This figure shows velocity perturbations relative to a 1-D starting model
on a pseudo-plane parallel to the seafloor at a depth of 3 km. The
four plots below correspond to the regions boxed in blue. For each plot,
the "footprint" of the velocity anomaly was measured at a range of
depths. These values can be thought of as the area contained within
contours exceeding the stated threshold. The size of each anomaly is
plotted as a function of depths.
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The three plots above span (left) a 10km x 10km box around the caldera anomaly, (middle) a similar box around the east flank low velocity zone, and (right) a larger box which essentially sums the two regions together.
The very low velocity anomalies (< -1 km/s) peak at about 2.8 km below
seafloor. This is the most likely center of the magma chamber. Below 3
kilometers, the area of these anomalies drops off. At depth, there is
little of this material left. However, the region of "mild" low
velocities (< -0.5 km/s) is quite large in the lower crust. There is no
appearent bottom on this feature. One explanation for this is that
transient or diffuse magma is sourced through the lower crust. It is
never in great enough quantities to depress seismic velocities much more
than 0.5 km/s however. In the mid-crustal magma chamber centered on 2.7
km, this melt collects. Pooling magma increases the partial melt
fraction enough to create a siginificant seismic signature exceeding -1-2
km/s. The small amount of low velocity material in the upper crust may
be remnant melt from recent eruptions or weakened rock from hydrothermal
cracking. The latter interpretation is also supported by the lack of low
velocities immediately above the magma chamber at a depth of 2.0 km.
Fluid may not be able to penetrate this region due to its depth or
perhaps the extreme heat.

http://www.ldeo.columbia.edu/~mwest/AX/F/areas