CVA ionization spectra for mathrm{H}_{2}^{+} in the forward condition from (a) 1sσ and <em>R</em> = 2 au, solid line; (b) 2<em>p</em>σ and <em>R</em> = 2 au, dotted line; (c) 1sσ and <em>R</em> = 1.4 au, dashed–dotted line

2013-08-27T00:00:00Z (GMT) by R Della Picca J Fiol P D Fainstein
<p><strong>Figure 9.</strong> CVA ionization spectra for \mathrm{H}_{2}^{+} in the forward condition from (a) 1sσ and <em>R</em> = 2 au, solid line; (b) 2<em>p</em>σ and <em>R</em> = 2 au, dotted line; (c) 1sσ and <em>R</em> = 1.4 au, dashed–dotted line. The laser parameters are the same as used in figure <a href="http://iopscience.iop.org/0953-4075/46/17/175603/article#jpb471071f7" target="_blank">7</a>. Curves (b) and (c) are shifted in energy.</p> <p><strong>Abstract</strong></p> <p>We present a detailed study of the ionization probability of H and H_{2}^{+} induced by a short intense laser pulse. Starting from a Coulomb–Volkov description of the process we derive a multipole-like expansion where each term is factored into two contributions: one that accounts for the effect of the electromagnetic field on the free-electron final state and a second factor that depends only on the target structure. Such a separation may be valuable to solve complex atomic or molecular systems as well as to interpret the dynamics of the process in simpler terms. We show that the series expansion converges rapidly, and thus the inclusion of the first few terms is sufficient to produce accurate results.</p>