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Ilya ZaliapinDepartment of Mathematics and Statistics
University of Nevada, Reno
SAMSI workshop “Dynamics of Seismicity”Thursday, October 10, 2013
Yehuda Ben-ZionDepartment of Earth Sciences
University of Southern California
Spatio-temporal evolution of seismic clusters in southern and central California
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Earthquake clusters: existence, detection, stability
Clusters in southern California
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Outline
o Main types of clusterso Topological cluster characterization
Evolution of clustering with relation to large events44
Cluster type vs. physical properties of the lithosphere
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Data
•Southern California catalog: Hauksson, Yang, Shearer (2012) available from SCEC data center; 111,981 earthquakes with m ≥ 2
•Heat flow data from www.smu.edu/geothermal
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Baiesi and Paczuski, PRE, 69, 066106 (2004)Zaliapin et al., PRL, 101, 018501 (2008)
Zaliapin and Ben-Zion, GJI, 185, 1288–1304 (2011)Zaliapin and Ben-Zion, JGR, 118, 2847-2864 (2013)Zaliapin and Ben-Zion, JGR, 118, 2865-2877 (2013)
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10 , 0ibmdr
(Fractal) dimension of epicenters
Intercurrence time Spatial distance Gutenberg-Richter law
[M. Baiesi and M. Paczuski, PRE, 69, 066106 (2004)]
/2 /2Rescaled time 10 , Rescaled distance 10i ibm bmdT R r
[Zaliapin et al., PRL, 101, 018501 (2008)]
, log log logTR T R
Distance from an earthquake j to an earlier earthquake i :
Definition:
Property:
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Separation of clustered and background parts in southern California
Earthquake j
Pare
nt (n
eare
st n
eigh
bor)
i
Zaliapin and Ben-Zion, JGR (2012)
Zaliapin et al., PRL (2008)
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Background and clustered parts in models
Zaliapin and Ben-Zion, JGR (2013)
Zaliapin et al., PRL (2008)
Homogeneous Poisson process ETAS model
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Separation of clustered and background parts in southern California
Background = weak links(as in stationary,
inhomogeneous Poisson process)
Clustered part = strong links (events are much closer to each
other than in the background part)
Zaliapin and Ben-Zion, JGR (2013)
Zaliapin et al., PRL (2008)
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weak link
strong link
Cluster #3
Cluster #2
Cluster #1
Identification of clusters: data driven
Time
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Foreshocks
Aftershocks
Mainshock
Identification of event types: problem driven
Time
Single
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ETAS declustering: Example
29,671 events
9,536 mainshocks
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① Burst-like clusters Represent brittle fracture. Large b-value (b=1), small number of events,
small proportion of foreshocks, short duration, small area, isotropic spatial distribution.
Tend to occur in regions with low heat flow, non-enhanced fluid content, relatively large depth => increased effective viscosity.
② Swarm-like clusters Represent brittle-ductile fracture. Small b-value (b=0.6), large number of
events, large proportion of foreshocks, long duration, large area, anisotropic channel-like spatial pattern.
Tend to occur in regions with high heat flow, increased fluid content, relatively shallow depth => decreased effective viscosity.
③ Singles Highly numerous in all regions; some but not all are related to catalog
resolution.
④ Clusters of the largest events Most prominent clusters; object of the standard cluster studies. Not
representative of the majority of clusters (mixture of types 1-2).
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M5.75
M5.51
M5.51 M5.75
L= 417, tree depth = 9, ave. depth = 3.8 L= 572, tree depth = 44, ave. depth = 30.3
Swarm vs. burst like clusters:Topologic representation
Burst-like Swarm-like
Tim
e
Tim
e
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Average leaf depth (number of generations from a leaf to the root):Bimodal structure
HYS (2012), mM ≥ 2
Large topological depth:Swarm-like clusters
Small topological depth:Burst-like clusters
ETAS model
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Heat flow in southern Californiahttp://www.smu.edu/geothermal
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Preferred spatial location of burst/swarm like clusters 195 clusters with m ≥ 4, N ≥ 10; spatial average within 50 km
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Moment of foreshocks relative to that of mainshock 195 clusters with m ≥ 4, N ≥ 10; spatial average within 50 km
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Family size 112 Δ- clusters with m ≥ 4, N ≥ 10; spatial average within 50 km
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X-zoneX-zone
X-zoneX-zone
D-zoneD-zone
D-zoneD-zone
Time
Spa
ce
N-zone
Statistical analysis of premonitory patterns: zero-level approach
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D = 2 years, X = 1 year, R = 200 km, M=6.5mainshocks with m>3 are examined
All mainshocks
Topological depth (average leaf depth)
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Δ = X = 3 years, R = 100km m > 3, N > 20
ANOVA p =7x10-7 : Significant difference
Large families, N > 20
Topological depth (average leaf depth)
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Δ = X = 2 years, R = 100km m > 3
All mainshocks
Proportion of families
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Δ = X = 2 years, R = 100km m > 3, N >1
Families (N > 1)
Proportion of large families (N>=5)
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Large earthquakes in California, M6.5
2) Landers, M7.3, 1992
2) Landers, M7.3, 1992
4) Hector Mine, M7.1, 1999
4) Hector Mine, M7.1, 1999
1) Superstition Hills, M6.6, 1987
1) Superstition Hills, M6.6, 1987
5) El Mayor Cucapah, M7.2, 2010
5) El Mayor Cucapah, M7.2, 2010
3) Northridge, M6.7, 1994
3) Northridge, M6.7, 1994
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“San Jacinto Fault”
SH
EMC
LN
HM
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Families with 3 < m < 4
Families with size L > 10
“San Jacinto Fault”
SH EMC
L N HM
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Topological depth d > 6, mainshock m< 5
100 km from Superstition Hills, M6.6 of 1987
SH EMCL N HM
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Average leaf depth > 1, Family size > 5
SH EMCL N HM
Salton Trough
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Average leaf depth > 1, Family size > 5
Baja California
SH EMCL N HM
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Average leaf depth > 1, Family size > 5
R < 5 km
R < 20 km
R < 100 km
R < 300 km
El Mayor Cucapah, M7.2
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Topological depth d > 5
20 km from Landers, M7.3 of 1992
In this region: 613 mainshocks; 139 families; 11 mainshocks/10 families with m>3.5
Remote aftershock of Superstition Hill, M6.6 of 1987
Remote aftershock of Superstition Hill, M6.6 of 1987
Landers, M7.3 of 1992Landers, M7.3 of 1992
Remote foreshock to Hector Mine, M7.1 of 1999
Remote foreshock to Hector Mine, M7.1 of 1999
SH EMCL N HM
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Seismic clusters in southern California1
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Summary
o Four types of clusters:• Burst-like clusters• Swarm-like clusters• Singles• Largest regional clusters
o Topological cluster characterization
o Swarm-like clusters <-> decreased effective viscosityo Burst-like clusters <-> increased effective viscosity
Spatial variability: Relation to physical properties of the crust
Temporal variability: Relation to large events