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PROBLEMS 9.1 Space Bandwidth Product. Use Fourier uncertainty relationships to explain why the resolving power of dispersive spectrometers and the AOTF is proportional to the number of grating cycles in the instrument. How does this result relate to the resolving power of a volume re ection hologram [Eqn. (9.74)] Can you make similar arguments regarding the resolving power of a Fabry Perot or thin- lm lter Dispersive Spectroscopy. Design a slit spectrometer spanning the spectral range 350 950 nm with a spectral resolution of 5 nm. Your design should specify slit size, the focal lengths of any lenses or mirrors used and the period of the grating used. What are the resolving power, etendue, and volume of your system Coded Aperture Spectroscopy. Design and simulate a Hadamard S-matrix spectrometer with N 128. The spectrometer should span the spectral range 350 950 nm with 1 nm resolution. Specify the pixel pitch on the detector array, the coded aperture feature size, and grating and lens parameters. (a) Use synthetic spectra consisting of 1 10 Lorentzian lines of various widths to simulate data collection and processing. Evalutate the mean-square estimation error under linear least-squares and nonnegative least-squares inversion with various levels of additive Gaussian and Poisson noise.

In Step 1 of the previous exercise, I asked you to zoom to 50 percent before using the USM lter. There are two reasons I speci ed that zoom ratio. The rst reason is that historically, Photoshop does the best job of drawing the

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If you choose a color outside of the safe range, you have no assurances of how the color is rendered on a viewer s browser Some systems select the closest color in RGB values; some use dithering (positioning two or more colors next to each other to simulate another color) to try to overcome the limitations of the current screen color depth Therefore, be forewarned: If possible, stick with the browser-safe colors, especially when coloring text Select the Snap-To-Web Safe option in the color picker s context menu to automatically convert the colors you choose to the closest browser-safe color Mac Users: Bring up the system color picker by clicking the System Color Picker button on the Dreamweaver color picker The system color picker for the Mac is far more elaborate than the one available for Windows.

What to do with an unwanted custom pixel aspect ratio If you just can t stand seeing one that you ve created in that Preset list any longer, you can kill off the unwanted ratio by choosing Image Pixel Aspect Ratio Delete Pixel Aspect Ratio. Not much of a surprise there, eh When the resulting Delete Pixel Aspect Ratio dialog box opens, pick the preset you want to kill and click the Delete button. If all you wanted to do was change an existing preset, take a slightly different path: This time, instead of Delete Pixel Aspect Ratio, choose Reset Pixel Aspect Ratios from the Image Pixel Aspect Ratio submenu, and tinker with the Append field, which allows you to restore a previously deleted default ratio value and also keep your custom settings. If you skip the Append option and just click OK, all defaults are restored and anything custom is gone. Seems a bit rash, so handle this with care.

Not to be confused with the Batch Rename command (found on the Bridge, in the File menu), the Batch command in Photoshop s Automate submenu allows you to run any action on a group of files, including renaming the resulting files and storing a log of any errors encountered. This makes it possible to do cool, timesaving things like creating thumbnails (record an action that reduces the images to a specified size and resolution first) and naming them so that the original file name plus a serial number (serially applied) is added to the names. Just about anything that you repeatedly do to a series of files can be done with the Batch command, augmented by the ability to ignore steps

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with y - z replacing yTz. Likewise, if we project z onto the orthogonal direction to y, then the squared sin2(@) where now norm of the resulting projection would again be given by 1/z1)2 (15.43) Returning to Fig. 15.2, we therefore find that the squared distance from the endpoint of G,-1 to is equal to \lGt-1112 sin2(8,-1), where (cf. (15.43)):

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