A shell-model analysis of T=1 levels in the nuclei Li<SUP>5</SUP>, O<SUP>16</SUP> and Ti<SUP>18</SUP> is presented in appropriate configuration space and coupling scheme. The important feature of this analysis is that the matrix elements of various energy states are calculated in terms of the matrix elements of the effective interaction (i.e. the reaction matrix in Brueckner's theory) in two-nucleon states of definite relative orbital angular momentum I and total spin S. The nature of the effective interactions thus derived is discussed: the results throw some light on possible non-locality and configuration-dependence of the elements of the reaction-matrix in finite nuclei
The spectra of nuclides involving few valence particles or holes far from β¯ stability are important...
The configuration interaction (CI) approach to solving the nuclear many-body problem, also known as ...
The shell model is used to investigate quantitatively the nuclei in the range 29Si---40Ca. An inert ...
The energy level spectra of O17, O18, O19 and O20 are analysed in the framework of the nuclear shell...
The effective interaction in T=1 two-body states in the sd shell is parameterized in terms of radial...
A density-dependent effective interaction based on a modified G-matrix effective interaction which i...
A simple form of effective nuclear interaction, which has many of the features of the interaction de...
While explaining the success of the shell model of the nucleus, the Brueckner theory of nuclear many...
The shell model is used to investigate quantitatively some odd-parity levels of nuclei in the range ...
We present a quantitative study of the role played by different components characterizing the nucleo...
Ground state properties of finite nuclei ($^{16}$O and $^{40}$Ca) are evaluated from realistic nucle...
Recent breakthroughs in effective interaction and effective operator techniques allow us to take a n...
A simple model interaction for T=0 two-nucleon states in sd shell nuclei is described. All the two-b...
Nuclear spectra of A = 14, 18, 38, 42, 206 and 208 nuclei were calculated using free reaction matric...
Although a large variety of effective interactions have been proposed for the study of nuclear prope...
The spectra of nuclides involving few valence particles or holes far from β¯ stability are important...
The configuration interaction (CI) approach to solving the nuclear many-body problem, also known as ...
The shell model is used to investigate quantitatively the nuclei in the range 29Si---40Ca. An inert ...
The energy level spectra of O17, O18, O19 and O20 are analysed in the framework of the nuclear shell...
The effective interaction in T=1 two-body states in the sd shell is parameterized in terms of radial...
A density-dependent effective interaction based on a modified G-matrix effective interaction which i...
A simple form of effective nuclear interaction, which has many of the features of the interaction de...
While explaining the success of the shell model of the nucleus, the Brueckner theory of nuclear many...
The shell model is used to investigate quantitatively some odd-parity levels of nuclei in the range ...
We present a quantitative study of the role played by different components characterizing the nucleo...
Ground state properties of finite nuclei ($^{16}$O and $^{40}$Ca) are evaluated from realistic nucle...
Recent breakthroughs in effective interaction and effective operator techniques allow us to take a n...
A simple model interaction for T=0 two-nucleon states in sd shell nuclei is described. All the two-b...
Nuclear spectra of A = 14, 18, 38, 42, 206 and 208 nuclei were calculated using free reaction matric...
Although a large variety of effective interactions have been proposed for the study of nuclear prope...
The spectra of nuclides involving few valence particles or holes far from β¯ stability are important...
The configuration interaction (CI) approach to solving the nuclear many-body problem, also known as ...
The shell model is used to investigate quantitatively the nuclei in the range 29Si---40Ca. An inert ...