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. Author manuscript; available in PMC: 2012 Sep 1.
Published in final edited form as: J Magn Reson. 2011 Jun 25;212(1):116–123. doi: 10.1016/j.jmr.2011.06.016

Figure 1.

Figure 1

Geometry of the Six-Point-Sample (3-D) Phantom. The time-dependent frequency shift between a pair of point solvents aligned along a given principal axis is used to monitor the time-dependent, eddy-current-induced gradients in that direction.