Three-body models of the 6 ?? He and 9 ? Be hypernuclei with non-local interactions

[1]  I. Filikhin,et al.  Cluster models of 6 ?? He and 9 ? Be hypernuclei , 2004 .

[2]  I. Filikhin,et al.  Cluster models of (Lambda Lambda)He-6 and (Lambda)Be-9 hypernuclei , 2004, nucl-th/0406049.

[3]  M. Shoeb Variational Monte Carlo calculation ofHeΛΛΛ6and others-shell hypernuclei , 2004 .

[4]  Triumf,et al.  Faddeev calculation of ??6He using SU6 quark-model baryon-baryon interactions , 2004, nucl-th/0405056.

[5]  D. Baye,et al.  Faddeev calculation of 3α and ααΛ systems using αα resonating-group method kernels , 2004 .

[6]  T. Yamada ΛΛ−ΞN−ΣΣcoupling inHeΛΛΛ6with the Nijmegen soft-core potentials , 2004 .

[7]  M. Kohno,et al.  Brueckner rearrangement effects inΛ5HeandΛΛ6He , 2003 .

[8]  D. Baye,et al.  Comparative variational studies of 0+ states in three-α models , 2003, nucl-th/0501058.

[9]  D. Baye,et al.  Three body systems with Lagrange mesh techniques in hyperspherical coordinates , 2003 .

[10]  I. Filikhin,et al.  Faddeev calculations for the A = 5,6 Lambda Lambda hypernuclei , 2003, nucl-th/0303028.

[11]  M. Hesse,et al.  Solving the resonating-group equation on a Lagrange mesh , 2002 .

[12]  Y. Akaishi,et al.  ΛΛ-Ξ N coupling effects in light hypernuclei , 2002, nucl-th/0209090.

[13]  A. Fonseca,et al.  Three body calculation of the structure of lambda Be-9 , 2002 .

[14]  E. Hiyama,et al.  Four-body cluster structure of a = 7-10 double-Λ hypernuclei , 2002, nucl-th/0204059.

[15]  M. May,et al.  Hypernuclear fine structure in (Lambda*)Be-9 , 2002 .

[16]  M. Hesse,et al.  The unexplained accuracy of the Lagrange-mesh method. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[17]  Chung,et al.  Observation of a (Lambda Lambda)He-6 double hypernucleus , 2001 .

[18]  E. Hiyama,et al.  Three- and Four-Body Cluster Models of Hypernuclei Using theG-Matrix ΛN Interaction 9ΛBe, 13ΛC, 6ΛΛHe and 10ΛΛBe , 1997 .

[19]  D. Baye,et al.  Inverse scattering with singular potentials: A supersymmetric approach , 1997 .

[20]  S. Okabe,et al.  Evidence for a central repulsion potential from pionic decay of s-shell Λ-hypernuclei , 1995 .

[21]  Daniel Jean Baye,et al.  Regularization of singularities in Lagrange-mesh calculations , 1993 .

[22]  Baye Supersymmetry between deep and shallow nucleus-nucleus potentials. , 1987, Physical review letters.

[23]  H. Takaki,et al.  Λ N Exchange-Force Effects on the Binding Energies of 5 Λ He, 9 Λ Be, 6 Λ Λ He and 10 Λ Λ Be Hypernuclei , 1986 .

[24]  Daniel Jean Baye,et al.  Generalised meshes for quantum mechanical problems , 1986 .

[25]  K. Ikeda,et al.  Light p-Shell Λ-Hypernuclei by the Microscopic Three-Cluster Model , 1983 .

[26]  M. D. L. Ripelle,et al.  The potential harmonic expansion method , 1983 .

[27]  V. I. Kukulin,et al.  The orthogonal projection method in scattering theory , 1978 .

[28]  E. Sheldon,et al.  Unified Theory of the Nucleus , 1977 .

[29]  B. Buck,et al.  Local potential models for the scattering of complex nuclei , 1977 .

[30]  F. Wysotzki,et al.  A new determination of the binding-energy values of the light hypernuclei (A ≤ 15) , 1973 .

[31]  J. Raynal,et al.  Transformation coefficients in the hyperspherical approach to the three-body problem , 1970 .

[32]  S. H. R. Ali Phenomenological a-a potentials , 1966 .

[33]  Irene A. Stegun,et al.  Handbook of Mathematical Functions. , 1966 .