This thesis finds the basis states of the symplectic model for nuclear collective behaviour. We are able to find a complete set of states for Sp(6), the most important group of collective motions in nuclei. From the multitude of possible eigenstates we are interested in vibrational type ones, or Bohr-Mottelson type, which are at the same time a basis in the subgroup Sp(2) x 0(3) of Sp(6). The basis we find is not orthonormal but complete and nonredundant and we how to use it to determine generator matrix elements between these states. Since the Hamiltonian of the problem is in the enveloping algebra of Sp(6) it can be expressed as a low rank polynomial in the Sp(6) generators and the actual vibrational spectrum of nuclei is then calculable....
As suggested by Vanagas, we choose the microscopic collective states for a system of A nucleons to b...
In the present paper, we introduce partially coherent states for the positive discrete series irredu...
Matrix elements of the group generators for the symmetric irreducible representations of SO(6) are e...
By including the electric dipole operator among the generators, the sp(6, R) algebra of the nuclear ...
In this paper we consider a basis for N boson states classified by the chain of groups U(6)⊃U(3)⊃U(2...
The fermion dynamical symmetry model (FDSM) is a model of nuclear structure based on a fermion pair ...
Both non-Hermitian Dyson and Hermitian Holstein-Primakoff representations of the Sp(2d,R) algebra ar...
A practical method is given for the evaluation of the matrix elements of a general two-body interact...
A classification of nuclear states according to the non-compact Lie algebra Sp(4, R) is investigated...
Based on a generalized reduction scheme for boson representations of symplectic algebras of the type...
Microscopic nuclear calculations are approached by partitioning the many-nucleon Hilbert space as a ...
The generating function method that we had developing has various applications in physics and not on...
We give a complete classification of basis states with unitary (U(A 1); U(3)) and permutational(S(A...
In the present series of papers, the coherent states of Sp(2d,R), corresponding to the positive disc...
The representation theory of the recently introduced proton-neutron symplectic model in the many-par...
As suggested by Vanagas, we choose the microscopic collective states for a system of A nucleons to b...
In the present paper, we introduce partially coherent states for the positive discrete series irredu...
Matrix elements of the group generators for the symmetric irreducible representations of SO(6) are e...
By including the electric dipole operator among the generators, the sp(6, R) algebra of the nuclear ...
In this paper we consider a basis for N boson states classified by the chain of groups U(6)⊃U(3)⊃U(2...
The fermion dynamical symmetry model (FDSM) is a model of nuclear structure based on a fermion pair ...
Both non-Hermitian Dyson and Hermitian Holstein-Primakoff representations of the Sp(2d,R) algebra ar...
A practical method is given for the evaluation of the matrix elements of a general two-body interact...
A classification of nuclear states according to the non-compact Lie algebra Sp(4, R) is investigated...
Based on a generalized reduction scheme for boson representations of symplectic algebras of the type...
Microscopic nuclear calculations are approached by partitioning the many-nucleon Hilbert space as a ...
The generating function method that we had developing has various applications in physics and not on...
We give a complete classification of basis states with unitary (U(A 1); U(3)) and permutational(S(A...
In the present series of papers, the coherent states of Sp(2d,R), corresponding to the positive disc...
The representation theory of the recently introduced proton-neutron symplectic model in the many-par...
As suggested by Vanagas, we choose the microscopic collective states for a system of A nucleons to b...
In the present paper, we introduce partially coherent states for the positive discrete series irredu...
Matrix elements of the group generators for the symmetric irreducible representations of SO(6) are e...