We discuss a new method for seismically imaging mantle plumes by model
ing the plume as a,vertical elastic cylinder and analyzing the effects
of the cylinder on an incoming teleseismic plane wave. The incident p
lane wave decomposes into cylindrical waves for which the scattering c
oefficients can be computed by imposing continuity of stress and displ
acement at the cylinder boundary. We extended this development to cyli
nders with gradational boundaries by numerically integrating the elast
o-dynamic equations. Synthetic seismograms calculated using this techn
ique for a cylinder with. a range of parameters appropriate for a mid-
Pacific mantle plume (epicentral distance Delta 50 degrees-90 degrees,
Delta T = 200-400 K, boundary width 0-60 km) have the following chara
cteristics: (1) a delay of the P wave arrival for an observational poi
nt directly behind the plume, (2) the focusing of energy into the regi
on directly behind the plume where the focal length is similar to 2 ti
mes the plume diameter, and (3) the presence of secondary phases, and
especially the excitation of a transverse component whose amplitude is
up to 25% of the radial amplitude. Most of the phases arise from P-to
-S conversions and reflections at the boundary of the cylinder. Increa
sing the epicentral distance reduces the focal length and strengthens
the focusing effect for receivers near the plume. Increasing the therm
al anomaly reduces both the focal length and the amplitude of the seco
ndary phases. Using gradational boundaries does not affect the scatter
ing of low-frequency waves, but it does cause the reduction or disappe
arance of the secondary arrivals at high frequency because of the redu
ced efficiency of the conversions. Synthetic seismograms for an incide
nt S wave arrival show a time delay more than twice as long as for the
P wave and stronger focusing but only weak secondary phases. Consider
able coupling takes place between SV and SH. On the basis of these fin
dings we outline an observational program to image the Hawaiian plume:
stations should preferably be installed close to but not directly on
top of the most Likely position of the plume axis.