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Convert All Spot Colors to Process & Overprint Black check boxes: These check boxes control whether all spot colors print as process or black overprints Document Ink Options: This controls how the ink is printed or converts a spot color to a process color The Graphics pane offers these options: Paths: The Flatness setting adjusts the lines Curved lines are defined by lots of tiny straight lines The more accurate to the curved path, the better the quality and the slower it is to print The lower accuracy to the path, the faster it prints, but the quality may not be as high as you might want Fonts: This controls how PostScript fonts are downloaded to the printer Some fonts are stored in the printer, but others that aren t standard on your printer can either be held on the printer or your computer.

In Equation (226) the Bessel function Jm(kR) of order m and argument kR can be seen as a scaling factor between the two domains (near field excitation and far field radiation) The Bessel function is continuous but exhibits large oscillations and has several zeroes (Figure 29) With array sizes and frequencies kR, such that the Bessel function Jm is close to zero, it will not be possible to excite the corresponding far field component Em This has important implications for pattern synthesis and pattern stability versus frequency; more about this later For a given argument kR, the higher-order Bessel functions decay rapidly with increasing order and, hence, higher excitation phase modes radiate poorly How many higherorder modes need to be included before their contributions become negligible An indication is given by Figure 210, showing the error when excluding a particular order as a function of the argument.

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Options: The other options under Graphics are setting the PostScript language and Data format for type You can check the Compatible Gradient and Gradient Mesh printing by converting the gradient or gradient mesh to a JPEG format This area is also where you re informed of your Document Raster Effects Resolution (choose Effect Document Raster Effects Settings) The Color Management pane offers these options: Print Method: The Print Method lists the Color Handling (whether the printer or Illustrator handles the colors), Printer Profile (the color management profile that you want to use), and Rendering Intent (the rendering intent to use when converting colors to a profile space) The Advanced pane offers these options: Print as Bitmap: Click this check box to have your file print as a bitmapped image This is useful to see a quick printout without the quality.

Overprint and Transparency Flattener Options: In this area, you choose whether you want to Simulate, Preserve, or Discard Overprints You also choose the resolution from three presets or specify a custom resolution The Summary area lists the summary of the whole file All the printing options you ve chosen are listed here, and any warnings are listed at the bottom..

exact. Then the gauge bosons acquire a mass if the exact symmetry is hidden (spontaneously broken), A necessary consequence is that the degenerate multiplet structure characteristic of the Wigner realization of a symmetry is lost. Thus, precisely because we see approximately degenerate multiplet structure in the isospin and flavor degrees of freedom we must doubt the possibility of hidden symmetry there. This, and the lack of evidence for massless gauge bosons coupled to flavor degrees of freedom, appear to rule out the gauging of such degrees of freedom; they are thought to be associated with approximate global symmetries. A fundamental consequence of underlying local gauge invariance in a theory with hidden symmetry is the appearance of definite relations between the parameters of the theory. Such theories are typically characterized by a pronounced economy of adjustable constants relative to the predictivity of the theory, because of the stringent requirements imposed by a local gauge invariance. Although the symmetry is hidden, experimental verification of relations among the parameters provides a method to identify the hidden symmetry. It has also been demonstrated in many realistic examples that these relations are precisely what is required to cause cancelations among graphs with bad high-energy behavior and render such theories renormalizable (see Chs. 6 and

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