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where the incident beam is perfectly parallel to the axis of the transition, LD > 0. If the polarization is perfectly perpendicular to this axis, then LD < 0. In LD spectroscopy, samples are orientated in a single axis relative to the incident linearly polarized light and it is possible to vary the relative orientation of sample and light such that the incident light is parallel or perpendicular to this axis. A wide variety of physico-chemical means of achieving this orientation have been described (Figure 3.40). In the stretched polymer technique, orientation is achieved by absorbing sample onto a polymer (e.g. polyvinylalcohol) either before or after stretching it in a particular direction. The long axis of the sample molecule aligns in the stretch direction. Other popular techniques include ow orientation, electric eld orientation and squeezed gel orientation.

Axial Ratio (dB)

Within most application protocols, packets have an associated type (request, reply, and error messages are pretty common types). Some firewalls scan for suspicious patterns of message types to block potential attacks.

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relied on over any reasonable dynamic range. We therefore give only graphical presentations of spread functions in this chapter. 11.2.1. The Aberration Free Airy Pattern Figure 11.1 shows the Airy pattern, the monochromatic aberration-free point spread function for a system with a circular aperture of uniform transmission, and Figure 11.2 shows the same with logarithmic vertical scale. What is plotted in these two gures is the light intensity (vertical) against the radial distance from the center of the image (horizontal). The light intensity is scaled to unity at the center of the pattern. The radial coordinate z, which lies in the image plane, is given by 2p sin aZ 11:1 l where l is the wavelength of the light, a is the convergence angle (cone semiangle) of the image-forming beam, and Z is the actual radial distance. Thus the radial coordinate as shown is dimensionless and is often said to be in z units or diffraction z

and hedonic cues; these show considerable variability in their impact on individuals and probably contribute a signi cant role to susceptibility to obesity (see 8). Elucidating the neural and neurochemical basis of these effects seems most likely to advance the understanding and treatment of human obesity. Current evidence points to the involvement of dopaminergic pathways in the reward circuit of the brain, as well as endocannabinoids acting in the hypothalamus and elsewhere. Consistent with the latter suggestion, rimonabant (an antagonist of cannabinoid CB1 receptors) has been shown to reduce food intake and body weight in obese subjects (see 17). Susceptibility to obesity could be partly determined by polymorphisms in speci c dopamine, cannabinoid or other receptors that in uence the activity of the reward or related pathways.

private ModelAndView retrievePicture(HttpServletRequest req, HttpServletResponse resp) { // Implementation details omitted. } private ModelAndView createPicture(HttpServletRequest req, HttpServletResponse resp) { // Implementation details omitted. } }

To create a block, first create the objects just as you want to save them. You may include other blocks as objects in your block. (A block within a block is called a nested block.) After you ve created the objects for your block, follow these steps: 1. Choose Make Block from the Draw toolbar to start the BLOCK command and open the Block Definition dialog box, shown in Figure 18-3. The dialog box guides you through the process of defining a block.

160 163 164

Frequency (GHz)

C Li and T-W Chou, Vibrational Behaviors of Multiwalled-Carbon-Nanotube-Based Nanomechanical Resonators, Appl Phys Lett 84(1), 121 (2004) M Yudasaka, H Kataura, T Ichihashi, L C Qin, S Kar, and S Iijima, Diameter Enlargement of HiPco Single-Wall Carbon Nanotubes by Heat Treatment, Nano Letters 1(9), 487 489 (2001) B H Hong et al, Fabrication of Silver Nanowires, Science 294, 348 (2001) S J Tans, M H Devoret, H Dai, A Thess, R E Smalley, L J Geerligs, and C Dekker, Individual Single-Wall Carbon Nanotubes as Quantum Wires, Nature 386, 474 (1997) A Javey, M Shim, and H Dai, Electrical Properties and Devices of Large-Diameter Single-Walled Carbon Nanotubes, Appl Phys Lett 80(6), 1064 (2002) P C Collins, M S Arnold, and P Avouris, Engineering Carbon Nanotubes and Nanotube Circuits Using Electrical Breakdown, Science 292, 706 (2001) A Bachtold, P Hadley, T Nakanishi, and C.

Figure 18-42: The output file that results from extracting the attributes in the office building plan.

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