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where per denotes periodic convolution. If this sequence is sent over a channel with impulse response f, the output of the correlator becomes {f i } = ({b i } per {bi }) {fi }

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The conditions for proper operation of the array are given in the table in Figure 8.34. The erase operation is implemented by biasing the p well 2 at 20 V with the control gates of the memory blocks that are to be erased biased at ground. The source and drain junctions float so that there is no significant potential difference between the well and the source and drain junctions. Consequently, gate-aided breakdown and band-to-band tunneling are of no concern. The control gate lines in the cell stacks that are not to be erased are biased at 20 V so that there are only small potential differences between the floating gates and p

Figure 2.7 illustrates a multi-domain model while Figure 2.8 illustrates a single domain implementation.

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It is remarkable that all instantaneous frequencies in a range to can occur they are not restricted to the range of possible Doppler frequencies! Strong FM most likely occurs in fading dips: if the signal level is low, very strong relative changes can occur. This intuitively pleasing result can be shown mathematically by considering the pdf of the instantaneous frequency conditioned on the amplitude level r0 [Jakes 1974]: pdf ( |r0 ) = r0 2

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