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Don t let frame borders and colors cut up your site. Design so that frame divisions add to the look of your site, or so the page appears to be frameless. Make sure the size of each frame fits the contents nicely or scrolls elegantly to present it. If you ve got a banner that s 500 pixels wide, you ll need a frame that s 500 pixels wide to properly display it. If the frame will scroll, place it so the scrollbar doesn t break up the unified look of the site. Design your content pages with the frameset in mind, remembering that their content needs to fit inside the frames and design your frameset with your site s content in mind. The frameset you choose must be able to accommodate your content. The frameset icons you choose from the Objects palette provide excellent depictions of the frameset structures. Take a look at them in Figure 15-4 or in the Objects palette itself to help you envision your page.

1.2.2.2 Large-Scale PACS The late Roger Bauman, in two papers in the Journal of Digital Imaging (Bauman, 1996a, b), de ned a large-scale PACS as one that satis es the following four conditions: 1. Use in daily clinical operation. 2. Augmented by at least three or four imaging modalities connected to the system. 3. Containing workstations inside and outside of the radiology department. 4. Able to handle at least 20,000 radiological procedures a year. Such a de nition loosely separated the large and the small PACS at that time. However, nowadays most PACS installed except teleradiology are meeting these requirements. Colonel Fred Goeringer instrumented the Army MDIS project, which resulted in several large-scale PACS installations and provided a major stimulus for the PACS industry (Mogel 2003). Dr. Walter W. Hruby opened a completely digital radiology department in the Danube Hospital, Vienna in April, 1992 setting the tone for future total digital radiology departments (Hruby and Maltsidis, 2000; Fig. 1.1j ). Figure 1.1k depicts two medical imaging pioneers, Professor Heniz Lemke (left) and Professor Michael Vannier (right, then editor in chief, IEEE Transactions on Medical Imaging) at the Danube Hospital s opening ceremony. These two projects set the stage for the continuing PACS development.

Here s how to use point filters: 1. Start a command to draw an object. 2. To specify a coordinate, type .x or .y on the command line. You can also find point filters on the object snap shortcut menu (Shift+right-click). 3. The prompt requests a point. Generally, you specify the point by using an object snap. 4. The prompt requests the other coordinate value, which you generally provide by using an object snap. (If you re working in 2D, ignore the request for a Z coordinate.) 5. Continue your command.

Phase Conjugate Laser Optics, edited by Arnaud Brignon and Jean-Pierre Huignard ISBN 0-471-43957-6 Copyright # 2004 John Wiley & Sons, Inc.

Note The acad.pgp and aclt.pgp files contain a special User Defined Command Aliases section at the end for creating your own aliases. Aliases in this section override aliases in the main section.

and the minimum measurable height difference is determined by the total tuning range as 15:32 hmin p= kmax kmin However, other factors in uence these values; for example, the depth of eld of the objective may limit the maximum measurable depth of the object (see Section 1541) 1573 Signal Analysis As explained in the previous section, information about the relative distance between the object and reference plane can be retrieved by nding the fringe frequency or phase change rate at a given point At rst, the fringe frequency was determined by counting the number of zero-crossings of the signal at each pixel Later, a method based on the Fourier transform calculation was developed (Takeda and Yamamoto, 1994; Barnes et al, 1996; Yamaguchi et al, 1998) Figure 1542 shows three interferograms for three different objects at one wavelength during a wavelength scan.

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where A and S are the two constants of integration reflecting the initial conditions, and w ( s ) can be required to be a periodic function with periodicity C. Note the similarity to the harmonic oscillator solution. For K everywhere a positive constant, we would immediately write

Also shown is the signal as recorded by a pixel during a wavelength scan and the Fourier transform of the signal with the peak position determining the height of the object To further improve the resolution of the Fourier transform technique, the rate of phase change (spectral phase slope) along the spectral interference can be calculated (Kinoshita et al, 1999; Mehta et al, 2003a; Mehta et al, 2003b) Wavelength scanning interferometry requires tens or hundreds of registered interferograms during the wavelength scanning of the source The measurement time in wavelength scanning interferometry is the same for shallow and deep surfaces because the number of required frames does not depend on sample s depth like in white light interferometry In the Michelson interferometer object height can be, in relative terms, on both sides of the reference mirror.