By Edward R Dougherty
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Additional info for Mathematical morphology in image processing
A further interesting feature of the 0( ΐ> ) images is that the angular distribution is not peaked along the (vertical) direction of the photodissociation electric vector but rather at about 4 5 ° from that axis. The explanation for this phenomenon comes from the further observation that the image depends on the polarization of the ionization laser as well as on the polarization o f the photodissociation laser, as shown in Figure 10. The notation above the images corresponds to the polarization direction o f the dissociation and probe lasers.
ACS Symposium Series; American Chemical Society: Washington, DC, 2000. 9 Total Kinetic Energy [eV] Figure 5 An analysis of the data in Figure 4 shows the vibrational distribution of 0 ( ' A ) from the 265-nm photodissociation of ozone. ; ACS Symposium Series; American Chemical Society: Washington, DC, 2000. ; ACS Symposium Series; American Chemical Society: Washington, DC, 2000. 2 Figure 6 Inverse-Abel-transformed images of the 0 ( Ό ) velocity following photodissociation of ozone at (from upper left to lower right) 235, 245, 255, 265, 275, 280, 285, 290, 294, and 300 nm.
The transitions which lead to I and I* are polarized, respectively, perpendicular and parallel to the molecular axis of the linear molecule. The proof is that when E is parallel to E for the I* channel the REMPI signal of Hgl+ is increased. Conversely for the I channel, when E i s parallel to E the REMPI signal is decreased. The rise of the Hgl+ signal has two peaks. The earlier peak is due to the Hgl whose partner fragments are I atoms and the later peak is due to those Hgl whose partners are I* atoms.