In Experiment 1, the EEG was recorded from 32 scalp sites according to the international 10–20 system (FP1, FP2, F3, F4, C3, C4, P3, P4, O1, O2, F7, F8, T7, T8, P7, P8, Fz, Pz, Oz, FC1, FC2, CP1, CP2, FC5, FC6, CP5, CP6, TP9, TP10, HLeo, Veo, HReo). Signals were amplified (Brain Products GmbH, Munich, Germany) and sampled at 1000 Hz. The ground electrode was placed at the AFz location, and the on-line reference electrode at the Cz location. Electrode impedances were kept below 5 kΩ.
In Experiment 2, we switched to an active electrodes EEG system. The EEG was recorded from 32 electrodes (actiCAP, Brain Products) at 5000 Hz sampling rate. The ground electrode was placed at FPz, and the on-line reference electrode at FCz location. Electrode impedances were below 25 kΩ (the lowest impedance signaled by the actiCAP system).
Experiment 3 had identical EEG setup, except that only Oz, the ground electrode and the reference electrode were placed on the head. As participants had to wear the Oculus Rift headset, it was not possible to record from more electrodes. We chose to record at Oz, which showed the highest SSVEP responses in Experiments 1 and 2 (
Figure 4; see also Chen, Valsecchi, & Gegenfurtner,
2017a,
2017b). Note that the VR headset inevitably causes some additional baseline noise in EEG signals. It is, however, less of a problem for the present study, as we measured the amplitude of responses at the stimulus frequency relative to the background noise assessed at nearby frequency bins. The SSVEP technique has been successfully used in VR, mostly for brain computer interfaces (Royer, Doud, Rose, & He,
2010; see Kerouš & Liarokapis,
2016, for a recent review).
Analyses were carried out using EEGLAB toolbox (Delorme & Makeig,
2004) and customized scripts in MATLAB (MathWorks). EEG signals were re-referenced to a common average reference in Experiments 1 and 2 (in Experiment 3, re-referencing was not possible because only Oz electrode was recorded). EEG epochs lasting 5 s (corresponding to a flickering stimulus with a certain size) were cut out. Each epoch was first de-trended by removing the linear fit (Bach & Meigen,
1999), and multiplied by a Tukey window (i.e., tapered cosine window, alpha = 0.2). Fast Fourier transform (
fft.m in MATLAB) was used to obtain the amplitude spectrum. At each frequency (e.g., 8 Hz), we subtracted from the peak amplitude the average amplitude of the four nearby bins (e.g., 7.6, 7.8, 8.2, 8.4 Hz), so that the background noise was removed (e.g., Liu-Shuang, Torfs, & Rossion,
2016). To calculate the total SSVEP amplitude, we summed all harmonics below 45 Hz. Note that including harmonics without significant powers would not change the result, as their amplitudes were close to zero after subtracting the background noise. All the SSVEP analyses were identical in all three experiments, except that we did not include the second harmonic (i.e., 10 Hz) of the 5 Hz stimulus in Experiment 3. The reason was that 10 Hz lies exactly at the peak of spontaneous alpha oscillations, which tends to increase throughout the experiment as participants get tired. The main results remained unchanged regardless of whether the 10 Hz harmonic was included or not. For analyses of SSVEP phases we used the circular statistic toolbox in MATLAB (Berens,
2009).
SSVEP amplitudes differ largely between the central and peripheral visual field, between different frequencies, and across participants. We used standard procedures to normalize the amplitudes (Andersen, Fuchs, & Müller,
2011; Andersen, Müller, & Hillyard,
2015), by transforming them into z scores for each participant, separately for locations in visual field (Experiment 1) and separately for each stimulus frequency (Experiment 2). We excluded data points with z scores exceeding the range of [-2.5, 2.5] (0.59% of total trials for Experiment 1; 0.67% for Experiment 2; 0.97% for Experiment 3). Results were similar regardless of whether outliers were removed or not. In Experiments 1 and 2, the average amplitudes at O1, Oz, and O2 electrodes were used for statistics, as the SSVEP responses were confined to these electrodes (
Figure 4). In Experiment 3, the amplitudes at Oz were used, which was the only electrode recorded.
In all figures in the results, we report
within-subject confidence intervals calculated with the method provided by Cousineau (
2005), as between-subject variability measurements are misleading for a within-subject design such as the current study.