def test_filterfit(self): """Test function filterfit.""" p = EventRelatedPac() x_pha = np.random.rand(100, 1000) x_amp = np.random.rand(100, 1000) p.filterfit(256, x_pha, x_amp=x_amp, method='circular') p.filterfit(256, x_pha, x_amp=x_amp, method='gc')
def test_fit(self): """Test function fit.""" data = np.random.rand(100, 1000) p = EventRelatedPac() pha = p.filter(256, data, 'phase') amp = p.filter(256, data, 'amplitude') p.fit(pha, amp, method='circular') p.fit(pha, amp, method='gc')
def test_fit(self): """Test function fit.""" data = np.random.rand(100, 1000) p = EventRelatedPac() pha = p.filter(256, data, 'phase') amp = p.filter(256, data, 'amplitude') p.fit(pha, amp, method='circular') p.fit(pha, amp, method='gc') p.fit(pha, amp, method='gc', n_perm=2) p.fit(pha, amp, method='gc', smooth=5) p.surrogates, p.pvalues
def test_functional_erpac(self): """Test function test_functional_pac.""" # erpac simultation n_epochs, n_times, sf, edges = 400, 1000, 512., 50 x, times = pac_signals_wavelet(f_pha=10, f_amp=100, n_epochs=n_epochs, noise=.1, n_times=n_times, sf=sf) times = times[edges:-edges] # phase / amplitude extraction (single time) p = EventRelatedPac(f_pha=[8, 12], f_amp=(30, 200, 5, 5), dcomplex='wavelet', width=12) kw = dict(n_jobs=1, edges=edges) phases = p.filter(sf, x, ftype='phase', **kw) amplitudes = p.filter(sf, x, ftype='amplitude', **kw) n_amp = len(p.yvec) # generate a normal distribution gt = np.zeros((n_amp, n_times - 2 * edges)) b_amp = np.abs(p.yvec.reshape(-1, 1) - np.array([[80, 120]])).argmin(0) gt[b_amp[0]:b_amp[1] + 1, :] = True plt.figure(figsize=(16, 5)) plt.subplot(131) p.pacplot(gt, times, p.yvec, title='Ground truth', cmap='magma') for n_meth, meth in enumerate(['circular', 'gc']): # compute erpac + p-values erpac = p.fit(phases, amplitudes, method=meth, mcp='bonferroni', n_perm=30).squeeze() pvalues = p.pvalues.squeeze() # find everywhere erpac is significant + compare to ground truth is_signi = pvalues < .05 erpac[~is_signi] = np.nan # computes accuracy acc = 100 * (is_signi == gt).sum() / (n_amp * n_times) assert acc > 80. # plot the result title = f"Method={p.method}\nAccuracy={np.around(acc, 2)}%" plt.subplot(1, 3, n_meth + 2) p.pacplot(erpac, times, p.yvec, title=title) plt.tight_layout() plt.show()
# Second signal : one second of random noise x2 = np.random.rand(n_epochs, 1000) # now, concatenate the two signals across the time axis x = np.concatenate((x1, x2), axis=1) time = np.arange(x.shape[1]) / sf ############################################################################### # Define an ERPAC object and extract the phase and the amplitude ############################################################################### # use :class:`tensorpac.EventRelatedPac.filter` method to extract phases and # amplitudes # define an ERPAC object p = EventRelatedPac(f_pha=[9, 11], f_amp=(60, 140, 5, 1)) # method for correcting p-values for multiple comparisons mcp = 'bonferroni' # extract phases and amplitudes erpac = p.filterfit(sf, x, method='circular', mcp=mcp).squeeze() # get the p-values and squeeze unused dimensions pvalues = p.pvalues.squeeze() # set to nan everywhere it's not significant erpac[pvalues > .05] = np.nan vmin, vmax = np.nanmin(erpac), np.nanmax(erpac) p.pacplot(erpac, time, p.yvec,
# an alpha <-> gamma coupling. This peak is essentially comprised between # [8, 12]Hz. This range of frequencies is then gonig to be used to see if there # is indeed an alpha <-> gamma coupling (Aru et al. 2015 # :cite:`aru2015untangling`) ############################################################################### # Compute and plot the Event-Related PAC ############################################################################### # To go one step further we can use the Event-Related PAC (ERPAC) in order to # isolate the gamma range that is coupled with the alpha phase such as when, in # time, this coupling occurs. Here, we compute the ERPAC using the # Gaussian-Copula mutual information (Ince et al. 2017 # :cite:`ince2017statistical`), between the alpha [8, 12]Hz and several gamma # amplitudes, at each time point. rp_obj = EventRelatedPac(f_pha=[8, 12], f_amp=(30, 160, 30, 2)) erpac = rp_obj.filterfit(sf, data, method='gc', smooth=100) ############################################################################### plt.figure(figsize=(8, 6)) rp_obj.pacplot(erpac.squeeze(), times, rp_obj.yvec, xlabel='Time', ylabel='Amplitude frequency (Hz)', title='Event-Related PAC occurring for alpha phase', fz_labels=15, fz_title=18) add_motor_condition(135, color='white') plt.show()
def test_filter(self): """Test function filter.""" data = np.random.rand(7, 1000) p = EventRelatedPac() p.filter(256, data, 'phase') p.filter(256, data, 'amplitude')
plt.rc('font', family=cfg["font"]) ############################################################################### n_epochs = 300 n_times = 1000 sf = 1000. ############################################################################### x1, tvec = pac_signals_wavelet(f_pha=10, f_amp=100, n_epochs=n_epochs, noise=2, n_times=n_times, sf=sf) x2 = np.random.rand(n_epochs, 1000) x = np.concatenate((x1, x2), axis=1) time = np.arange(x.shape[1]) / sf p = EventRelatedPac(f_pha=[9, 11], f_amp='hres') pha = p.filter(sf, x, ftype='phase', n_jobs=-1) amp = p.filter(sf, x, ftype='amplitude', n_jobs=-1) plt.figure(figsize=(14, 6)) for n_m, (method, nb) in enumerate(zip(['circular', 'gc'], ['A', 'B'])): # to be fair with the comparison between ERPAC and gcERPAC, the smoothing # parameter of the gcERPAC is turned off but results could look way better # if for example with add a `smooth=20` erpac = p.fit(pha, amp, method=method, n_jobs=-1).squeeze() plt.subplot(1, 2, n_m + 1) p.pacplot(erpac, time, p.yvec, xlabel='Time (second)', cmap=cfg["cmap"], ylabel='Frequency for amplitude (Hz)', title=p.method, vmin=0., rmaxis=True, fz_labels=20, fz_title=22, fz_cblabel=20) plt.axvline(1., linestyle='--', color='w', linewidth=2) if n_m == 1: plt.ylabel('')
from tensorpac import EventRelatedPac import matplotlib.pyplot as plt import seaborn as sns plt.style.use('seaborn-poster') sns.set_style("white") plt.rc('font', family=cfg["font"]) # erpac simultation n_epochs, n_times, sf, edges = 400, 1000, 512., 50 x, times = pac_signals_wavelet(f_pha=10, f_amp=100, n_epochs=n_epochs, noise=.1, n_times=n_times, sf=sf) times = times[edges:-edges] # phase / amplitude extraction (single time) p = EventRelatedPac(f_pha=[8, 12], f_amp=(30, 200, 5, 5), dcomplex='wavelet', width=12) kw = dict(n_jobs=1, edges=edges) phases = p.filter(sf, x, ftype='phase', **kw) amplitudes = p.filter(sf, x, ftype='amplitude', **kw) n_amp = len(p.yvec) # generate a normal distribution gt = np.zeros((n_amp, n_times - 2 * edges)) b_amp = np.abs(p.yvec.reshape(-1, 1) - np.array([[80, 120]])).argmin(0) gt[b_amp[0]:b_amp[1] + 1, :] = True plt.figure(figsize=(16, 5)) plt.subplot(131) p.pacplot(gt, times, p.yvec, title='Ground truth', cmap='magma') for n_meth, meth in enumerate(['circular', 'gc']): # compute erpac + p-values