The presence of the SWIFT, SSVEP, and IM signals was confirmed by the respective SNR that differed significantly from 1 (see
Figure 4).
Table 1 shows the results of the one-tailed
t-tests for all frequency bins of interest. The fundamental frequency of the SSVEP signal (
f3 = 12.5 Hz) showed the highest SNR, followed by its first harmonic, 2
f3 = 25 Hz. The two fundamental SWIFT frequencies were clearly detectable (
f1 = 0.8 Hz and
f2 = 1 Hz), as well as their first-order harmonics (2
f1 = 1.6 and 2
f2 = 2 Hz). The harmonics of
f1 = 0.8 Hz were continually detectable up to the sixth-order harmonic: 6
f1 = 4.8 Hz;
M = 1.46; 99% CI, 1.25–infinity;
t(19) = 5.47, FDR-adjusted
p < 0.01. However, the harmonics of
f2 = 1 Hz were detectable up to the eighth-order harmonic: 8
f2 = 8 Hz;
M = 1.34; 99% CI, 1.22–infinity;
t(19) = 7.12; FDR-adjusted
p < 0.001. There were more higher order harmonics with an SNR greater than 1 that are not reported here (for more extensive
t-test data, see
Supplementary Table S1). The signal of the four first-order IM frequencies also differed from 1 (
f3 −
f2 = 11.5 Hz,
f3 −
f1 = 11.7 Hz,
f3 +
f1 = 13.3 Hz,
f3 +
f2 = 13.5 Hz; all FDR-adjusted
p < 0.01). The same applied for three of four second-order IM frequencies (
f3 − 2
f1 = 10.9 Hz,
f3 + 2
f1 = 14.1 Hz,
f3 + 2
f2 = 14.5 Hz; all FDR-adjusted
p < 0.01). Only one second order IM component did not differ from 1 (
f3 – 2
f2 = 10.5 Hz; FDR-adjusted
p = 0.27). The linear combination of the two SWIFT frequencies (
f1 +
f2 = 1.8 Hz) also did not show an SNR greater than 1 (FDR-adjusted
p = 1.00).