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Holographic stereogram parameters: partial coherence theory The previous discussion uses a purely geometrical description to introduce the basic elements of holographic stereographic imaging. If we want to describe in detail the effects of recording geometry parameters on the final image, however, we need to take into account the wavelike nature of light. Such a physical optics treatment of holographic stereograms, based on partial coherence theory, is presented by St.-Hilaire (1994) and (1995).1v St.-Hilaire (1997) further extends the treatment to arbitrary stereogram geometries and viewer Like the corresponding geometrical interpretation, a physical optics treatment of stereograms starts with the consideration that the planes of interest in the previous section (that is, the hologram plane, the slit plane, and the viewer plane) define a series of pupils through which the light propagates (the very last pupil being the observer s iris itself). It can be demonstrated that the discrete sampling of individual perspectives is equivalent to introducing a quadratic phase error across these pupils. This quadratic phase error corresponds to a defocusing error in the case of a conventional imaging system. Thus the discrete sampling operation results in a blurring akin to misfocus as the focal plane is moved away from the hologram plane. It should be noted that this effect is fundamentally different from the degradation observed when illuminating a conventional hologram

Digital Audio Fundamentals File formats Making audio files lighter MIDI Files MP3 Mini-Primer Player support Encoding MP3 Linking to Audio Files Embedding Sounds and Music Playing background music Targeting Specific Plugins Windows Media Player audio Using Embed with ActiveX Installing Streaming Audio Working with floating or embedded RealAudio players Accessing RealAudio parameters Summary 837 837 839 841 842 842 843 843 844 846 847 847 849 850 850 853 854.

Finding solutions to [E] and [ES ] requires that stasis exists, that their concentrations are constant with time and accordingly that the rates of formation and decomposition of ES and ES are equal, giving rise to the following two equations: k1 [E][S] = (k 1 + k2 ) [ES] [ES ] = k2 k3 [ES] (8.37) (8.38)

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1 Llewellen, T and Karp, J, Pet Systems, pp. 179 194. In Wernick, MN and Aarsvold, Jn, Emission Tomography, The Fundamentals of PET and SPECT, New York, Elsevier, Inc., 2004, p. 180. 2 DuBois, D and DuBois, EF, A Formula to Estimate the Approximate Surface Area if Height and Weight be Known. Arch Int Med, 1916, 17: 863 871. 3 Kim, CK, Gupta, NC, Chandramouli, B, and Alavi, A, Standardized Uptake Values of FDG: Body Surface Area Correction is Preferable

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OSEM One widely used iterative reconstruction technique is the maximum likelihood expectation maximization (MLEM) algorithm. The computation time is very lengthy when all of the projection views are used in each iteration to create the correction slices. To shorten the processing time a smaller group, or subset, of matched projection views from the estimated and original datasets are used for each iteration to create the correction slices. For each iteration a different group or subset is used. Each subset consists of projection views sampled evenly over the entire arc of the acquisition, 180 or 360 . For example, the rst subset might contain every twelfth projection view beginning with the rst projection view. The second subset might contain every twelfth projection view beginning with the sixth projection view, and so on. The process of using subsets for expectation maximization is called ordered subsets expectation maximization (OSEM).

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ribbons and inter-chain interacting base pairs as either rings or rods perpendicular to the helical axis There are two structural grooves that corkscrew along the length of the double helix, the wider of which is called the major groove and the narrower the minor groove (Figure 169) The helix and base pair parameters of B-form DNA are also summarised (Table 12) The helix sense of B-form DNA is right handed, there are 115 base pair residues per turn, and the 2 -deoxy- -d-ribofuranose rings do not adopt the characteristic envelope conformation of furanose rings, but instead exist in a C2 -endo twist conformation (Figure 171) In the original model structure for DNA devised by Watson and Crick, base pairs are coplanar and base pair planes stack perpendicular to the main helix axis.

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