Neath Death Brain Activity

7
 Suppo rting Information Borjigin et al. 10.1073/pnas.1308285110 SI Materials and Methods Analysis of Power Spectrum.  The original sampling frequency of 1,000 Hz was down-sampled to 500 Hz to reduce computation time. A notch lter was used to remove the 60-Hz artifact and its possible superharmonics. In Fig. 2, the spectrograms using short- time Fourier transform were calculated based on discrete Fourier transform with 2-s segment size and 1 s overlapping for each frequency bin (0.5250 Hz with 0.5 Hz bin size; spectrogram.m in Mat Lab Sig nal Proces sing Tool box; MathWorks Inc .). Each segment is windowed with a Hamming window. The absolute power was expressed in log scale (Fig. 2  A,  Top and  Middle). The relative power (Fig. 2  B) was calculated at each EEG epoch by dividing the absolute power of each frequency bin with the total power over all frequency bands (0.5250 Hz). Thus, for each EEG epoch, the sum of relative power over all frequency bands should be 100%. The mean and SD of absolute and relative powe rs was cal cul ate d (Fi g. 2  B,  Bottom) for eig ht fre que ncy bands: delta (05 Hz), theta (510 Hz), alpha (1015 Hz), beta (1525 Hz), low gamma (γ1; 2555 Hz), medium gamma (γ2; 80115 Hz), high gamma (or  γ3; 125145 Hz), and ultra gamma (γ4; 165250 Hz). The grouping of the gamma bands into the four fre quency ranges was des igned to avoid the possible art ifa ct contaminations from 60 Hz and its superharmonic. For the mean spectral power, the 10-min-long EEG epochs in the middle of the whole EEG data for waking and anesthesia states, and 20-s- long epochs corresponding to CAS3 state were taken from all rats (  n  = 9). To test the statistical signi cance of the change of spectra l powers across three states, repeat ed-meas ures one-wa y  ANOVA and Bonferronis multicomparison were carried out for the eight frequency bands. The adjusted P  values by Bonfer roni correction are denoted in Fig. 2 (*  P  < 0.05, **  P  < 0.01, ***  P  < 0.001). Analysis of Coherence.  The coherence between EEG channels was measured by amplitude squared coherence  C  xy ð  f Þ  (mscohere.m in MATLAB signal toolbox; MathWorks, Inc.), which is a co- herence estimate of the input signals  x  and  y  using Welchs av- eraged, modi ed periodogram method. The magnitude squared coherence estimate C  xy ð  f Þ  is a function of frequency with values between 0 and 1 that indicates how well  x  corresponds to  y  at each frequency. C  xy ð  f Þ  = j  P  xy ð  f Þj 2  P  xx ð  f Þ  P  yy ð  f Þ ; 0 C  xy ð  f Þ 1;  [1]  where P  xx ð  f Þ  and  P  yy ð  f Þ are the power spectral density of  x  and  y and P  xy ð  f Þ is the cross-power spectrum spectral density. For each rat, the mean coherence among the 15 pairs of six EEG channels  was calculated (Fig. 3  A). Specically, EEG signal was segmented into 2-s epochs with 1 s overlapping over the whole EEG re- cording. The magnitude squared coherence estimate was calcu- lated at each epoch and freque ncy bin (over the freque ncy range of 0.5250 Hz) for each rat. The mean and SD of coherence for six EEG channels were then computed for all rats across the thre e sta tes (wa king, ane sthesia, and CAS3; Fig . 3  B). Again , 10-min-long EEG epochs during waking and anesthesia states and 20-s-long EEG epochs in CAS3 states were taken from nine rats. To test the statistical signicance of the change in coherence across the three states, repeated-measures one-way ANOVA and Bonferronis multicomparison tests were carried out for eight fre- quen cy band s. The adj ust ed P  value s by Bonfer roni correct ion  were denoted in Fig. 3  B (*  P  < 0.05, ***  P  < 0.001). Analysis of Directional Connectivity.  The directional connectivity betwee n EEG channels was measur ed by normali zed symbolic transfe r entropy (NSTE), which is a nonlinear and model-free estimation of directional functional connection based on in- formation theory. STE measures the amount of information provided by the additional knowledge from the past of the source signal  X ð  X  P Þ  in the model describing the information between the past  Y ðY  P Þ  and the future  Y ðY  F Þ  of the target signal  Y , which is dened as follows: STE  X Y  = I  Y  F ; X  P jY  P  = H  Y  F jY  P   H  Y  F j  X  P ; Y  P  ;  [2]  where H ðY  F jY  P Þ is the entropy of the process Y  F , conditional on its past. Each vector for  Y  F ; X  P ; and Y  P is a symbolized vector point. For the appropriate embedding parameters of symbolized  vector, three embedding parametersembeddi ng dimensi on (  d  E ), time delay ( τ), and prediction time (δ )are needed. Here  we selected the paramete r set that provid es the maximum in- formation transfer from the source signal to the target signal as the primary connectivity for a given EEG dataset. By investi- gating the NSTE in the broad parameter space of  d  E  (from 2 to 10) and  τ  (from 1 to 30), we    xed the embedding dimension ð  d  E Þ at 3, which is the smallest dimension providing a similar NSTE, and found the time delay (τ) producing maximum NSTE. In this parameter space, a vector point could cover from 11.7 ms (with  τ = 1 and  d  E  = 3) to 351 ms maximally (with  τ  = 30 and  d  E  = 3). By taking the maximum NSTE as the primary connec- tivity for a given EEG dataset, all other processes are nonpara- metric without subjective decisions for embedding parameters. The prediction time was determined with the time lag (from 1 to 100, 3.9390 ms), resulting in maximum cross-correlation, assuming the time lag as the interaction delay between the source and target signals. Thepote ntial bi asof STE fora gi ven EEG dataset was removed  with a shuf ed data, and the unbiased STE is normalized as follows:  NSTE  X Y  = STE  X Y  − STE Shuffled  X Y  H ðY  F jY  P Þ  ½0; 1;  [3]  where  STE Shuffled  X Y  = H ðY  F jY  P Þ  H ðY  F j  X  P Shuff ; Y  P Þ.  X  P Shuff  is a shuf ed data by replacing the  rst half to the other half of data. STE Shuffled  X Y  estimates a bias generated by characteristic of given EEG data, not by true causality. Therefore, NSTE is normal- ized STE (dimensionless), in which the bias of STE is subtracted from the original STE and then divided by the entropy within the target signal,  H ðY  F jY  P Þ. In EEG connectivity, NSTE represents the fraction of information in the target EEG channel not ex- plained by its own past and explained by the source EEG channel. The feedback and feedforward connectivity between frontal and parietaloccipital EEG channels was dened by averaged NSTE. The feedback connectivity (  NSTE  FB ) was calculated over the eight pairs of EEG channels between the frontal ( f Þchannels and the parietal ( p) and occipital (  o) channels, which is dened as follow s:  NSTE  FB = 1  n  f  ·  n  p X  n  f  ; n  p;  o ði;  jÞ = 1  NSTE i j ;  [4]  where n  f  = 2 and n  po = 4. The feedforward connectivity (  NST E  FB ) from the parietal and occipital channels to the frontal channels Borjigin et al. www.pnas.org/cgi/content/short/130828511 0  1 of 6

description

Near Death Brain activity

Transcript of Neath Death Brain Activity

  • Supporting InformationBorjigin et al. 10.1073/pnas.1308285110SI Materials and MethodsAnalysis of Power Spectrum. The original sampling frequency of1,000 Hz was down-sampled to 500 Hz to reduce computationtime. A notch lter was used to remove the 60-Hz artifact and itspossible superharmonics. In Fig. 2, the spectrograms using short-time Fourier transform were calculated based on discrete Fouriertransform with 2-s segment size and 1 s overlapping for eachfrequency bin (0.5250 Hz with 0.5 Hz bin size; spectrogram.m inMatLab Signal Processing Toolbox; MathWorks Inc.). Eachsegment is windowed with a Hamming window. The absolutepower was expressed in log scale (Fig. 2A, Top and Middle). Therelative power (Fig. 2B) was calculated at each EEG epoch bydividing the absolute power of each frequency bin with the totalpower over all frequency bands (0.5250 Hz). Thus, for eachEEG epoch, the sum of relative power over all frequency bandsshould be 100%. The mean and SD of absolute and relativepowers was calculated (Fig. 2B, Bottom) for eight frequencybands: delta (05 Hz), theta (510 Hz), alpha (1015 Hz), beta(1525 Hz), low gamma (1; 2555 Hz), medium gamma (2; 80115 Hz), high gamma (or 3; 125145 Hz), and ultra gamma (4;165250 Hz). The grouping of the gamma bands into the fourfrequency ranges was designed to avoid the possible artifactcontaminations from 60 Hz and its superharmonic. For the meanspectral power, the 10-min-long EEG epochs in the middle ofthe whole EEG data for waking and anesthesia states, and 20-s-long epochs corresponding to CAS3 state were taken from allrats (n = 9). To test the statistical signicance of the change ofspectral powers across three states, repeated-measures one-wayANOVA and Bonferronis multicomparison were carried out forthe eight frequency bands. The adjusted P values by Bonferronicorrection are denoted in Fig. 2 (*P < 0.05, **P < 0.01, ***P