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lattice a sandwich of layers of material of a very different refractive index that stops photons of a particular frequency from passing through. Some photons managed to penetrate the obstacle by tunnelling and these appeared to arrive at nearly twice the speed of light. Chiao didn t nd this disturbing. Because the technique he used to generate photons for his experiment meant that they were produced at random, there was no way to send a signal, which meant no possibility of getting information to travel back in time and disrupt causality. The next year, though, G nter Nimtz came up with another experiment that seemed to show something very different and, being Nimtz, he publicized it in a very dramatic way.

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For constant D and l, NF decreases as z increases. The Fresnel diffraction intensity from a square aperture is visualized in Figures 5.2 5.5. As z gets less, the intensity starts resembling the shape of the input square aperture. This is further justi ed in Example 5.5. Figure 5.2 shows the image of the square aperture used. Figure 5.3 is the Fresnel intensity diffraction pattern from the square aperture. Figure 5.4 is the same intensity diffraction pattern as a 3-D plot.

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try { _IsCompleted = readBoolean(xs.takeAttributeValue()); } catch (Exception x) { throw new ConversionException(an, x); } isDefaulted_IsCompleted = false; continue; } throw new InvalidAttributeException(an); } { xs.takeStart("idNumber"); String s; if (xs.atChars(XMLScanner.WS_COLLAPSE)) { s = xs.takeChars(XMLScanner.WS_COLLAPSE); } else { s = ""; } try { _IdNumber = Integer.parseInt(s); } catch (Exception x) { throw new ConversionException("idNumber", x); } has_IdNumber = true; xs.takeEnd("idNumber"); } if (xs.atStart("name")) { xs.takeStart("name"); String s; if (xs.atChars(XMLScanner.WS_COLLAPSE)) { s = xs.takeChars(XMLScanner.WS_COLLAPSE); } else { s = ""; } try { _Name = String.valueOf(s); } catch (Exception x) { throw new ConversionException("name", x); } xs.takeEnd("name"); } if (xs.atStart("description")) { xs.takeStart("description"); String s; if (xs.atChars(XMLScanner.WS_COLLAPSE)) { s = xs.takeChars(XMLScanner.WS_COLLAPSE); } else { s = ""; } try { _Description = String.valueOf(s); } catch (Exception x) { throw new ConversionException( "description", x); } xs.takeEnd("description"); } { List l = PredicatedLists.create(this, pred_Task, new ArrayList());

Figure 6.17 ATR spectrum of a nylon 6 lm. From Polymer Analysis, AnTS Series, Stuart, B. H. Copyright 2002. John Wiley & Sons Limited. Reproduced with permission.

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Diffractive optics involves creation of holograms by computation in a digital computer, followed by actual implementation by a recording system such as a laser lm writer, scanning electron beam writer, high resolution printer, usually followed by photoreduction, and the like. Diffractive optics is very versatile since any type of wave can be considered for computation within the computer. Digital holograms created with such technology are more commonly called diffractive optical element (DOE). Another name for DOE is computer-generated hologram (CGH). Because of these equivalent terminologies, the words hologram, DOE, and CGH will be used equivalently in this chapter. In communication engineering, it is well known that a complex signal must be coded in some fashion before it can be transmitted over a single channel. This can be done by modulating the amplitude of a carrier by the modulus of the complex signal and/or by modulating the phase of the carrier by the phase of the complex signal. The real part of this modulated carrier then can be transmitted, and through proper demodulation procedures, the complex signal can be recovered at the receiver. Both holography and diffractive optics are based on such modulation and demodulation principles. DOEs have found applications in many areas such as wave shaping, laser machining, 3-D displays [Yatagai, 1975], optical pattern recognition, optical interconnects, security devices [Dittman, et al., 2001], optical communications/networking, and spectroscopy. Some important advantages of DOEs are as follows: A DOE can perform more than one function, for example, have multiple focal points, corresponding to multiple lenses on a single element. It can also be designed for use with multiple wavelengths. DOEs are generally much lighter and occupy less volume than refractive and re ective optical elements. With mass manufacturing, they can be manufactured less expensively for a given task.

9.2.4.5 Weighted De cit Round Robin (WDRR)

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