scholarly journals Doubly-Excited States of Beryllium-Like Ions with Screened Coulomb Potentials

Atoms ◽  
2018 ◽  
Vol 6 (3) ◽  
pp. 41
Author(s):  
Arijit Ghoshal ◽  
Yew Ho

The screening effects of the interaction potentials on the lowest 1S doubly-excited states of beryllium-like ions were investigated by calculating the density of resonance states within the framework of the stabilization method. Two types of screened interaction potentials, namely static screened Coulomb potential and exponential cosine screened Coulomb potential, were taken into consideration. A model potential was used to describe the interaction between the core and outer electrons, and the Be-like ions were treated as being effectively three-body systems. Calculations were performed for Be and B+. It was possible to calculate the energy and width of one doubly-excited state of Be and four doubly-excited states of B+ lying above the 1s22p threshold. Significant changes were found to exist in the behaviour of the width with varying screening parameters. To the best of our knowledge, such an investigation on the doubly-excited states of Be-like ions under screened environments is the first reported calculation of this type in the literature.

Author(s):  
Lalit Kumar Sharma ◽  
Philip Monowe ◽  
Samuel Chimidza

Using nonperturbative solutions, the binding energies for different atoms have been evaluated for the screened Coulomb potentials. The variation of the wavefunction with distance  has also been studied. The results obtained are in excellent agreement with earlier calculations.  


2004 ◽  
Vol 18 (17n19) ◽  
pp. 2590-2594
Author(s):  
BINGCONG GOU ◽  
YIDONG LIU ◽  
FENG WANG

The energies, radiative and Auger rates of the doubly excited states of Be-like Ar 14+ ion are studied by using the multi-configuration-interaction method and model potential method. The doubly excited states of Be-like Ar 14+ are labeled by the quantum numbers K, T and A to show the systematic regularity. The results show that the spectroscopy of Be-like ions is different from that of He-like ions because of the polarization and core penetration effects from the 1s2 core electrons.


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