Geophysical Test of Low-Angle Dip on the Seismogenic Dixie Valley Fault,
Nevada
Robert E. Abbott1, John N. Louie1, S. John Caskey2,
Stephen G. Wesnousky3
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University of Nevada, Reno Seismological Laboratory and Department of Geological
Sciences
-
San Francisco State University
-
University of Nevada, Reno Center for Neotectonic Studies and Department
of Geological Sciences
Presented at the Fall 1998 American Geophysical Union meeting, San Francisco
(Presentation also available as a 2.4 Mb Acrobat
PDF file.)
Abstract
The Dixie Valley fault ruptured in a normal event of Ms 6.8 in August of
1954. Recent geologic study of the fault trace has been used to suggest
that much of the trace is characterized by dips as low as 25 degrees. Nodal
planes for the event are poorly defined for the event because of coda from
the nearby Fairview Peak earthquake (Ms 7.2) that occurred 4 minutes earlier.
Our recent collection of high-resolution and medium-resolution seismic
reflection profiles across the fault provides data consistent with the
low-angle hypothesis.
The high-resolution survey was conducted within 130 m of the rupture
with 100 Hz geophones and a sledgehammer source. The medium-resolution
line used near-surface explosive sources, 8 Hz geophones, and extended
from the rupture to 2.9 km into the basin. Both high- and medium-resolution
profiles define the surface as dipping at 25-30 degrees to 1.5 km depth.
The high-resolution survey shows fault-surface reflections from within
10 m of the surface to 50 m depth; the medium-resolution survey shows fault-surface
reflections from 100 m to 1.5 km depth. Reflections subparallel to the
fault-surface may be seen in the granite footwall, from 10 to 200 m depth.
Also seen are rollover anticlines and buried rupture-graben structures
in the sedimentary hanging wall. A vertically coincident refraction off
the fault-surface from a long-offset source is also consistent with the
presence of a smooth, shallowly dipping fault from 50 to 700 m depth. Gravity
results support a shallow basin model, as required by the shallowly dipping
boundary normal fault.
Introduction
Estimates of extension in the Basin and Range range are commonly above
100 percent (Hamilton, 1978; Wernicke et. al, 1988; Proffett, 1977). Examination
of earthquake mechanisms in the western United States reveals the complete
absence of large events occurring on normal faults with dips less than
38 degrees (Doser and Smith, 1989). A global study by Jackson (1987) shows
a similar limit (approximately 35 degrees) on normal fault dip and reveals
that faults are essentially planar and dip steeply down to the brittle-ductile
transition. As well, frictional constraints have been used to argue that
it is more favorable to create new, steeply-dipping faults than accumulate
slip on low-angle normal faults.
Given planar faults and minimum fault dip of 38 degrees, simple geometric
relations (Jackson and McKenzie, 1983) can be used to show that the maximum
extension possible from a single fault system with rotation of dip is 40%.
Beyond 40%, extension must be taken up by a new set of high-angle faults
cutting the old system, or by aseismic slip on faults which have rotated
to a low angle.
In contrast, several researchers have compiled observations to argue
for the existence of Quaternary seismic slip on low-angle normal faults
(Axen et al., 1998; Abers, 1983; Burchfiel et al., 1987, Johnson and Loy,
1992). Also, it has been shown that it is energetically more feasib le
to accommodate large amounts extension on normal faults of low dip (Forsyth,
1992).
Here, we present the results of a seismic reflection and gravity experiment
to test whether or not part of the 16 December 1954 Dixie Valley Earthquake
(Ms=6.8) produced slip on a low-angle normal fault.
Fig. 1: Dixie Valley Rupture Map

Map
of Dixie Valley in central Nevada. The extent of the 1954 Dixie Valley
surface rupture is denoted by the white arrow. The large error estimate
in the epicenter location is a result of contamination of the waveforms
by the nearby Fairview Peak (Ms=7.2) earthquake, four minutes in advance.
There is a correspondingly large error in fault dip determination.
Fig. 2: 1998 Traverses

This
figure shows the location of our 1998 geophysical field work. High- and
medium-resolution seismic reflection profiles were conducted along Cattle
Road from the range-front scarp eastward. Gravity transects were conducted
across the valley along Settlement and Cattle Roads and along the scarp
from Willow Canyon to Brush Canyon.
Field Acquisition and Data Reduction Methods
Fig. 3: Seismic Data Acquisition

This is a view of Dixie Valley near the fault scarp and looking east, along
Cattle Road. Receiver locations for the medium-resolution survey are red
flags. The medium-resolution profile utilized 8 Hz geophones, explosives
at 2 m depth, and extended 3.6 km into the basin. It was composed of 4
stationary setups of 48 receivers with 15.2 meter spacing. The high-resolution
profile was conducted within 130 m of the range-front scarp with 100 Hz
geophone groups, 2 m spacing, and a sledgehammer source. A linear array
of 6 geophones per group was used to reduce ground-roll in the high-resolution
survey. In both surveys, off-end and longer-offset shots were recorded
to increase fold and gather deep velocity information.

Photo by Karl V. Steinbrugge
1954: Picture of Range-Front Scarp, East Job Canyon
Gravity Data Acquisition
Gravity measurements were made with a LaCoste & Romberg Model G gravity
meter. Vertical control is supplied by a Trimble geodetic-quality GPS.
Data were reduced to simple Bouguer anomaly with a 2.67 g/cc reduction
density and inner-ring terrain corrections to 100 m. Additional data from
Schaefer's (1984) gravity study were incorporated to increase station density.
Fig. 5: Processing Flows
| Post-Stack Migration |
Velocity Analysis and Pre-Stack Migration |
| Trace Editing and Top-Muting |
First Break Picking |
Bandpass Filtering
6-8 and 100-120 Hz trapezoidal frequency domain filter |
Simulated-Annealing Optimization to determine
V(x,z) |
f-k Filtering -->
Polygonal Filter, 50 trace, 500 ms time window |
--> AGC of f-k Filtered Records
500 ms time window |
AGC
200 ms time window |
Pre-Stack Kirchhoff Migration
Includes Lumley-Claerbout operator anti-aliasing |
NMO Correction
Velocities picked in 200 m/s intervals from CV stacks |
Estimation of Noise Data Set
by sign flips on random traces |
CMP Binning and Stacking
15.2 m bin centers, mid-points assigned to bin fold is
variable, no amplitude variation for fold. |
Re-Migration of Noise
for image of artifacts |
Stolt Time Migration
2 km/s migration velocity |
Harlan Coherency Enhancement
scale image by signal expectation |
Velocity Analysis and Acoustical Modeling
Fig. 6: 3-D Velocity Model

This is a velocity model obtained from
a simulated-annealing non-linear optimization of first arrival picks (Pullammanappallil
and Louie, 1994). A three-dimensional inversion was calculated because
of a slig htly crooked-line geometry along the Cattle Road profile. The
3-D model was subsequently "flattened" to 2-D for use in Kirchhoff pre
-stack migration as in Chavez-Perez et al. (1998).
Fig. 7: Refraction Experiment

This raw, long-offset
shot gather from our medium-resolution profile shows a headwave propagating
vertically from the fault surface (highlighted). The coincident first-arrivals
across the entire receiver array limit the range of the dip of the fault.
The shot geometry and interpretation is given in Figure 8.
Fig. 8: Acoustic Model of Headwave

This is an acoustic model of the vertically propagating headwave shown
in Figure 7. The model assumes a basement-alluvium velocity contrast of
2 to 1, along a 30-degree dipping fault plane. The array of receivers is
shown near the fault scarp. Energy from the blast, at flag number 101 (2.1
km), reflects and refracts off the fault interface. This geometry reproduces
the vertically propagating headwave seen on the shot record. Similar refractions
along the high-resolution seismic line (not shown) demonstrate that the
fault plane continues along this dip to the surface. The synthetics were
produced by a finite-difference solution to the scalar wave equation described
by Helmberger and Vidale (1988).
Results
Fig. 9: 2.0 km/s Stolt-Migrated Stack

This is a post-migrated stack of our medium-resolution Cattle Road profile,
following the processing flow given in figure 5. The fault plane reflector,
dipping eastward at 25-30 degrees, can be traced to its surface outcrop.
Reflections sub-parallel to the fault can be seen in the footwall, suggesting
foliation in the granite. Highly reflective Tertiary basalt layers in the
hanging wall begin to obscure the fault reflections at about 500 ms. However,
the basalt layers can be traced to the extension of the fault at depth,
where they are seen to terminate, after forming small roll-over anticlines.
The roll-over anticlines support a listric fault geometry.
Fig. 10: Enhanced, Anti-Aliased Pre-Stack Migration

This is a pre-stack migration of the same profile as above, also following
the flow given in figure 5. The migration used the Lumley-Claerbout operator
anti-aliasing criterion, yielding a longer-wavelength view of subsurface
reflectivity. With it, we can see below the reflective basalts in the hanging
wall, and image the shallowly-dipping fault to 1.5 km depth.

Fig. 11: Preliminary Gravity Basin Model

This is a modeled basin geometry of the gravity data obtained along the
Cattle Road Profile. The scatter in the observed points is due to insufficient
elevation control as the roving-mode GPS data has yet to be fully rectified.
Even so, the shape of the anomaly is not affected by the scatter and it
is compatible with a low-angle geometry. A 1:1 overlay of the seismic results
is consistent with the low-angle hypothesis. The gradational density in
the basin fill follows a regional scheme used by Blakely et al. (1996)
in their gravity inversions. Modeling was done with the GM-SYS package
by Northwest Geophysical Associates.
Conclusions
Our results indicate that slip along a section of the 16 December 1954
Dixie Valley earthquake rupture took place along a fault plane of unusually
low dip (25-30 degrees). In this regard, it is the first large historical
earthquake for which slip on a low-angle normal fault has been documented.
Selected References
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Abers, G. A., 1991, Possible seismogenic shallow-dipping
normal faults in the Woodlark-D'Entrecasteaux extensional province, Papua
New Guinea: Geology, 19, 1205-1208.
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Axen, G. J., J. M. Fletcher, E. Cowgill, M. Murphy, P. Kapp,
I. MacMillan, E. Ramos- Velazquez, and J. Aranda-Gomez, 1998, Range-front
fault scarps of the Sierra El Mayor, Baja California: Formed above and
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Blakely, R. J., R. C. Jachens, J. P. Calzia, and V. E. Langenheim,
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Burchfiel, B. C., K. V. Hodges, and L. H. Royden, 1987, Geology
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Caskey, S. J., S. G. Wesnousky, P. Zhang, and D. B. Slemmons,
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(Ms 6.8) earthquakes, Central Nevada: Bull. Seis. Soc. Am., 86, 761-787.
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Chavez-Perez S., J. N. Louie, and S. K. Pullammanappallil,
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Doser, D. I., and R. B. Smith, 1989, An assessment of source
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Acknowledgements
This project was funded by the National Science Foundation
(EAR-9706255). The W. M. Keck Foundation donated seismic equipment, computers,
and modeling software. All geophysical fieldwork was performed by the spring
1998 Geophysical Applications class at the University of Nevada, Reno.
Class participants were: Ana Cadena, Travis Rabe, Matt Herrick, Mandy Johnson,
Andrew Rael, Tom Blechen, and Evan Hobson. Additional field assistance
was rendered by Christine Mann, Jim Ollerton, and John Oswald. Simulated-annealing
of first-arrival picks was performed by Sathish Pullammanappallil of OPTIM
LLC. Thanks to Mike Dennis and Nevada Precision Drilling and Blasting for
their work. We also thank Prill Meacham and the Carson City office of the
BLM for their assistance and cooperation.