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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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frequency when all the electrodes are scanned, solely a few <strong>of</strong> them will detect a spike. If atsampl<strong>in</strong>g frequency it is created a vector conta<strong>in</strong><strong>in</strong>g what each <strong>of</strong> the electrodes captures <strong>in</strong> thatclock cycle, that vector most probably will be sparse as well, and so it can be compressed byapply<strong>in</strong>g CS. By repeat<strong>in</strong>g this operation dur<strong>in</strong>g all the acquisition time (N samples), N vectorswill be composed, each <strong>of</strong> them with M measurements. In Fig.5.2.1 it is sketched the SCSconception <strong>for</strong> the first clock time multielectrode acquisition, which leads to a spatially collectedsparse signal. When acquisition time is completed, orig<strong>in</strong>al <strong>signals</strong> can be reconstructed byrevers<strong>in</strong>g the operation dur<strong>in</strong>g the <strong>of</strong>f-l<strong>in</strong>e signal process<strong>in</strong>g.Figure 5.2.1. Spatial CS example. The composition <strong>of</strong> the first sample <strong>of</strong> all <strong>of</strong> the electrodes gives rise toa sparse signal.If spatial sparsity is guaranteed, several benefits arise from SCS, without apply<strong>in</strong>g threshold<strong>in</strong>gor signal-dependent pre-process<strong>in</strong>g neural <strong>signals</strong> can be recovered by achiev<strong>in</strong>g a largerCompression Ratio, because <strong>signals</strong> <strong>of</strong> length N can be recovered by M measurements, thelatter one depend<strong>in</strong>g on the number <strong>of</strong> electrodes <strong>of</strong> the array. Similarly, the new compactrandom generator which is <strong>in</strong>cluded <strong>in</strong> Chapter 4 can be used without eventual drawbacks <strong>of</strong>correlation between paths, because each <strong>of</strong> the samples <strong>of</strong> a signal is <strong>in</strong>volved <strong>in</strong> a different CSspatial operation.As <strong>in</strong> 5.1., the reconstruction methods which have been considered <strong>in</strong> order to test this new CSapproach have been the ones based on SPGL1 [30], (see 5.3). In Fig.5.2.2 it can be observedthe orig<strong>in</strong>al and reconstructed <strong>signals</strong> <strong>in</strong> 10 ms <strong>for</strong> two sample channels us<strong>in</strong>g MATLAB andcircuit simulations, which has been <strong>in</strong>cluded <strong>in</strong> [31].51

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