scholarly journals Application of Coulomb wave function discrete variable representation to atomic systems in strong laser fields

2006 ◽  
Vol 125 (15) ◽  
pp. 154311 ◽  
Author(s):  
Liang-You Peng ◽  
Anthony F. Starace
2021 ◽  
Vol 323 ◽  
pp. 14-20
Author(s):  
Naranchimeg Dagviikhorol ◽  
Munkhsaikhan Gonchigsuren ◽  
Lochin Khenmedekh ◽  
Namsrai Tsogbadrakh ◽  
Ochir Sukh

We have calculated the energies of excited states for the He, Li, and Be atoms by the time dependent self-consistent Kohn Sham equation using the Coulomb Wave Function Discrete Variable Representation CWDVR) approach. The CWDVR approach was used the uniform and optimal spatial grid discretization to the solution of the Kohn-Sham equation for the excited states of atoms. Our results suggest that the CWDVR approach is an efficient and precise solutions of excited-state energies of atoms. We have shown that the calculated electronic energies of excited states for the He, Li, and Be atoms agree with the other researcher values.


2007 ◽  
Vol 06 (04) ◽  
pp. 823-831
Author(s):  
KAI-JUN YUAN ◽  
ZHIGANG SUN ◽  
SHU-LIN CONG ◽  
NANQUAN LOU

The Bessel discrete variable representation (DVR) method is tested to describe the interaction of atomic hydrogen with intense laser fields by numerically solving the time-dependent Schrödinger equation. Using the Bessel functions of the first kind, the singular terms, r-2 or r-1 at the origin, in the kinetic energy operators are analytically solved. As an illustration example, the high-order harmonic generation (HOHG) spectra in atomic hydrogen is calculated in length and acceleration forms. From the numerical results, it is concluded that this simple Bessel DVR may be a useful method for describing the interaction of atomic hydrogen with intense laser fields.


2003 ◽  
Vol 02 (01) ◽  
pp. 73-90 ◽  
Author(s):  
G. D. BILLING

We present a new method for treating the dynamics of molecular systems. The method has been named "quantum dressed" classical mechanics and is based on an expansion of the wave function in a time-dependent basis-set, the Gauss–Hermite basis-set. From here it is possible to proceed in two ways, one is in principle exact and the other approximate. In the exact approach one constructs a discrete variable representation (DVR) in which the grid points are defined by the Hermite part of the Gauss–Hermite basis set. In the approximate method a second order expansion of the potential around the classical trajectories is introduced and the quantum dymamics solved in a second quantization rather than a wave-function representation.


2015 ◽  
Vol 92 (6) ◽  
Author(s):  
Noslen Suárez ◽  
Alexis Chacón ◽  
Marcelo F. Ciappina ◽  
Jens Biegert ◽  
Maciej Lewenstein

2012 ◽  
Vol 137 (9) ◽  
pp. 094101 ◽  
Author(s):  
Qi-Cheng Ning ◽  
Liang-You Peng ◽  
Xue-Feng Hou ◽  
Zhen Xu ◽  
Qihuang Gong

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