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Physical Four Wire: The most commonsense FDX con guration involves a physical four-wire circuit with one pair of wires supporting transmission in one direction and another pair supporting transmission in the other direction. This approach is commonly used for high-capacity, dedicated circuits, of which most are multichannel in nature. T-carrier and E-carrier circuits traditionally were con gured in this way. All wideband and broadband circuits are FDX in nature. Physical Two Wire: FDX modems use another approach in order to achieve FDX data transmission on a physical two-wire circuit. Modems cause a twowire circuit to emulate a four-wire circuit through a split-channel approach, using Frequency Division Multiplexing (FDM) to create two frequency channels. This process allows the creation of two carrier waves that are then modulated using Frequency Modulation (FM). Figure 6.12 illustrates this technique over a voice-grade circuit. In this example, one channel uses an unmodulated carrier wave at 1170 Hz, modulating it at 1070 Hz to represent 0 bits and at 1270 Hz to represent 1 bits. The reverse channel uses an unmodulated carrier wave at 2125 Hz, modulating it at 2025 Hz to represent 0 bits and at 2225 Hz to represent 1 bits. Other modulation techniques can be used within these channels as well, including AM, PSK, and QAM. Optical: FDX transmission in optical bers is achieved either by using separate bers for transmission in different directions or by using Wavelength Division Multiplexing (WDM), which essentially is FDM at the optical level. POTS: This discussion of FDX begs the question as to how FDX is achieved over a physical two-wire circuit for Plain Old Telephone Service (POTS), that is, analog voice communications, since there is only one voice-grade channel of

Low capacity drift diode Nucl Instrum Methods A 253, 378 381 (1987) 32 Hartmann, R, Hauff, D, Krisch, S, Lechner, P, Lutz, G, Richter, RH, Seitz, H, Str der, L, Bertuccio, G, Fau soli, L, Fiorini, C, Gatti, E, Longoni, A, Pinotti, E and Sampietro, M Design and test at room temperature of the rst silicon drift detector with on-chip electronics IEDM Tech Digest 535 539 (1994) 33 Lechner, P, Pahlke, A and Soltau, H Novel high resolution silicon drift detector X-ray spectrom in press..

CrossReference You ll find more information on user-defined types in 29, Persisting Custom Data Types.

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Along with the improvement of LLD, the standardization of TXRF analysis for semiconductors has been attracting more attention in recent years. On the background of previous two crosscheck works,18,19 ISO/TC201/WG2 was organized to establish international standards of TXRF measurement in 1993, primarily for the semiconductor industry. After an international round-robin test (RRT) and its data analysis, the rst international standard, ISO14706:2000 ( Surface chemical analysis Determination of surface elemental contamination on silicon wafers by total-re ection X-ray uorescence (TXRF) spectroscopy ) was published. The ISO/TC201/WG2 then decided to standardize chemical preconcentration methods for VPD-TXRF as its second major task, and the work started in 1998. This work consisted of two international RRTs. In the rst RRT, the experimental conditions were left to each participant s discretion, which brought about poor interlaboratory reproducibility. The lesson learned from the rst RRT contributed to the conduct of the second RRT. In the second RRT, both the VPD-TXRF and VPD-wet (e.g. ICPMS) methods were tested, and basic experimental conditions and calculation procedures were carefully provided by the organizer. For example, internal addition of V or Sc was applied to normalize the uorescence intensities between different dried residues, and 2 % HF + 2 % H2 O2 was speci ed as the scanning solution. Figure 7.2.10 summarizes the results of the rst and second RRT for Ni.20 The careful control of experimental conditions and calculation procedures in the second RRT accomplished signi cant

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Figure 4.2.13 Calculated energy versus axial distance (every twentieth collision) for a typical single electron drifting in Xe under a reduced electric eld intensity of 0.5 V cm 1 Torr 1 . (Calculations by Barata17 based on Dias et al.,3,18 Dias4,19 and Santos16 )

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