Radio frequency magnetic field mapping of a 3 Tesla birdcage coil: Experimental and theoretical dependence on sample properties

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Abstract

<jats:title>Abstract</jats:title><jats:p>The RF <jats:italic>B</jats:italic><jats:sub>1</jats:sub> distribution was studied, theoretically and experimentally, in phantoms and in the head of volunteers using a 3 T MRI system equipped with a birdcage coil. Agreement between numerical simulation and experiment demonstrates that <jats:italic>B</jats:italic><jats:sub>1</jats:sub> distortion at high field can be explained with 3D full‐Maxwell calculations. It was found that the <jats:italic>B</jats:italic><jats:sub>1</jats:sub> distribution in the transverse plane is strongly dependent on the dielectric properties of the sample. We show that this is a consequence of RF penetration effects combined with RF standing wave effects. In contrast, along the birdcage coil z‐axis the <jats:italic>B</jats:italic><jats:sub>1</jats:sub> distribution is determined mainly by the coil geometry. In the transverse plane, the region of <jats:italic>B</jats:italic><jats:sub>1</jats:sub> uniformity (within 10% of the maximum) was 15 cm with oil, 6 cm with distilled water, 11 cm with saline, and 10 cm in the head. Along z the <jats:italic>B</jats:italic><jats:sub>1</jats:sub> uniformity was 9 cm with phantoms and 7 cm in the head. Magn Reson Med 46:379–385, 2001. © 2001 Wiley‐Liss, Inc.</jats:p>

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