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. 2010 Dec 8;2011:891585. doi: 10.1155/2011/891585

Figure 2.

Figure 2

The diffeomorphic flow exp (D) associated to the vector field D is the solution at time t = 1 on the trajectory tangent to D at each point (here represented in 2D). We see that the motion of x induced by exp (D)(x) is more compatible with V than this produced by Δ(x) = x + D(x).