. Nuclear rotational bands and SL(3, R) symmetry , 1970 .
[57] D. Rowe,et al. Coupled SU(3) models of rotational states in nuclei and quasi-dynamical symmetry , 2006 .
[58] Poisson algebra of diffeomorphism generators in a space-time containing a bifurcation , 2004, hep-th/0403219.
[59] Ab-initio coupled-cluster study of 16O. , 2005, Physical review letters.
[60] H. T. Coelho,et al. Taming the two-pion exchange three-nucleon potential , 1986 .
[61] S. Coon,et al. Reworking the Tucson-Melbourne Three-Nucleon Potential , 2000, nucl-th/0101003.
[62] W. Greiner,et al. The general collective model applied to the chains of Pt, Os and W isotopes , 1981 .
[63] R. Blin-stoyle. A Unified Theory of the Nucleus , 1978 .
[64] P. Navrátil,et al. Ab initio shell model calculations with three-body effective interactions for p-shell nuclei. , 2002, Physical review letters.
[65] P. Navrátil,et al. Shell Model in a First Principles Approach , 2004 .
[66] Stoks,et al. Partial-wave analysis of all nucleon-nucleon scattering data below 350 MeV. , 1993, Physical review. C, Nuclear physics.
[67] A Nogga,et al. Structure of A=10-13 nuclei with two- plus three-nucleon interactions from chiral effective field theory. , 2007, Physical review letters.
[68] Kenji Suzuki. Construction of Hermitian Effective Interaction in Nuclei--General Relation between Hermitian and Non-Hermitian Forms , 1982 .
[69] P. Heenen,et al. On the deformation energy surface of 16O , 1984 .
[70] A unitary correlation operator method , 1997, nucl-th/9709038.
[71] J. P. Elliott,et al. Collective motion in the nuclear shell model. I. Classification schemes for states of mixed configurations , 1958, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[72] From non-Hermitian effective operators to large-scale no-core shell model calculations for light nuclei , 2006, nucl-th/0603034.
[73] Petr Navratil,et al. Large-basis ab initio no-core shell model and its application to 12 C , 2000 .
[74] A. Zuker,et al. Structure of O 16 , 1968 .
[75] Tensor correlations in the unitary correlation operator method , 2002, nucl-th/0207013.
[76] G. Rosensteel. Irreducible U(3) tensor interactions in the symplectic collective model , 1980 .
[77] E. Boeker. HARTREE--FOCK CALCULATIONS IN LIGHT NUCLEI. , 1967 .
[78] U. van Kolck,et al. Few-nucleon forces from chiral Lagrangians. , 1994 .
[79] J. Vary. How Effective are Strong Interactions , 2005 .
[80] Franz Wegner. Flow‐equations for Hamiltonians , 1994 .
[81] R. Furnstahl,et al. Similarity renormalization group for nucleon-nucleon interactions , 2006, nucl-th/0611045.
[82] Tomás Dytrych,et al. Evidence for symplectic symmetry in Ab initio no-core shell model results for light nuclei. , 2007, Physical review letters.
[83] David J Rowe,et al. Microscopic theory of the nuclear collective model , 1985 .
[84] A. Richter,et al. Structure of the Hoyle state in 12C. , 2007, Physical review letters.
[85] A. I. Mazur,et al. Novel NN interaction and the spectroscopy of light nuclei [rapid communication] , 2004, nucl-th/0407018.
[86] J. Draayer,et al. Shell-model operator for KJ-band splitting in odd-A nuclei , 1992 .
[87] D. Rowe. Coherent state theory of the noncompact symplectic group , 1984 .
[88] B. G. Wybourne,et al. Classical Groups for Physicists , 1974 .
[89] L. Zamick,et al. Four-particle-four-hole states in 4He , 1984 .
[90] J P Vary,et al. Properties of 12C in the Ab initio nuclear shell model. , 2000, Physical review letters.
[91] Y. Leschber,et al. Shape variables and the shell model , 1988 .
[92] P. Navrátil,et al. Few-nucleon systems in a translationally invariant harmonic oscillator basis , 1999, nucl-th/9907054.
[93] Suzuki,et al. Isoscalar monopole and quadrupole strength of 16O in an alpha +12C cluster and symplectic mixed basis. , 1989, Physical review. C, Nuclear physics.
[94] J. Draayer,et al. SU(3) symmetry breaking in lower fp-shell nuclei , 2000, nucl-th/0009014.
[95] S. Gupta,et al. PHENOMENOLOGICAL APPROACH TO FOUR-PARTICLE, FOUR-HOLE STATES IN $sup 16$O. , 1969 .
[96] W. Greiner,et al. Collective potential energy surfaces and nuclear structure , 1971 .
[97] F. Hoyle,et al. On Nuclear Reactions Occuring in Very Hot STARS.I. the Synthesis of Elements from Carbon to Nickel. , 1954 .
[98] J. P. Elliott,et al. Collective motion in the nuclear shell model II. The introduction of intrinsic wave-functions , 1958, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[99] Wilson loops as precursors , 1999, hep-th/9909013.
[100] J. Draayer,et al. Shell-model operator for K-band splitting , 1990 .
[101] H. Ui. Quantum Mechanical Rigid Rotator with an Arbitrary Deformation. I Dynamical Group Approach to Quadratically Deformed Body , 1970 .
[102] A. I. Mazur,et al. Nucleon–Nucleon Interaction in the J-Matrix Inverse Scattering Approach and Few-Nucleon Systems , 2003, nucl-th/0312029.
[103] Nd elastic scattering as a tool to probe properties of 3N forces , 2000, nucl-th/0010013.
[104] J. Draayer. Structure calculations for 25Mg-25Al , 1973 .
[105] Barrett,et al. No-core shell-model calculations with starting-energy-independent multivalued effective interactions. , 1996, Physical review. C, Nuclear physics.
[106] K. Hecht,et al. Symplectic and cluster excitations in nuclei:: Evaluation of interaction matrix elements , 1986 .
[107] David J Rowe,et al. On the algebraic formulation of collective models III. The symplectic shell model of collective motion , 1980 .
[108] S. Pollock,et al. Intermediate-energy semileptonic probes of the hadronic neutral current☆ , 1993, nucl-th/9307022.
[109] G. E. Brown,et al. Collective admixtures in the odd-parity states of O16 , 1965 .