This analysis served to show that the statistical Session × Valence buy Nutlin-3a interaction was actually driven by differences in post-conditioning

CS processing attributable to affective conditioning effects, as opposed to pre-existing baseline differences. Based upon the theoretical account of a role of the right hemisphere in withdrawal-related, and the left hemisphere in approach-related, behaviour (Davidson, 1992; Davidson & Irwin, 1999), we expected hemispheric asymmetries in CS+ and CS− processing. To demonstrate asymmetries between hemispheres, it is obligatory to test not only for effects within corresponding regions in left and right hemisphere separately but to calculate the statistical interaction across hemispheres for this effect (Davidson & Irwin, 1999; Pizzagalli et al., 2003). To statistically test for differential CS processing across hemispheres, mirror-symmetric sensor groups were selected in the opposite hemisphere find more and submitted to a three-way repeated-measures anova including the factor Hemisphere (cf.

Davidson & Irwin, 1999). The analysis of sensor space data can be used to determine systematic differences of neural activity between experimental conditions in target AEF components. However, the localisation of the underlying neural sources generating such differences cannot be simply deduced from the measured field topographies. To estimate the cortical sources of the AEFs in the present study, we applied the L2-minimum-norm-pseudoinverse (L2-MNP) method. This inverse source modelling technique allows the estimation of distributed neural network activity as recorded by modern whole-head MEG scanners without a priori assumptions regarding the location

and/or number of current sources (Hämäläinen & Ilmoniemi, 1994). In addition, from all possible generator sources only those exclusively determined by the measured magnetic fields are considered by the method (Hauk, 2004). A spherical shell with evenly distributed 2 (azimuthal and polar direction; radial dipoles do not generate magnetic fields outside a sphere) × 350 dipoles was used as source model. A source shell radius of 87% of the individually fitted head radius oxyclozanide has been chosen, roughly corresponding to the grey matter volume. Across all participants and conditions, a Tikhonov regularisation parameter k of 0.02 was applied. Although this distributed source reconstruction in MEG does not give the precise location of cerebral generators, it allows for a fairly good approximation of cortical generators and corresponding assignment to larger cortical structures. To promote better intelligibility, L2-MNP topographic maps were projected onto a realistic brain geometry. Topographies of source direction-independent neural activities, i.e.