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frequency-dependent features of the antennas [3 6] Therefore, the effects of the transfer function jH(v)j given in Equation (62) on the output signals are evaluated Also, the performance of the antenna systems is measured by pulse delity for the single-band scheme and system transmission ef ciency The received signals, which are transmitted through both narrowband and broadband antenna systems, are compared for the single-band and multiband schemes The source pulses used in Figures 63 and 64 are adopted, respectively The narrowband and broadband antenna systems comprise a pair of thin-wire dipoles and planar square dipoles, which have been used in Figure 65 Figure 68 illustrates the system transfer function jH(v)j and the radiation transfer function jHrad (v)j for the narrowband and broadband antenna systems.

The comparison shows that the broadband antenna system features a atter jH(v)j or Hrad (v)j than the narrowband antenna system within the UWB band Figure 69(a) (c) shows the waveforms of the received signals in the singleband and multiband schemes, when the signals go through the narrowband thinwire dipole system The pulse waveforms illustrated in Figure 69(a) and (b) are not identical with the waveforms of source pulses, even the radiated pulses shown in Figure 66 In the single-band scheme, the severe distortion results mainly from the narrowband ltering of the antenna systems In other words, the dispersion in magnitude and phase of jH(v)j results in the distortion of the pulse waveforms In a multiband scheme, the change in the magnitude of jH(v)j causes the uneven envelope of the magnitudes of the received signals, which accords with the shape of jH(v)j shown in Figure 68.

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Figure 69(c) displays the group delay and the variation in the group delay, which also distort the signals, especially when a large change in the group delay occurs Due to narrowband operation, the.

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The Task Group TG4a has speci ed that the UWB portion of the PHY should be capable of both communications and ranging, and that it should occupy a bandwidth of at least 500 MHz. That would be centered somewhere between 3.85 GHz and 4.05 GHz. Options include two additional 500 MHz bands, an above-6 GHz band with a guaranteed bandwidth of more than 1.5 GHz and possibly a sub-gigahertz band (subject to regulations). The UWB-PHY shall be based upon impulse radio (pulse-shape independent), support different receiver architectures (coherent/ noncoherent), and multiple rates, and support simultaneously operating piconets (SOP).1 On the other hand, the chirp PHY will operate in the 2.45 GHz band but will not be capable of ranging. CSS uses a frequency-modulated pulse. Chirp pulses are robust and can be generated and processed without complex digital circuitry, thereby increasing battery life and reducing costs. Because it works in the 2.45 GHz band, the CSS-PHY can supposedly interoperate with ZigBee devices. On top of that, in contrast to the ZigBee radio s narrowband operation, the CSS operation should provide greater coverage and allow for lower-power operation and for mobility (fast connections) at up to 100 mph.2 As of today, the standard is still under evolution and many technical details of the PHY remain to be xed. Other issues under discussion include common packets for communications and ranging, and support for multiple rates. In the rest of the chapter, we will focus on UWB-PHY since many of the target applications within 802.15.4a require support for ranging and localization. 14.1.3 PHY: 802.15.4a vs 802.15.4

After the buffer has been overflowed, the attacker is in control of the parameters that were passed to the function. Because of this, when the instructions at 0x004011BC perform the *buf = p; operation, we have the possibility of an arbitrary memory overwrite or the chance to cause an access violation. Looking at the latter of these two possibilities, if we overwrite the parameter at EBP + 8 with 0x41414141, then the process will try to write a pointer to this address. Because 0x41414141 is (not normally) initialized memory, then we

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