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Mirror-touch synaesthesia: the role of shared ... - UCL Discovery

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115<br />

Chapter 6<br />

overall duration <strong>of</strong> roughly 1 ms (Figure 6.1). The extent to which <strong>the</strong> resulting TMS<br />

pulse disrupts neural processing in <strong>the</strong> targeted area depends on <strong>the</strong> orientation <strong>of</strong> <strong>the</strong><br />

coil and <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> underlying nerve fibres (Amassian, Eberle, Maccabee,<br />

and Cracco, 1992). If <strong>the</strong> induced field is uniform across <strong>the</strong> cell membrane <strong>the</strong>n no<br />

current will be induced. The TMS effects are optimised when <strong>the</strong> electric field is<br />

tangential to <strong>the</strong> orientation <strong>of</strong> <strong>the</strong> nerve fibre ei<strong>the</strong>r due to <strong>the</strong> electric field<br />

orientation being perpendicular to a straight axon or an axon bending relative to <strong>the</strong><br />

orientation <strong>of</strong> <strong>the</strong> induced field (Figure 6.2).<br />

Two types <strong>of</strong> coils are typically used in TMS studies. They are <strong>the</strong> figure-<strong>of</strong>-<br />

eight and circular coils (Figure 6.3). All <strong>of</strong> <strong>the</strong> studies reported in this <strong>the</strong>sis use a<br />

figure-<strong>of</strong>-eight coil, which has been shown to produce <strong>the</strong> most focal effects <strong>of</strong> TMS<br />

(Ueno, Tashiro, and Harada, 1988). In <strong>the</strong> figure-<strong>of</strong>-eight coil, current flows in<br />

opposite directions around each <strong>of</strong> <strong>the</strong> windings and converges on <strong>the</strong> centre point <strong>of</strong><br />

<strong>the</strong> coil where <strong>the</strong> electrical currents summate. This leads to focal neural stimulation<br />

with <strong>the</strong> largest effect occurring in <strong>the</strong> cortex situated directly under <strong>the</strong> centre-point<br />

<strong>of</strong> <strong>the</strong> coil. Because <strong>the</strong> outer-windings <strong>of</strong> <strong>the</strong> coil are away from <strong>the</strong> surface <strong>of</strong> <strong>the</strong><br />

scalp <strong>the</strong>y are unlikely to induce an additional disruptive magnetic field. The<br />

stimulation effects dissipate gradually as distance from <strong>the</strong> maximal point increases<br />

(Figure 6.3).

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