GEOLOGY
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Volume 44
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Number 7
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www.gsapubs.org 575
Rapid variation in upper-mantle rheology across the San Andreas
fault system and Salton Trough, southernmost California, USA
Shahar Barak* and Simon L. Klemperer
Department of Geophysics, Stanford University, 397 Panama Mall, Stanford, California 94305, USA
ABSTRACT
We present new shear-wave splitting data showing systematic lat-
eral variations in upper-mantle anisotropy across the plate boundary
in southernmost California (USA). Beneath the Peninsular Ranges
batholith, fast polarization directions parallel the direction of former
Farallon subduction, suggestive of a slab remnant. Near the eastern
edge of the batholith, across the Elsinore fault, fast polarization direc-
tions change rapidly to align with the direction of San Andreas fault
shear. We infer that the Elsinore fault penetrates the entire lithosphere
and may represent a future localization of the plate boundary that is
migrating west from the San Andreas fault. Beneath the Salton Trough
and the Chocolate Mountains region, large splitting times, despite a
very thin lithosphere, imply vertical melt pockets in the uppermost
mantle aligned in the shear direction. Largest splitting times, ~1.2 s,
are seen closest to the Sand Hills fault that projects southeast from the
San Andreas fault. Further east, in the southern Basin and Range prov-
ince, fast directions align with North America absolute plate motion.
INTRODUCTION
Analysis of teleseismic shear-wave splitting is a standard tool for study-
ing upper-mantle anisotropy created by strain-induced lattice-preferred
orientation of minerals or by preferentially oriented melt-filled inclusions,
and hence also for studying changes in rheology (e.g., Savage, 1999, and
references therein). A shear wave passing through an anisotropic medium
splits into slow and fast waves with orthogonal polarizations. Two splitting
parameters (polarization, ϕ, and delay time, δt ) provide a direct estimate
of the axis and magnitude of the anisotropy for simple cases and show
systematic variations with back-azimuth to the source earthquake in more
complex scenarios.
Despite Southern California’s (USA) complex tectonic history and
active plate boundary oriented northwest-southeast (e.g., Dickinson,
2008, 2009; Barak et al., 2015) (Fig. 1A), previous studies of shear-
wave splitting in Southern California (e.g., Polet and Kanamori, 2002;
Kosarian et al., 2011) show a nearly uniform fast axis of anisotropy ori-
ented approximately west-east (Fig. 1C). This has been interpreted as due
to inherited North America plate motion (Kosarian et al., 2011), pre–late
Cenozoic compression (Polet and Kanamori, 2002), or mantle flow around
the southern edge of the subducting Gorda slab (Zandt and Humphreys,
2008). The same general west-east pattern continues to the southern tip
of Baja California (Mexico), west and east of the Gulf of California rift
margins (Long, 2010; Fig. 1A). Recent three-dimensional (3-D) tomo-
graphic inversion of shear-wave splitting measurements, despite the pre-
vious scarcity of data in southernmost California, has begun to suggest
complicated structure, including a northwest fast axis of anisotropy in
the Salton Trough (ST) (Monteiller and Chevrot, 2011) where Gulf of
California ocean spreading propagates into continental crust along the
San Andreas fault (Elders et al., 1972).
Here we analyze shear-wave splitting measurements on our array of
48 seismometers that spanned southernmost California from A.D. 2011 to
GEOLOGY, July 2016; v. 44; no. 7; p. 575–578
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Data Repository item 2016190
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doi:10.1130/G37847.1
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Published online 15 June 2016
© 2016 Geological Society of America. For permission to copy, contact editing@geosociety.org.
32°N
33°N
34°N
PAC(HS)
NAM(HS)
PAC(NAM)
10 mm/yr
1.0 s
0
117°W 116°W 115°W 114°W -113˚
32°N
33°N
34°N
SHF
AF
IF
SJF
SAF
LSF
EF
CPF
SAFs
USA
Mexico
{
USA
Mexico
AZ
CA
PRB
CMR
ST
BRP
Pacific
Ocean
ECSZ
PAC
Gulf of
California
A
B
C
20
40
Diff. from SAFs [°]
M7.2
N
N
N
Figure 1. A: Pacific (PAC)–North America (NAM) plate boundary
(black—transform; orange—spreading center), showing location of
B and C (black rectangle), and shear-wave splitting (SWS) fast polari-
zations further south in Mexico (Long, 2010) using length scale and
color scale as in C. B: Shaded-relief topography overlain with our
seismic stations (stars), other permanent stations shown in Figure 2
(triangles), and line of section in Figure 2 (white line). BRP—south-
ern Basin and Range province; CMR—Chocolate Mountains region;
PRB—Peninsular Ranges batholith; ST—Salton Trough. Dot-patterned
orange boxes show active spreading centers (Elders et al., 1972).
Strike-slip focal mechanism: 4 April 2010 El Mayor–Cucapah earth-
quake. Thick red lines show major faults of San Andreas fault system
(SAFs) (AF—Algodones; CPF—Cerro Prieto; EF—Elsinore; IF—Impe-
rial; LSF—Laguna Salada; SAF—San Andreas; SHF—Sand Hills;
SJF—San Jacinto). Thin red lines show southeast extension of Eastern
California Shear Zone (ECSZ) (Darin and Dorsey, 2013). C: SWS fast
polarizations with lengths proportional to delay time (colored bars).
This study: white circles (open circles if no “good” or “fair” results
were available); other SWS results: Wüstefeld et al. (2009); Liu et al.
(2014; only “A” quality data, weighted by their standard deviation).
Color of bars indicates difference in degrees from trend of SAFs.
Black arrows are plate-motion vectors relative to fixed-hotspot (HS)
frame (Gripp and Gordon, 2002). Red line is 55 km depth contour of
lithosphere-asthenosphere boundary (Lekic et al., 2011). Thin black
lines are fault traces (Plesch et al., 2007). *Current address: Noble Energy, Houston, Texas 77070, USA.