Figure 12
From: Interference patterns in ionization of Kramers–Henneberger atom
Unfiltered (a) and filtered (b) PMD in the (x, y) plane. PMD is exponentiated (\(P(p_x,p_y)^{1/3}\) is shown) for improving visibility of the patterns. IR field parameters: \(E_0=0.1\) a.u., \(\omega =0.0577\) a.u. XUV field parameters: \(E_0^\mathrm{probe}= 1.5\) a.u., \(\Omega =1.5\) a.u.
