Ej. Garnero et Dv. Helmberger, A VERY SLOW BASAL LAYER UNDERLYING LARGE-SCALE LOW-VELOCITY ANOMALIESIN THE LOWER MANTLE BENEATH THE PACIFIC - EVIDENCE FROM CORE PHASES, Physics of the earth and planetary interiors, 91(1-3), 1995, pp. 161-176
A multi-phase analysis using long-period World Wide Standardized Seism
ograph Network and Canadian Network data has been conducted using core
-phases for deep focus events from the southwest Pacific. These includ
e SKS, S2KS, SVdiff, and SPdKS. The last phase emerges from SKS near 1
06 degrees and is associated with a P-wave diffracting along the botto
m of the mantle. Patterns in S2KS-SKS differential travel times (T-S2K
S-SKS) correlate with those in SPdKS-SKS(T-SPdKS-SKS). T-S2KS-SKS valu
es strongly depend on variations in V-s structure in the lower third o
f the mantle, whereas T-SPdKS-SKS values mainly depend on V-p structur
e and variations in a thin zone (100 km or less) at the very base of t
he mantle. Anomalously large T-SPdKS-SKS and T-SPdKS-SKS values (relat
ive to the Preliminary Reference Earth Model (PREM)) are present for F
iji-Tonga and Kermadec events (recorded in North and South America), a
long with anomalously large SVdiff amplitudes well into the core's sha
dow. More northerly paths beneath the Pacific to North America for Ind
onesian and Solomon events display both PREM-like and anomalous times.
A model compatible with the observations is presented, and contains a
thin very-low-velocity layer at the base of the mantle that underlies
the large volumetric lower-mantle low-velocity regions in the southwe
st Pacific. A low-velocity layer of 20-100 km thickness with reduction
s of up to 5-10% (relative to PREM) can reproduce T-SPdKS-SKS as well
as SVdiff amplitudes. Large-scale (more than 1000 km) lower-mantle V-s
heterogeneity (2-4%) can explain long-wavelength trends in T-S2KS-SKS
. The exact thickness and velocity reduction in the basal layer is unc
ertain, owing to difficulties in resolving whether anomalous structure
occurs on the source- and/or receiver-side of wavepaths (at the CMB).