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Continue scanning over the enclosure surface concentrating near suspected seams, joints, openings, or I/O interconnects and their attached cables Calculate wavelength from frequency ( = C/f ) and physically measure all seams and potential antenna structures that are roughly either a half-wavelength or quarter-wavelength dimension based on this equation Write down the relative levels from each source using a constant measurement distance from each radiating source The highest level provides a starting point as to the potential location of the enclosure leak point If the highest reading is from a wire or cable, use a current clamp to measure the noise current on it The radiated field is directly proportional to this current level If one needs a 6-dB reduction, current in the cable must be reduced by 6 dB.

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HIGH HARMONIC GENERATION recently Rose-Petruck et al. used ultrashort X-ray pulses to measure the response of a GaAs crystal to a sudden heating. The material is heated up so rapidly that no notable expansion can take place. The impulsive heat deposition launches an acoustic wave that travels into the material forming regions of compression and expansion. The lattice dynamics was characterized by observing the temporal evolution of the Bragg diffraction line. In this experiment sub-picosecond temporal and sub-milliangstrom spatial resolution has been demonstrated. After these rst pioneering experiments time-resolved X-ray diffraction has been used to characterize non-thermal melting (Siders et al., 1999; Rousse et al., 2001a), acoustic transients in solids (Sokolowski-Tinten et al., 2001), and solid solid phase transitions (Cavalleri et al., 2001). These experiments clearly demonstrate the impressive potential of table-top picosecond X-ray sources and brings us closer to the goal of watching, on femtosecond time scales, so called molecular movies.

2.370 (0.01) 2.130 (0.02) 1.804 (0.05) 1.555 (0.10) 1.414 (0.15) 1.311 (0.20) 1.234 (0.25)

Because the source of the RF noise is usually generated internal to the enclosure, further near-field probing may be performed on inside wires, traces, or components on various PCBs If excessive radiation is measured directly on the PCB, this may indicate poor layout, trace routing, or decoupling With near-field probing, one will generally observe RF noise only when physically close to the source It must be kept in mind that near-field readings are dependent upon the nature of the source, its geometry, and its properties There will be no correlation between near-field and far-field measurement Near-field measurements are a means of identifying the source of the noise Small movements of a near-field.

Indexing for improving performance Interpreting query execution plans A database strategy for improving performance

On (-ca, and on (z1,m), we expect the likelihood ratios to be constant, and we zo) try densities of the form

v (n1) = 0 1 2 3 4 5 6

Figure 6.5 shows an example of a type-l decomposition. Type-2. The decomposition into type-2 polyphase components is given by

INDEX IEEE 802.11b model, 216 218 IEEE 802.11 MIMO model, 233 234 interarrival delays, 224 JTC model, 214 215, 272 274 Poisson distribution model, 220 222 Poisson model, modi ed, 222 224 Saleh-Valenzuela model, 218 219, 233 Spencer model for AOA, 232 233 Suzuki model, 221 Path loss modeling: IEEE 802.15 WPAN models, 589 590 Intel model for UWB, 588 589 JTC, 103 108 macrocell, 107 109 microcell, 107 109 mobile radio, 59 60 partitioned indoor, 105 107 Personal communication services (PCS): comparison with cellular, 36 CT-2, 27, 679 DCS-1800, 27 DECT, 680 overview, 36 37 table of standards, 36 Phase locked loop, 331 Physical operating environment: indoor commercial, 81 indoor of ce, 62, 81 indoor residential, 81, 83 outdoor residential, 82 outdoor urban high-rise, 82, 83 outdoor urban/suburban low-rise, 82, 83 table of Doppler shift ranges, 83 Picocells, 508 Polling, 532 Positioning, see RF location sensing Probability of outage: for erfc error functions, 345 for exponential error functions, 345 for MRC, 351 Propagation in free space, 57 Pseudonoise (PN) sequence in DS-CDMA, 477 Pulse shaping, 332 335 Raised cosine lter, 333 RAKE receiver: in IS-95, 453 performance, 453 464 structure, 451 452 RAM mobile, see Mobitex Random access methods: ALOHA-based, 539 547 CSMA-based, 547 560 DSMA, 547, 552 throughput comparisons, 549 551 Ray tracing: computation time, 264 diffraction coef cient, 253 254

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