2006
DOI: 10.1088/0256-307x/23/10/026
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Real-Space Wave-Packet Propagation Method: Application to Photoabsorption Processes of Hydrogen Atoms

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Cited by 4 publications
(2 citation statements)
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“…We have used a square grid with a higher concentration of grid points near the nucleus, i.e., r i = i 2 R 0 /N 2 . Furthermore, in the present application of the method, the outer boundary (R 0 ) and the total number of grid points (N ) are chosen to be adaptive for different n and l. Larger R 0 and N are chosen for larger n and l. This kind of numerical-basis set has been used before to calculate atomic photoabsorption spectra for highly excited states as well as continuum states [33,34]. These previous results indicate that the atomic energy levels and dipole transition matrix elements can be well reproduced using the numerical-basis set.…”
Section: A Numerical-basis Statesmentioning
confidence: 99%
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“…We have used a square grid with a higher concentration of grid points near the nucleus, i.e., r i = i 2 R 0 /N 2 . Furthermore, in the present application of the method, the outer boundary (R 0 ) and the total number of grid points (N ) are chosen to be adaptive for different n and l. Larger R 0 and N are chosen for larger n and l. This kind of numerical-basis set has been used before to calculate atomic photoabsorption spectra for highly excited states as well as continuum states [33,34]. These previous results indicate that the atomic energy levels and dipole transition matrix elements can be well reproduced using the numerical-basis set.…”
Section: A Numerical-basis Statesmentioning
confidence: 99%
“…To this end, we numerically obtain finite-space energy eigenstates for the hydrogen atom in a box [33,34], represent the numericalbasis set on a grid, and propagate the system under the influence of an intense laser pulse. As examples, we calculate the transition probabilities to excited bound states and into the continuum as well as electron momentum spectra.…”
Section: Introductionmentioning
confidence: 99%