In general, the strong-field induced dynamics are in many aspects similar to the dynamics observed by the XUV pulses. This is direct evidence of general photochemical properties of the PAHs, dictated by their molecular and electronic structures, such as the closely connected carbon framework and a highly conjugated nature of π-bonds. However, there are some noticeable differences with the XUV regime, which are signs of the strong-field excitation character. Here, we will focus the discussion on the channels that were not observed with XUV excitation.