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(5.17) where 2 F1 ( , ; ; ) is the Gauss hypergeometric function [1, Eq. (15.1.1)]. Thus, using (5.17) in (5.16) gives Im (a, m, ) k 2 m 1 2 1 1 2 a 2m a 2k , 1 2 k 2m 4 k=0 a 2 /2 a2 = , 2m m + a 2 /2 m integer = m+ 1 a 2 /2m 1 I (a, m, ) = 2 m 2 1 + a 2 /2m m+(1/2) (m + 1) 1 m , 2 F1 1, m + ; m + 1; 2 m + a 2 /2 m noninteger

(SEC), Food and Drug Administration (FDA), National Association of Securities Dealers (NASD) and so on. In this phase, performance is not critical, but the architecture needs to provide low cost, security, longevity as mandated by policy, reliable access during the retention period and full expungement at the end of the life cycle. Discovery. As a common thread for data across its life cycle, a storage architecture needs to accommodate an ability to easily search and retrieve data at any point from creation to archive. This has been often overlooked in the past, but recent regulatory pressures have led organizations to reengineer their storage environment to accommodate this requirement. This requirement necessitates the ability to search for data using key words and has an ability to access the data reliably using intuitive means, ideally with minimal intervention from system administrators, as this can become a costly endeavour.

09:29:03

(E.37)

TABLE 15-6

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A message-based architecture tends to handle load balancing and fail-over much better than an RPC-based architecture. Typically, message-based architectures use asynchronous messaging, by means of which data are transferred using messages that are sent to a queue. The queue handles processing from there. There s no need

The File menu item contains items to create and manage the terminal tabs: Open Terminal: Start a new shell session in a new GNOME Terminal window. Open Tab: Start a new shell session on a new tab in the existing GNOME Terminal window. New Pro le. . .: Allows you to customize the tab session and save it as a pro le which you can recall for use later. Close Tab: Close the current tab in the window. Close Window: Close the current GNOME Terminal session, closing all active tabs. Most of the items in the File menu are also available by right-clicking in the session tab area. The New Pro le entry allows you to customize your session tab settings and save them for future use. The New Pro le rst requests that you provide a name for the new pro le, then produces the Editing Pro le dialog box, shown in Figure 2-10.

est transition temperature to superconductivity, a value of 12.8 K, was reported for a halogenated BEDT-TTF-Cu-complex (Williams and Beno, 1990). Molecular and crystal structures are shown in Fig. 4.8- 15. Raman spectroscopy has appreciably promoted the understanding of these systems, since it demonstrates that any type of charge-transfer leads to a considerable line shift of molecular vibrational modes (Bozio et al., 1975). In TTF, shifts by as much as 80 cm have been observed during charge-transfer between zero and 0.7 (Kuzmany and Kundu, 1979). Similarly, a charge-transfer of 1 in TCNQ resulted in a downshift of the Agv4 mode (C=C stretching) by up to 65 cm ~ 'Assuming . a linear relation between charge-transfer and frequency shift of TTF-TCNQ, the chargetransfer was determined to be 0.55, which yields band filling up to 2 kp- = 0.275 in reciprocal lattice units (Kuzmany et al., 1978). This is in very good agreement with neutron scattering experiments. The linear relation between charge-transfer and mode shift is confirmed by investigations of mixed crystal systems, such as NMP.,Phen, .%TCNQ. In this system, the charge-transfer is expected to increase linearly with x,since phenazin always remains neutral. This is demonstrated in Fig. 4.8- 16, in which the line position of the C=C stretching mode is plotted versus the NMP concentration in the mixed crystal. Again, the charge-transfer affords the position of the Fermi level. In the resonance Raman spectra of BEDT-TTF, an interesting line was observed around 100 cm-' which could be associated with the symmetric stretch mode of the 1; molecule shown in Fig. 4.8-15. At low temperature, the mode splits into three components, a behavior which has been attributed to crystal field interaction (Swietlik et al., 1987).

1.0E 2

2 n = /2

to outer level adding immediate to SP to same level to outer level ROL - Rotate (not thru Carry) Left reg by 1 memory by 1 1100 1010 : 16-bit displacement 4-13 23

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