Holographic Imaging |
MAS.450/854
|
Holographic Imaging |
MAS.450/854
|
(printable PDF version available here)
When a diffraction grating has a constant groove spacing, or spatial frequency, it deviates an incident beam by a constant angle (which varies with the wavelength of the light). If the spatial frequency varies smoothly with location, the deviation angle also varies smoothly. Thus rays passing through different areas of the grating will no longer be parallel to each other, but may be converging toward each other, or diverging, separating from each other. If the spatial variation of spatial frequency is just right, light from everywhere on the grating will converge at exactly the same point downstream, so that the grating behaves like a perfect "positive" lens. Or, the rays might appear to be diverging from a single common point (or both at the same time). It might be possible to generate such a groove pattern mechanically, after much computation, but it is much easier to do it holographically, by recording the interference pattern produced by two point sources at different distances. Often, one of these sources is a point focus produced by a lens, and the resulting hologram will mimic some of the focusing properties of that lens. One might consider it as a hologram of the lens itself, a sort of "optical clone" of the original lens.
In this lab, you will make and study an in-line hologram of a lens that has been chosen to produce interference fringes that are, in places, coarse enough to be seen with a simple magnifier, and in other places, fine enough to produce significant angles of diffraction. While this may seem to be a very simple type of hologram, it is also one of the most subtle, and most difficult to execute flawlessly. Here our approach will be deliberately crude, but these holographic optical elements will contain all the elements of much more sophisticated image holograms to follow.
Turn on the He-Ne laser, pass the beam through a shutter, and diverge the beam so that it covers half a 4"x5" plate fairly uniformly at about 2 meters away. Install the "split-lens" between the diverging lens and the plate holder so that the plate is illuminated by "straight through" light, and by the focused beam that has gone on to diverge. Position the "split-lens" so that the shadow cast by the lens is roughly the same size as the light focused by the lens. Look from the plates location toward the laser (through a dark filter, please!) and see that there are TWO point sources at different distances, and that the angular separation between them varies with location of your eye (i.e., location on the plate).
Note: To conserve time and holographic plates (they cost about $5.00 each!), several people should share the same holographic lens.