Noninvasive Measurement of Conductivity Anisotropy at Larmor Frequency Using MRI

<div class="floats-full-page floats-full-page-figure"><h2>Figure 1</h2><div class="floats-full-page-caption"><table> (a) Numerical phantom with anisotropic effective admittivity by stacking periodic binary medium, (b) placement of the imaging object inside the RF coil.</table></div><div class="floats-full-page-content"><table class="table-group" width="800px"><tr class="fig-image" id="a"><td><img alt="421619.fig.001a" src="https://static-01.hindawi.com/articles/cmmm/volume-2013/421619/figures/421619.fig.001a.jpg" /></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(a) </b></td></tr></table></td></tr><tr class="fig-image" id="b"><td><img alt="421619.fig.001b" src="https://static-01.hindawi.com/articles/cmmm/volume-2013/421619/figures/421619.fig.001b.jpg" /></td></tr><tr class="fig-caption"><td align="center"><table><tr><td><b>(b) </b></td></tr></table></td></tr></table></div></div>

Figure 1 | Noninvasive Measurement of Conductivity Anisotropy at Larmor Frequency Using MRI

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Figure 1: Noninvasive Measurement of Conductivity Anisotropy at Larmor Frequency Using MRI

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Figure 1

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