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The preceding chapter discussed to the two-step, master-transfer, or Hl-H2 method of making holograms, in which a first hologram is used to create a real image in space, which then becomes the object for a second hologram Normally, the image is brought as close as possible to the plane of the second hologram, the H2, so as to minimize the sensitivity of the resulting image to the source-size and color blurs usually produced by an ordinary white-light source, such as a spotlight or the sun As such, the resulting hologram was first popularly described as an image-plane hologram, although technically the image has no plane because it has depth! We prefer to call these open-aperture transfers, or full-aperture transfers for reasons that will become clear in the next chapter.

It is true that the image is usually intended to straddle the hologram plane very carefully, to minimize the maximum depth of the image This chapter is the story of the H2 and its optics The previous chapter tells us almost everything we need to know about the H1, and a great deal of what we will need to know about the H2 as well Basically, the H2 is also recorded as an off-axis transmission hologram that is later reconstructed with phase-conjugate illumination The pseudoscopic image that results is then a depth-reversed image of a projected real image that was itself pseudoscopic, or depthreversed Two pseudos make an ortho, might be the rule-the final image reads with the correct depth compared to the original object Thus we have produced a right-reading holographic image that is remarkably clear when viewed with ordinary light sources.

There are quite a few complicating factors that we have to take into account though First, the coordinate system for the H2 is oriented differently from what we have been used to, and we have to agree upon a convention for the rotation and translation of local hologram coordinate systems in general Second, the H2 is actually a hologram of two things at once: of the projected real image of the object, and of the H1 itself Consideration of the second brings a new point of view to the imaging process The exposure of the H2 is to a focused and nearly photographic-like real image, with large intensity variations over small distances, which makes the beam ratio more difficult to measure and adjust.

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You can even determine the order of execution for the actions connected to a single event. With Dreamweaver behaviors, hours of complex JavaScript coding are reduced to a handful of mouse clicks and a minimum of data entry. All behavior assigning and modification are handled through the Behaviors panel.

And finally, because the H1 and H2 play very different roles in the imaging process, their exposure and processing should be separately optimized with quite different criteria in mind As impressive as a full-aperture transfer hologram is upon first sight, be cautioned that it is only a transitory state The technique is of major importance for reflection holograms (serving as the H2), and we will revisit it later But it will serve here mainly to frame the discussion in the following chapter about more advanced rainbow transmission holograms There are quite a few concepts to layer on.

Likewise, if you want a particular element to be a certain height, you can specify the height using the height property.