Photoelectron spectra (PES) of the atom are investigated in a Debye plasma environment using an intense, linearly polarized femtosecond (fs) pulsed laser. In the strong field approximation, for a single active electron, the three-dimensional nonrelativistic time-dependent Schrödinger equation is solved numerically by the Crank–Nicolson method. PES is investigated for different Debye lengths (5[Formula: see text]a.u.,10[Formula: see text]a.u. and 15[Formula: see text]a.u.) using the infinite surface flux method, and a shift in the peak positions is observed. PES in the plasma environment for various laser pulse cycles ([Formula: see text], 20 and 30) is also analyzed. Momentum-resolved PES shows the increase in the radius of the above-threshold ionization (ATI) rings due to the plasma screening effect.
The one-electron potential, [Formula: see text], appearing in the Schrödinger equation for the charge density is calculated for the neutral atoms from hydrogen to uranium, and t...
The radial charge distribution, D(r), for the neutral atoms, hydrogen through uranium, and the singly positive ions, helium through barium and lutetium through radium, are compu...
Femto- to picosecond excited-state dynamics of the complexes [Re(L)(CO)_(3)(N,N)]^n (N,N = bpy, phen, 4,7-dimethyl-phen (dmp); L = Cl, n = 0; L = imidazole, n = 1+) were invest...
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