Compressive Sensing system for recording of ECoG signals in-vivo
Compressive Sensing system for recording of ECoG signals in-vivo
Compressive Sensing system for recording of ECoG signals in-vivo
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and <strong>in</strong>terleave these outputs with the others <strong>in</strong> order to ma<strong>in</strong>ta<strong>in</strong> the largest distance betweenthe FFs which are <strong>in</strong>volved, <strong>for</strong> <strong>in</strong>stance, that means not considered as successive outputs bit 3<strong>in</strong> 4FF-PRBS and bit 1 <strong>in</strong> 5FF-PRBS <strong>for</strong> the output i, and bit 4 <strong>in</strong> 4FF-PRBS and bit 2 <strong>in</strong> 5FF-PRBS <strong>for</strong> the output i + 1, because this choice <strong>in</strong>troduced correlation <strong>in</strong> that fragment <strong>of</strong> randomsequence.Figure 4.1.3.2. Serial Implementation with two PRBS (4-FF and 5-FF) to obta<strong>in</strong> 16 outputs.In 4.1.3 it is studied the randomness <strong>of</strong> this model, because, as the XOR<strong>in</strong>g cross<strong>in</strong>g has beenexploited as much as possible to maximize the number <strong>of</strong> outputs per pair <strong>of</strong> PRBScomb<strong>in</strong>ation, the model shows fragments <strong>in</strong> some <strong>of</strong> the states are shifted versions <strong>of</strong> previousstates. In spite <strong>of</strong> the partial correlation which exist between successive outputs <strong>of</strong> the mixedrandom generator, regard<strong>in</strong>g how the random values are provided to the measurement matrixand by consider<strong>in</strong>g that each <strong>of</strong> the outputs <strong>of</strong> this matrix generator block supplies a column <strong>of</strong>the measurement matrix at each <strong>in</strong>tegration period (see Fig. 4.1.3.3), the correlation betweenthe generated sequences <strong>in</strong> this design does not affect the per<strong>for</strong>mance <strong>of</strong> the reconstructionbecause the similarity periods do not occur simultaneously and they are shifted <strong>in</strong> time. ThisPRBS has been implemented <strong>for</strong> different dimensions <strong>of</strong> the measurement matrix <strong>in</strong> Cadenceand it is considered <strong>in</strong> the CS operation along the next chapters.44Figure 4.2.3.3. Random states propagation by columns to the measurement matrix.