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Mathematics in Independent Component Analysis

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218 Chapter 15. Neurocomput<strong>in</strong>g, 69:1485-1501, 2006<br />

<strong>in</strong>troduced by the statistical analysis procedure, hence denois<strong>in</strong>g deemed necessary.<br />

The algorithms discussed above have been applied to an experimental 2D Nuclear<br />

Overhauser Effect Spectroscopy (NOESY) proton NMR spectrum of the<br />

polypeptide P11 dissolved <strong>in</strong> water. The synthetic peptide P11 consists of 24<br />

am<strong>in</strong>o acids only and represents the helix H11 of the human Glutathion reductase<br />

[21]. A simple pre-saturation of the water resonance was applied to prevent<br />

saturation of the dynamic range of the Analog Digital Converter (ADC).<br />

Every data set comprises 512 Free Induction Decays (FIDs) S(t1, t2) ≡ xn[l]<br />

or their correspond<strong>in</strong>g spectra ˆ S(11, ω2) ≡ ˆxn[l], with L = 2048 samples each,<br />

which correspond to N = 128 evolution periods t1 ≡ [n]. To each evolution<br />

period belong four FIDs with different phase modulations, hence only FIDs<br />

with equal phase modulations have been considered for analysis. A BSS analysis,<br />

us<strong>in</strong>g both the algorithm GEVD us<strong>in</strong>g Matrix Pencil (GEVD-MP) [28]<br />

and the algorithm dAMUSE [33], was applied to all data sets. Note that the<br />

matrix pencil with<strong>in</strong> GEVD-MP was conveniently computed <strong>in</strong> the frequency<br />

doma<strong>in</strong>, while <strong>in</strong> the algorithm dAMUSE <strong>in</strong> spite of the filter<strong>in</strong>g operation<br />

be<strong>in</strong>g performed <strong>in</strong> the frequency doma<strong>in</strong>, the matrix pencil was computed <strong>in</strong><br />

the time doma<strong>in</strong>. The GEVD is performed <strong>in</strong> dAMUSE as described above to<br />

achieve a dimension reduction and concomitant denois<strong>in</strong>g.<br />

4.3.1 Local ICA denois<strong>in</strong>g<br />

For denois<strong>in</strong>g we first used the LICA denois<strong>in</strong>g algorithm proposed above<br />

to enhance the reconstructed prote<strong>in</strong> signal without the water artifact. We<br />

applied the denois<strong>in</strong>g only to those components which were identified as water<br />

components. Then we removed the denoised versions of these water artifact<br />

components from the total spectrum. As a result, the additional noise is at<br />

least halved as can also be seen from figure 7. On the part of the spectrum<br />

away from the center, i.e. not conta<strong>in</strong><strong>in</strong>g any water artifacts, we could estimate<br />

the <strong>in</strong>crease of the SNR with the orig<strong>in</strong>al spectrum as reference. We calculated<br />

a SNR of 17.3 dB of the noisy spectrum and a SNR of 21.6 dB with apply<strong>in</strong>g<br />

the denois<strong>in</strong>g algorithm.<br />

We compare the result, i.e. the reconstructed artifact-free prote<strong>in</strong> spectrum of<br />

our denois<strong>in</strong>g algorithm to the result of a KPCA based denois<strong>in</strong>g algorithm<br />

us<strong>in</strong>g a gaussian kernel <strong>in</strong> figure 8. The figure depicts the differences between<br />

the denoised spectra and the orig<strong>in</strong>al spectrum <strong>in</strong> the regions where the water<br />

signal is not very dom<strong>in</strong>at<strong>in</strong>g. As can be seen, the LICA denois<strong>in</strong>g algorithm<br />

reduces the noise but does not change the content of the signal, whereas the<br />

KPCA algorithm seems to <strong>in</strong>fluence the peak amplitudes of the prote<strong>in</strong> resonances<br />

as well. Further experiments are under way <strong>in</strong> our laboratory to <strong>in</strong>vestigate<br />

these differences <strong>in</strong> more detail and to establish an automatic artifact<br />

21

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