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Temporal and spatial variations of microearthquake activity along the Dead Sea Fault, 1984-2004

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Patterns of spatial and temporal variations in microearthquake activity during 1984-2004 were studied in five segments along the Dead Sea Fault (DSF). In each segment there is a narrow zone in which intense seismic activity is concentrated; the most active one is the Dead Sea segment. Segments are also characterized by distributions of hypocenter depths, with the northern Arava and Dead Sea showing the deepest hypocenters. The annual distribution of earthquakes is nonuniform in all segments, with years of peak activity occurring between 1989 and 1992 in the different segments. The maximum annual number for the DSF as a whole was 215 earthquakes (ML ≥ 0) in 1991, while in 1984 and in 2001 the number of earthquakes was only about 70. The cumulative seismic moment for the DSF decreased exponentially from 1984 (2.1022 dyne cm) to 20% of that value in 2003 and then increased by two orders of magnitude in 2004. During 1995-2004 the changes in the annual number of earthquakes were concomitant with changes in the average annual Rn concentration, as measured close to the active boundary fault in the NW Dead Sea. In southern Israel and Jordan, where only few earthquakes had occurred between 1984 and 1995, a marked increase in seismic activity took place after the 1995 Nuweiba earthquake in the Gulf of Elat.
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Isr. J. Earth Sci.; 54: 1–14
© 2005 Science From Israel/ LPPLtd. 0021-2164/05 $4.00
E-mail: begin_bz@mail.gsi.gov.il
Temporal and spatial variations of microearthquake activity along the
Dead Sea Fault, 1984–2004
Ze’ev B. Begin and Gideon Steinitz
Geological Survey of Israel, 30 Malkhe Yisrael Street, Jerusalem 95501, Israel
(Received 6 January 2004; accepted in revised form 28 October 2004)
ABSTRACT
Begin, Z.B. and Steinitz, G. 2005. Temporal and spatial variations of microearth-
quake activity along the Dead Sea Fault, 1984–2004. Isr. J. Earth Sci. 54: 1–14.
Patterns of spatial and temporal variations in microearthquake activity during 1984–
2004 were studied in five segments along the Dead Sea Fault (DSF). In each segment
there is a narrow zone in which intense seismic activity is concentrated; the most
active one is the Dead Sea segment. Segments are also characterized by distributions
of hypocenter depths, with the northern Arava and Dead Sea showing the deepest
hypocenters.
The annual distribution of earthquakes is nonuniform in all segments, with years of
peak activity occurring between 1989 and 1992 in the different segments. The maxi-
mum annual number for the DSF as a whole was 215 earthquakes (M
L
0) in 1991,
while in 1984 and in 2001 the number of earthquakes was only about 70. The
cumulative seismic moment for the DSF decreased exponentially from 1984 (210
22
dyne cm) to 20% of that value in 2003 and then increased by two orders of magnitude
in 2004. During 1995–2004 the changes in the annual number of earthquakes were
concomitant with changes in the average annual Rn concentration, as measured close
to the active boundary fault in the NW Dead Sea. In southern Israel and Jordan, where
only few earthquakes had occurred between 1984 and 1995, a marked increase in
seismic activity took place after the 1995 Nuweiba earthquake in the Gulf of Elat.
INTRODUCTION
The Dead Sea Fault (Transform) is an active fault zone
forming the Arabian–Sinai plate boundary, stretching
from the spreading Red Sea to the Eastern Anatolian
Fault. All along the Transform it is accompanied by a
conspicuous rift valley. Based on considerations of
plate kinematics and matching of structures across the
Fault (summarized by Garfunkel, 2001), it is generally
accepted that the principal sense of movement along
the Fault has been left lateral, with a total slip of 105
km (Quennel, 1959; Freund, 1965; Freund et al., 1970;
Garfunkel et al., 1981; Garfunkel, 2001). According to
a different view, the horizontal slip along the Dead Sea
fault is smaller (Mart, 1991; Horowitz, 2001), amount-
ing to 10–20 km (Mart et al., 2005).
The average horizontal slip rate along the Dead Sea
Fault (DSF) during the last 5 Ma was determined to be
6–7 mm/year, based on plate kinematics (Joffe and
Garfunkel, 1987; Garfunkel, 2001). Along the middle
and northern Arava segment of the DSF, several esti-
mates of horizontal slip rates were suggested, based on
2 Israel Journal of Earth Sciences Vol. 54, 2005
displaced alluvial fans, terraces, and gullies: 3–7.5 mm/
year during the last 5–2 Ma (Ginat et al., 1998); 4 ±
2 mm/year during the last 70,000–140,000 years and
5 ± 1.2 during the last 2,000–3,000 years (Klinger et al,
2000); 4.7 ± 1.3 mm/year during the last 15,000 years
and 3.9 ± 0.5 during the last 6,000 years (Niemi
et al., 2001). In the Missyaf segment of the DSF in
Syria, north of the Yammuneh restraining bend, a
displaced aqueduct shows a slip rate of 7 mm/year
during the last 2000 years (Meghraoui et al., 2003).
Based on GPS measurements, the current slip rate
along the DSF is 3.3 ± 0.4 mm/year (Wdowinski et al.,
2004).
A century-long record that includes strong earth-
quakes shows that the moment released by the ob-
served earthquakes along the DSF did not account for
more than 2 mm/year of the rate of relative motion
across the Transform (Ben-Menahem, 1981;
Garfunkel et al., 1981; Salamon et al., 2003; Shapira et
al., 2004). Noting that in these calculations the mo-
ments were added regardless of the actual direction of
movement on particular faults (Salamon et al., 2003),
this is a maximum value. Deficiency in seismic mo-
ment along the Dead Sea Fault is also shown for the
period 70–14 ky BP in the record of the Lisan Forma-
tion, by the meagerness of strong earthquakes (Marco
et al., 1996; Begin et al., 2005), as well as in the record
of damaged cave deposits in the Soreq Cave, 40 km west
of the Dead Sea (Kagan et al., 2005). Thus, the seismic
activity accounts for only a part of the movement along
the DSF.
Of the earthquakes that occurred along the DSF in
the last 20 years about 99% were of a magnitude <4,
and one should be cognizant of the fact that the rela-
tionship between such small seismic events and the
seismotectonic regime along the DSF is not at all
obvious. This problem is examplified by the fact that
in spite of the overwhelming evidence for a left-lateral
movement along the DSF, several fault-plane solu-
tions along it (carried out for M
L
4 earthquakes)
indicate other mechanisms and directions of move-
ment, some attesting to normal faulting and hence
extension in a direction perpendicular to the DSF di-
rection. The expected main component of left-lateral
motion on NNE-striking faults along the DSF is found
in the fault-plane solutions for the strongest events, in
1927 and in 1995 and their aftershocks (Salamon et al.,
2003). On top of these problems, the present study is
based on an instrumental record that is only 21 years
long and the limitations on the ability to draw pertinent
tectonic information from this short period are clear.
On the other hand, the importance of micro-
earthquakes should not be dismissed hastily. Their
analysis reveals regular patterns that are characteristic
of tectonic provinces (Wesnouski, 1990; Stirling et al.,
1996), and it has also been shown that a rise in the
seismic rate of small earthquakes may herald a strong
earthquake (Shapira, 1990; Bowman et al., 1998).
Time-dependent seismic behavior of strong earth-
quakes along the DSF has been shown on the scale of
tens of thousands of years (Marco et al., 1996; Begin et
al., 2005), thousands of years (Amit et al., 1995;
Leonard et al., 1998; Zilberman et al., 2000; Amit et
al., 2002), and hundreds of years (Migowski et al.,
2004). Seismic characteristics of segments along the
DSF, based on short records of microearthquakes,
have been discussed previously (Wu et al., 1973; Arieh
and Rotstein, 1985; Rotstein and Arieh, 1986; Shapira
and Feldman, 1987; van Eck and Hofstetter, 1989,
1990; Hofstetter et al., 1996). However, these short-
term analyses did not permit presentation of temporal
patterns in the rate of seismic activity along the DSF.
Here we report temporal patterns in the rate of
microearthquake seismicity on the scale of years, after
two decades of meticulous data gathering of mi-
croearthquakes in this region by the Seismology Divi-
sion of the Geophysical Institute of Israel.
METHOD
In some previous studies that addressed seismicity
along the DSF, the area between the Gulf of Elat and
the Baqaa in Lebanon was subdivided into two seg-
ments: a northern segment, which either includes the
southern Dead Sea (Ben-Menahem, 1991; Yücemen,
1992) or excludes it (Khair et al., 2000), and the Arava
segment. In other studies a more detailed subdivision
was employed, based on geological considerations.
Since the DSF comprises pull-apart grabens and seg-
ments between them that are structurally higher
(Heimann, 1990; Garfunkel, 1997; Frieslander and
Bartov, 1997), in the studied area the DSF lends itself
to a natural subdivision into four segments (Arieh and
Rabinowitz, 1989; Shamir et al., 2001): The Arava
structural high, the Dead Sea pull-apart, the Jordan
valley structural high, and the Kinneret–Hula pull-
aparts. In an attempt to furnish more detail on the
120-km-long Arava segment, we divided it further into
northern and southern segments with the border be-
tween them in the Arava water divide (Fig. 1).
The earthquake data set for the study area (Fig. 1)
was taken from the Israeli earthquake catalog for 2004
Z.B. Begin and G. Steinitz. Dead Sea Fault earthquake activity, 1984–2004 3
(www.gii.co.il/html/seis/seis_search.html), as pub-
lished by the Seismology Division of the Geophysical
Institute of Israel, which operates the Israel Seismic
Network (ISN). The magnitude threshold of complete
record for the area along the DSF is, since 1986,
M
L
2.0 (Shapira, 1992); for 1984–1985 the threshold
is M
L
2.5 (Shapira, 2002, appendix A). Although the
ISN was installed in 1980, the record analyzed here
starts in 1984, taking into account initial difficulties
in the ISN operation. The magnitude–frequency rela-
tionship (Fig. 2) shows that this study deals with
microearthquakes.
The presentation of the results starts with general
considerations: a description of the spatial distribution
of earthquakes, the adequacy of the data set, and the
temporal nonuniformity of the time series for the DSF
as a whole. We then proceed to describe in each seg-
ment the temporal patterns of two aspects of seismic-
ity: number of earthquakes and seismic moment.
RESULTS
A. General considerations
Spatial clusters
As already noted, on the basis of few years of
observations (van Eck and Hofstetter, 1989, 1990;
Shapira, 1990), the spatial distribution of microearth-
quakes along the DSF is nonuniform. Five spatial
Fig. 1. Earthquakes (M
L
2) during 1984–2004 along the
DSF and near it, classified according to their magnitude
(M
L
), shown on the backdrop of faults that are potentially
active (Bartov et al., 2002). Rectangles are segments used in
this study; from bottom: (1) southern Arava (135/–120 to
175/–030), (2) northern Arava (155/–030 to 200/040), (3)
Dead Sea (175/040 to 215/140), (4) Jordan Valley (190/140
to 215/230), (5) Kinneret (190/230 to 215/300). Grey area
denotes the Dead Sea rift valley.
Fig. 2. Cumulative magnitude–frequency diagram for earth-
quakes in the five segments along the DSF (Fig. 1). Data are
based on periods with complete records: since 1900 for
M
L
5, since 1940 for M
L
4, and since 1984 for M
L
2.
The resulting b-value is 0.96.
4 Israel Journal of Earth Sciences Vol. 54, 2005
clusters, one in each segment, are revealed in Figs. 3
and 4. Measured along the north–south direction, the
width of these clusters comprises only some 10% of
the rift length, but more than 20% of the earthquakes
that occurred in 1984–2004 are concentrated in them.
In the Arava, Dead Sea, and Jordan valley segments
(Fig. 1) the locations of these clusters coincide with
junctions of the DSF with transversal faults: The
Thamad fault in the Southern Arava, the Paran–Arif
fault in the northern Arava, an E–W fault east of the
Dead Sea, and the Faria fault in the Shomeron (see also
Aldersons et al., 2003, fig. 1).
The five segments also show characteristic distribu-
tions of hypocenter depths (Fig. 5), despite the large
error in their determination and recognizing that depth
was truncated in the determination algorithm at 25 km
(A. Shapira, personal communication, 2004). Charac-
terizing the depth distributions by their medians, the
northern Arava and Dead Sea segments are similar
(median depth = 11.5 km), the southern Arava has
shallower hypocenters (median = 9.5 km), and the Jor-
dan valley and Kinneret segments show still shallower
hypocenters (median depths of 9 km and 7.5 km, re-
spectively). The differences between the depth distri-
butions of the northern Arava and Dead Sea segments
and those of the three other segments are significant at
the p < 10
–5
level (Fig. 5). Except for the southern
Arava segment, this trend corresponds to the south-to-
north thinning of the crust by 5 km along the DSF
(Aldersons et al., 2003).
Earthquake doublets
Earthquake “doublets” are those that occur a short
time (here defined as less than one day) after a previ-
ous earthquake. “Doublets” might spuriously affect
the analysis of the annual number of earthquakes be-
cause some of them are dependent on the occurrence
of earthquakes that immediately precede them. To ex-
Fig. 3. A space–time diagram showing seismic activity along
the DSF, 1984–2004, for all recorded earthquakes. Note
clustering of earthquakes in narrow zones within each seg-
ment. Segment numbers in right-hand column correspond to
Fig. 1.
Fig. 4. Distribution of earthquakes along the DSF, for 1984–
2004. Discussed segments are indicated. Bin size is 10 km.
A: M
L
0. B: M
L
2. The figures are quite similar, but with
the smaller earthquakes the clustering along the DSF is more
pronounced.
A
B
Z.B. Begin and G. Steinitz. Dead Sea Fault earthquake activity, 1984–2004 5
Fig. 5. Depth of hypocenters in the five segments along the
DSF for the period 1984–2004, depicted by the cumulative
percent of earthquakes in each segment. The differences
between the depth distributions in the Dead Sea and northern
Arava segments, with a median of 11.5 km, are significantly
different (p < 10
–5
, tested with the Mann–Whitney test) from
the depth distributions in the segments of the Kinneret (me-
dian = 7.5 km), the Jordan valley (median = 9 km), and the
southern Arava (median = 9.5 km).
Fig. 6. For all earthquakes during 1984–2004 in the five segments along the DSF: A–B: Occurrence of distance to previous
earthquake (D
p
) for two different time intervals to previous earthquake (T
p
). About 30% of earthquakes with T
p
< 1 day are
found at D
p
< 5 km. Bin size is 5 km. C–D: Occurrence of time intervals to previous earthquakes (T
p
) for two different distances
to previous earthquake (D
p
). About 70% of the earthquakes with D
p
< 5 km have a T
p
< 0.5 day, while for D
p
> 5 km only 25%
are within that time interval. Bin size is 0.5 day.
amine this issue, the difference (T
p
) between the occur-
rence time of an earthquake and the occurrence time of
an immediate previous one was calculated, as well as
the distance (D
p
) between the locations of the two
earthquake epicenters. The data set was subdivided
into two subsets: one with T
p
<1 day (Fig. 6A) and the
other with T
p
1 day (Fig. 6B). It is seen that for
earthquakes with T
p
< 1 day the modal D
p
is 0–5 km.
The same data set was further subdivided into D
p
results
in two different subsets: one with D
p
< 5 km (Fig. 6C)
and the other with D
p
5 km (Fig. 6D). These subsets are
quite distinct: Only 20% of earthquakes with D
p
5 km
occurred within T
p
< 0.5 day, while about 70% of the
earthquakes with D
p
< 5 km occur within that time
interval, indicating a correlation between consecutive
earthquakes that occur within a short distance from pre-
vious ones. The percent of earthquakes with D
p
< 5 km
increases with the annual number of earthquakes
(Fig. 7B).
Nonuniformity of the earthquake time series
Only earthquakes with M
L
2.0 are fully repre-
sented in the catalog, and the percent of earthquakes
6 Israel Journal of Earth Sciences Vol. 54, 2005
with M
L
< 2.0 increases with the annual number of
earthquakes (Fig. 7A). In the following analyses we
included all earthquakes that are registered in the cata-
log, assuming that the total number provides an indica-
tor for the seismic activity.
Considering only earthquakes with M
L
2.0 and
D
p
> 5 km, which may be viewed as the “harder core”
of the data, the temporal nonuniformity is obvious
(Fig. 7C). For earthquakes with M
L
3.0, the com-
pleteness of the record along the DSF allows us to
extend the time series back to 1964 (Shapira, 2002).
Although the total number of these earthquakes is
small (Fig. 7D), it is possible to compare their numbers
in the first 20 years of this period (1964–1983, 30
earthquakes) to the latter 20 years (1984–2003, 114
earthquakes, even without considering 2004 with its
exceptionally high number of M
L
3.0 earthquakes)
and to test through the χ
2
test the probability of random
occurrence of such deviation from the long-term aver-
age (p < 0.0001). We may conclude that on a decadal
scale the nonuniformity of the time series of annual
number of earthquakes is a real attribute of the seismic
behavior along the DSF during the studied period.
B. Number of earthquakes
Annual distribution of earthquakes
Incorporating all earthquakes (M
L
0) within the
studied area, the time series for the different segments
is presented in Fig. 8. In each of the segments, the
distribution of earthquakes in time is significantly
Fig. 7. For all segments. A: The increase in the percent of earthquakes having M
L
< 2 with increasing annual number of
earthquakes having M
L
0 (1984–2004). p is the probability of random occurrence of the correlation coefficient r. B: The
increase in the percent of earthquakes having D
p
< 5 km with increasing annual number of earthquakes having M
L
0 (1984–
2004). C: The temporal nonuniformity of earthquake occurrence along the DSF, for earthquakes having M
L
2 and D
p
5 km.
Cubic polynomial fit is statistically significant. Horizontal line shows the average for this period. D: The temporal nonuni-
formity of earthquake occurrence along the DSF, for the complete record of earthquakes having M
L
3 for 1964–2004, with a
5-year running average. Horizontal line shows the average for this period.
Z.B. Begin and G. Steinitz. Dead Sea Fault earthquake activity, 1984–2004 7
different from a random one. The timing of the
maxima of annual earthquake occurrence in the five
segments changes slightly between 1989 and 1992; the
maximum for the DSF as a whole is in 1991.
Earthquakes in the southern Arava and adjacent areas
After the 22 November 1995 Nuweiba earthquake
(Shamir et al., 2003), a remarkable increase in seismic-
ity is discerned, mainly NW and NE of Elat, more than
100 km north of the earthquake epicenter (Fig. 9). In
these areas faults trending NW and NE, respectively,
are not known. There was a marked increase in seis-
micity NW of Elat immediately after the Nuweiba
earthquakes and a small increase in seismicity NE of
Elat a year after that earthquake (Fig. 10), whereas in
the southern Arava many earthquakes occurred before
the Nuweiba earthquake. However, an increase in the
number of earthquakes in the southern 50 kilometers
of the Arava after the Nuweiba earthquake can be
clearly seen in the bottom of Fig. 3. We propose that
redistribution of stress following the Nuweiba earth-
quake is the cause of the increased seismicity in south-
ern Israel and Jordan during 1995–1998.
Rate of seismicity and Rn concentration at the NW
Dead Sea
Radon concentration has been measured near the
western boundary fault in the northwestern Dead Sea
since 1995. A statistically significant connection be-
tween anomalies in Rn concentration and earthquakes
Fig. 8. Changes in the annual number of earthquakes (M
L
0) along the DSF during 1984–2004. Temporal trends are
illustrated through polynomial fits (quadratic polynomials for the southern Arava and Jordan valley segments, cubic polynomials
for the Dead Sea and Kinneret segments, as well as for all segments together). p denotes the statistical significance of the fits.
8 Israel Journal of Earth Sciences Vol. 54, 2005
Fig. 10. A, B, C—quarterly earthquake
(M
L
0) occurrence in the three areas
depicted in Fig. 9, respectively, showing
an increase in the number of earth-
quakes after the Nuweiba 1995 earth-
quake in the Gulf of Elat. D—quarterly
occurrence of earthquakes with M
L
4
in the Gulf of Elat for the period 1980–
2004.
Fig. 9. Earthquakes (M
L
0) in the southern Negev and Jordan for the period 1984–2004, classified according to their time of
occurrence relative to the Nuweiba earthquake in the Gulf of Elat, 22 November 1995. Histograms of quarterly earthquake
occurrence in areas A, B, and C are shown in Fig. 10. In areas A and C most earthquakes occurred after the Nuweiba
earthquake.
Z.B. Begin and G. Steinitz. Dead Sea Fault earthquake activity, 1984–2004 9
in the Dead Sea and Kinneret basins has been pre-
sented (Steinitz et al., 2003). Here (Fig. 11), a statisti-
cally significant relationship between the annual num-
ber of earthquakes along the DSF and the annual
average of Rn concentration is presented for the period
1995–2004. This correlation is quite remarkable, re-
membering that Rn concentration varies seasonally
(Steinitz et al., 2003) and that the record pertains to
only one station in the NW Dead Sea, while the num-
ber of earthquakes is recorded along the whole Dead
Sea Fault, 200 km north and south of the Rn monitor
(see also the Discussion below).
Seismic activity and fault offset
The seismic activity along five California strike-
slip faults was shown to be inversely proportional to
the overall fault displacement (Wesnousky, 1988).
Seismic activity was measured as the number of earth-
quakes with M
L
3 that occurred in 55 years per km of
fault length, normalized per 1 mm of Holocene slip. In
order to permit comparison to the DSF, seismicity is
further normalized here per year, taking the DSF com-
plete record for M
L
3 of 41 years (1964–2004). The
DSF fits well within the California scheme (Fig. 12).
C. Seismic moment
For 418 earthquakes in the area of study, seismic mo-
ment (M
0
) values appear in the ISN catalog, being
determined according to the method presented in
Shapira and Hofstetter, 1993. These were used in order
to estimate seismic moment for all other earthquakes
studied here, by regressing log M
0
on magnitude, M
L
(Fig. 13). For the range 0 M
L
5.2 the relationship is
well represented by the quadratic equation: log M
0
=
18.46 + 0.177 M
L
+ 0.160 M
L
2
. A similar relationship
was found for California earthquakes (Hanks and
Boore, 1984; Ben-Zion and Zhu, 2002), and for earth-
quakes in the DSF, the upward curvature of this non-
linear relationship is implied by the findings of
Hofstetter et al. (1996, fig. 7). From a linear regression
of log seismic moment on earthquake magnitude, for
the range 4 < M
L
< 6.7, Shapira and Hofstetter (1993)
obtained the regression equation: log M
0
= (16.0 ± 0.4)
+ (1.5 ± 0.1) M
L
. This calculation underestimates the
seismic moment of earthquakes with M
L
> 5.5; for
M
L
> 6 it underestimates M
0
by more than 50%.
The annual seismic moment for the 425-km-long
DSF studied here (Fig. 14) shows a significant expo-
nential decrease during 1984–2003. On average, the
cumulative seismic moment along the DSF in 2003
(5.310
21
dyne cm) was only 20% of the seismic mo-
ment in 1984. For certain time intervals, in the Arava
segments statistically significant (p < 0.05) exponen-
tial decrease in annual seismic moment release can be
traced, while in the Kinneret segment an increase is
discerned (Fig. 14); no trend is apparent in the Dead
Fig. 11. A—Annual number of earthquakes (M
L
0) in the DSF and annual average Rn concentration measured in the
northwestern Dead Sea (Steinitz et al., 2003), 1995–2004. B—Correlation between annual number of earthquakes in the DSF
and annual average Rn concentration measured in the northwestern Dead Sea. p is the probability of random occurrence of the
correlation coefficient r.
10 Israel Journal of Earth Sciences Vol. 54, 2005
Fig. 13. The relationship between log seismic moment (dyne
cm) and M
L
as determined for 418 earthquakes in the five
segments along the DSF (Fig. 1), showing a significant
quadratic relationship.
Fig. 12. The statistically significant correlation between fault offset and the annual number of earthquakes (M
L
3) per km of
fault length, normalized per 1 mm of annual slip rate, modified after a relationship originally proposed by Wesnouski (1990).
Data points 1–5: Southern California strike-slip faults for 1932–1986 (Wesnousky, 1990). 1. Neweport-Inglewood. 2. San
Jacinto. 3. Elsinore. 4. Garlock. 5. San Andreas. For (1) and (3), the offset is presented as the geometric mean of two extreme
estimated values (Wesnousky, 1990, table 1). Data point 6: the Dead Sea strike-slip fault (1964–2004). p is the probability of
random occurrence of the correlation coefficient r.
Sea and Jordan valley segments. For the 21 years
studied here, the cumulative seismic moment along the
DSF is presented in Table 1, showing the change in the
distribution of seismic moment between segments that
took place after the M
L
= 5.2 earthquake of 11.2.04.
DISCUSSION
The data presented above for 1984–2004 show some
regularity in temporal trends in the seismic activity
along the DSF, both in the annual number of earth-
quakes and in seismic moment. Although the centers
of seismic activity in the five segments are 50–100
kilometers apart and the earthquakes are very small,
the timing of the peaks of earthquake activity is simi-
lar, within a range of two years (1991–1992) in four of
the five segments and within a range of four years
(1989–1992) in all of the five segments. Simulating a
random process, the probability was calculated of ran-
domly obtaining a situation in which all five segments
have their maximum number of earthquakes in any 4-
year window within 21 years of measurements. The
resulting probability is < 0.004 (we thank D. Steinberg
Z.B. Begin and G. Steinitz. Dead Sea Fault earthquake activity, 1984–2004 11
Table 1
Annual seismic moment (dyne cm) for the period 1984–2004
Segment Annual average of seismic moment × 10
22
dyne cm Seismic moment × 10
22
dyne cm
(Fig. 1) 1984–2003 during 2004
Southern Arava 0.2 0.05
Northern Arava 0.2 0.02
Dead Sea 0.4 66.5
Jordan valley 0.8 8.5
Kinneret 0.2 0.2
Fig. 14. Annual changes in seismic moment release (dyne cm) for 1984–2004. The lines show time intervals in which there is
a statistically significant exponential change in seismic moment; p is the probability of random occurrence of correlation
coefficient r. Note significant multi-year decrease in seismic moment for the DSF (Fig. 14A) during 1984–2003. Most of the
seismic moment released in 2004 is due to M
L
5.2, 4.7, and 4.3 that occurred during February–July.
12 Israel Journal of Earth Sciences Vol. 54, 2005
for the simulation). This indicates the operation of a
mechanism that drives common earthquake activity
along the DSF. This conclusion is supported by the
gradual and consistent decrease of seismic moment for
20 years, during the period 1984–2003.
Such common mechanism is also indicated by the
10-year correlation between the annual number of
earthquakes along the whole DSF and the average Rn
concentration, as measured in one point, within the
Dead Sea segment. It should be noted that many Rn
anomalies in the Dead Sea area are not the result of
earthquakes. Rather, they were shown to precede
earthquakes and were interpreted as signifying tran-
sient stress along the DSF (Steinitz et al., 2003).
Hence, a change in annual Rn concentration seems to
indicate a change in the frequency of occurrence of
stress transients. This leads us to assume that the de-
crease in number of earthquakes along the DSF during
1995–2000 and its increase during 2001–2004 do not
signify an availability of fault planes that are ready to
yield while the regional stress remains constant.
Rather, they reflect general changes in stress.
As it is assumed that most of the smaller earth-
quakes along the DSF are an expression of normal
faulting that is secondary to the main strike-slip move-
ment on the DSF, it is intriguing to realize that their
activity does reflect a large-scale tectonic process
driven by a common source along the 400-km-long
segment of the DSF.
The 20-year decrease in seismic moment and the
decadal decrease in number of earthquakes along the
DSF preceded the M
L
= 5.2 earthquake in the NE Dead
Sea on 11 February 2004. Its fault plane solution indi-
cates that it probably did not occur on one of the main,
N–S aligned, Dead Sea faults but on a plane that
deviates 30° anticlockwise off the trend of the Trans-
form (Salamon, 2004). This earthquake, the strongest
one along the DSF since the M
L
= 5.5 earthquake in the
Dead Sea segment on 18.12.1956, released a seismic
moment of 6.510
23
dyne cm, which is an order of
magnitude greater than the cumulative seismic mo-
ment that had been released in the Dead Sea segment
during the preceding 20 years. In hindsight, it may be
that the gradual decrease in seismic activity along the
DSF during 1991–2000, as well as the slight increase
in seismic activity along the DSF after 1999 that could
be discerned after 2003 (Fig. 7C), could have served as
an indication for increasing probability of the occur-
rence of a strong earthquake after 2003.
The correlation between rate of seismicity (normal-
ized to slip rate) and fault offset (Fig. 12) signifies a
gradual process of decreased seismicity along the DSF
on the scale of millions of years. For other faults, such
decrease was explained by the continuous, long-term
elimination of irregularities (Wesnouski, 1990; Stirling
et al., 1996). Hence, the rate of seismicity along strike-
slip faults evolves with time, and we may now apply
this analysis to the Dead Sea Fault as well. This long-
term evolution of seismicity means that the present
seismic activity along a strike-slip fault system is the
result of both its initial fault pattern and the unidirec-
tional slow process through which it becomes less
complex, with earthquakes converging towards its
main faults (Ben-Zion et al., 1999). This means that
the present seismicity of these strike-slip faults is
affected by their past.
ACKNOWLEDGMENTS
Helpful suggestions by G. Baer, Y. Ben Zion, A.
Hofstetter, V. Lyakhovsy, A. Shapira, and A. Salamon
are gratefully acknowledged. Comments by two anony-
mous reviewers contributed much to the improvement
of the manuscript. We thank D. Steinberg for his help
with some statistical aspects of the study. We are
grateful to L. Feldman for her effective asstance.
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... And finally, geodetic measurements are consistent and confirm the left-lateral slip as well as the slip rate from other palaeoseismic evidence of 4±1 mm/yr (Le Beon et al., 2006;McClusky et al., 2003;Reilinger et al., 2006;Wdowinski et al., 2004). This rate, as well as uniform Gutenberg-Richter frequency-magnitude relation, indicate stable tectonic regime in the last 60 ka (Begin et al., 2005;Hamiel et al., 2008). ...
... Using an 8-year record of Rn, obtained next to a major active boundary fault of the DST, a statistically significant relation between multi-day Rn signals and earthquakes in the nearby sector of the DSR was demonstrated by Steinitz et al. (2003). In these works the establishment of the geodynamic nature of the signatures and signals is based on negation of atmospheric influence, analyzing radon signatures in the geological, spatial, time and frequency domains and, primarily, on correlating radon with geophysical phenomena, and specifically the correlation to earthquakes (Steinitz et al., 2003;Begin and Steinitz, 2005). ...
... The seismic activity at the DST in general is small compared to other transform faults (Begin & Steinitz 2005). However, these authors showed that the relationship between fault offset and number of earthquakes proposed by Wesnousky (1990) for California, is also valid for the DST. ...
... However, these authors showed that the relationship between fault offset and number of earthquakes proposed by Wesnousky (1990) for California, is also valid for the DST. In several studies of the seismicity along the DST (van Eck & Hofstetter 1989, 1990Aldersons et al. 2003;Begin & Steinitz 2005) the DSB is found to be one of the main regions of seismic activity. Using data from stations on both sides of the basin, Aldersons et al. (2003) determined the depth of the local events. ...
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Thesis
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Technical Report
Full-text available
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Examining the temporal variation of the decomposed components at a site suggests an association, or even influence, between the overall level of the long-term variation of radon and the amplitude of the daily variation. The daily mean level of radon and the daily standard deviation vary periodically throughout the year. Such a coupling cannot be envisaged operating on a gas (geogas) system with radon (half-life = 3.82 days) as a trace component, but rather operating on the radon source (solid) system. The generator of the long-term (SR) variation is separate from the generator of the DR signal, but both seem to be indirectly linked. Time offsets of hours are observed among time series of the measured signal from the sites. The lag was investigated for the measured signal and separately for the decomposed MD and DR components, using consecutive 20-day long time intervals. The resulting time series of the lag show that systematic time offsets (1-3 hours) occur, whereby the radon signal always occurs first at the easternmost site. The MD component shows a significant gradual long-term varying lag of 0-12 hours, and the DR component a significant stable 1-3 hour lag. This dissimilarity between the lag of the MD and DR components is enhanced when examining the lag of the difference between consecutive measurements. In this case of the MD signal a significant lag exists, in the range of 0.5-6 hours. In the case of DR signal a significant correlation is not obtained throughout. These differences in the statistical behavior probably point to a fundamental difference in the driving mechanism of MD and DR signals. Diurnal (24-hours) and semidiurnal (12-hours) constituents characterize the periodic aspect of the DR component in the time series of radon. Diurnal constituents typical for gravity related phenomena are absent. The amplitudes of these constituents, calculated for consecutive 512-hour long time intervals, exhibit at all sites a similar regular temporal variation of the amplitudes of the daily cyclic constituents, clearly reflecting a seasonal pattern. The co-occurring amplitudes of the diurnal and semidiurnal constituents define an overall linear correlation with a slope in the range 0.3-0.8. This result points to a systematic and fundamental statistical property in the frequency domain of the radon time series, reflecting a specific external driving mechanism. Correlation analysis between radon level and ambient atmospheric conditions (pressure, temperature) indicate that the latter cannot be considered as the main driving force for the observed phenomena. Analyzing the diurnal patterns of pressure and temperature in the frequency domain, in the same manner as for radon, shows clearly that linear co-variation of diurnal and a semidiurnal component does not occur in these time series. This dissimilarity in the statistical properties of the time series corroborates the assertion that radon variation in the geogas system is not driven by the variation of pressure and temperature. Radon signals in the geogas of the Elat granite behave as system that is driven by several geophysical processes. This proposition relies on the following: 1. The statistical properties of components within the time series and among them indicate that different processes are responsible for the periodic (SR and DR) and for the non-periodic MD variation. 2. The forcing processes are external to the local rock system and are reacting with the rock system. 3. The statistical properties in the frequency domain imply that a periodic process drives the DR with a fundamental diurnal frequency. This may also relate to the SR variation, placing both components as mirroring processes related to the rotation of the earth around itself and around the sun. 4. These processes are not influencing the radon signals through interaction with the gas phase in the pores and crevices of rock system, but are rather acting on the release of the radon from its source into the geogas. The resulting measured signal is a superposition of the different processes acting on the source of the radon in the rock system. 5. There is partial interaction between the processes, leading to non-linear effects. The most prominent interaction is the annual (seasonal) variation, which influences both the DR and the non-periodic MD signal. 6. The non-periodic MD signals can probably be associated with geophysical transients of a mechanical nature, i.e. geodynamic. This would be in line with their similarity to MD signals from the NW Dead Sea that have been correlated with seismic activity of the Dead Sea transform. The results indicate that hitherto unrecognized dynamic processes are driving the radon signal in the Elat granite pluton, in the uppermost crustal level of the area. Radon, as a trace component in the geogas filling the permeable system in the rock, is a sensitive proxy of these processes. As far as known such results and phenomena are specific to radon. This raises the question whether they are related to the special quality of radon as being a heavy noble gas and/or to the fact that nuclear processes govern its formation and disintegration. Furthermore, so far the phenomena are observed in the natural geological environment, which raises the question as to the role and interaction of mineral lattices. The results present new prospects for the investigation of radon phenomena in the frame of interacting geodynamic (tectonic?) and earth-sun system related geophysical processes.
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Temporal variations of radon in the geological environment (upper crust) are frequent and recognized as unique in terms of the signals encountered and for the lack of substantial and generally applicable explanations. The phenomena observed at the Roded site, located in arid southern Israel, emphasize this situation. Monitoring of radon during more than 10 years is carried out in massive meta-diorite of the Precambrian basement block of Roded. Measurement is conducted using an alpha detector at a resolution of 15-min, lowered in a borehole at a depth of 9 m, within a PVC casing to that depth. Systematic temporal variation patterns, manifesting large relative signals are composed of sub-daily (SDR) radon, multi-day (MD) and annual (AR) signals. The overall variation in dominated by the intense SDR signals which occur in some days, and may vary from background levels (5 counts or less) to peak values (attaining >1000 counts) and back to background in an interval of 6 to 12 h. Intervals of up to several tens of days without significant SDR signals interchange with times of intense daily occurrences of such signals. Their occurrence indicates very fast variations of radiation from radon at the point of measurement. The peak times, within the diurnal 24-h cycle of SDR signals occur preferentially in the interval of 14–16 h (UT+2). Spectral analysis indicates: (a) A diurnal periodicity composed of a primary 24-h and a secondary 12-h periodicity, which are attributed to the solar tide constituents S1 and S2. Tidal constituents indicative for gravity tide (O1, M2) are lacking; (b) An annual periodicity. A compound relation among the diurnal and annual periodicity is indicated by: (a) Wavelet (CWT) analysis showing an overall annual structure with a modulation of the S1 and S2 periodicities; (b) FFT analysis using consecutive 21.3-day long time intervals shows that the amplitudes of S1 and S2 vary in an annual pattern, with relatively high values in summer. The phase of S1 and S2 and S3 shows a systematic multi-year variation. Existing frames of reference of geophysical processes cannot explain the highly systematic phenomena. It is suggested that the significant signatures of the periodic phenomena and their modulations are reflecting a direct link with solar radiation tide.
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Four independent distributions of seismicity in the Dead Sea area underline the occurrence of lower-crustal seismic activity down-to at least 27 km and possibly as deep as 33.6 km. From these distributions, the seismogenic thickness is estimated to be 28.4 ± 2.2 km. The existence of a seismogenic zone extending deep into the lower crust is consistent with an average heat flow of only 40–45 mWm−2 over most regions of Israel, and around 40 mWm−2 in the Dead Sea area in particular. The seismogenic thickness in the Dead Sea area is thus nearly twice the average seismogenic thickness of 15 km observed in southern California. The fact that some seismic activity occurs down-to the Moho in the Dead Sea area suggests that the state of fully plastic deformation is probably not reached in the crust under the seismogenic zone. The ISC – GEM (Storchak et al. 2013) relocation of the MW 6.3 earthquake of 11 July 1927 from regional and teleseismic instrumental data resulted in a well-constrained epicenter located in the Jordan Valley, not far from the epicenter reported in the 1927 bulletin of the ISS. Since the causative fault of this earthquake is likely to be the Dead Sea transform, we propose a preferred epicenter at 31.92°N–35.56°E. The focal depth determined instrumentally by the ISC – GEM relocation is 15 ± 6 km, and we found an average macroseismic depth of 21.5 ± 2.5 km. Our results as a whole underline also the seismogenic importance of the transition between the upper and the lower crust in the Dead Sea area for moderate and probably also for large earthquakes.
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Recent advances in neotectonic, paleoseismic, and other studies of the Dead Sea Transform (DST) allow evaluating the lateral slip rate over different time periods, and also raise new questions. The long-term slip rate over time scales of millions of years represents continuous plate motions that are expected to vary slowly. GPS observations reveal the current plate motions which probably reflect the last 0.5-1 Ma. These results indicate that approximately 1-2 Ma ago the slip rate slowed to 4-5.5 mm/y, compared with the average rate of 6-7 mm/y over the last 5 Ma. At the same time the Euler pole of the Sinai-Arabia motion shifted eastward, continuing a longer term trend that began >5 Ma ago, which records an increase of the components of transverse motion along the N and S parts of the DST.The short-term slip rate over the last several kyr to tens of kyr is dominated by discrete earthquake-generating slip events that are distributed irregularly in space and time. These events relieve, to various extents, the shearing of the plate margins that is built up as a result of the continuing plate motions during the inter-seismic periods when the faults along the DST are locked. Offsets of various markers and variations in the earthquake distribution show that over the last ca. 2 kyr (perhaps more), which is not much longer than the recurrence times of the strongest earthquakes, the lateral slip rate varied irregularly along the DST. On short time scales, local slip rates could deviate by up to 50% from the plate motions in that period. Some findings raise the possibility that the magnitude-frequency relation deviated from the Gutenberg-Richter relation, an issue that requires further study.Offsets of geomorphic markers show that in the last 50 kyr and more, much longer than the recurrence times of the strongest earthquakes, the cumulative slip at any place was quite close to the plate motions during this period. Over this time scale the residual short-term variations of the slip become small compared with the total slip. This should be reconciled with the record of sediments disturbed by seismic shaking that suggests that the frequency of strong earthquakes varied considerably and was particularly low 15-40 kyr ago, at least in the Dead Sea basin. This raises questions regarding the magnitudes of past strongest earthquakes and the role of aseismic slip. Both of these issues require further study.
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Crustal deformation patterns are affected by multiscale granulation and healing processes associated with phase transitions between continuum and discrete states of rocks. The ongoing continuum-discrete transitions are accompanied by progressive evolution of disordered fault networks to dominant localized fault zones, development of bimaterial interfaces, and increasing dynamic weakening of fault surfaces. Results on individual fault zones point to three general dynamic regimes. The first is associated with broad range of heterogeneities, little dynamic weakening, power law frequency-size statistics, temporal clustering of intermediate and large events, and accelerated seismic release before large earthquakes. The second is associated with relatively uniform localized structures, significant dynamic weakening, characteristic earthquake statistics, and quasi-periodic temporal occurrence of large events without precursory accelerated release. For a range of conditions, the fault zone response can switch back and forth between the foregoing two dynamic regimes. Higher temperature, fluid content, and thickness of sedimentary cover reduce the seismic coupling in a region and change the properties of local earthquake sequences. Brittle regions with high seismic coupling have few foreshocks and long-duration aftershock sequences with high event productivity, whereas more viscous regions with low seismic coupling have increased foreshocks activity and low-productivity aftershock sequences or swarms. The results provide criteria for organizing data in classes associated with different evolutionary stages and different regional conditions. An ability to recognize the dynamic regime of a given fault zone or a region can increase the information content of the data and lead to improved strategies for seismic hazard assessment.
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The Nuweiba earthquake (1995 November 22; Mw= 7.2), the largest seismic event along the Dead Sea Transform (DST) in at least 160 yr, ruptured 45–50 km along the Aragonese segment of the left-stepping strike-slip fault system occupying the gulf of Elat/Aqaba (southern segment of the DST). The rupture initiated in a partly normal, low-slip first subevent near the southern end of the fault and propagated unilaterally north-northeastward as a high-slip, nearly pure sinistral second subevent, which was responsible for over 90 per cent of the total seismic moment. The source mechanism and slip distribution, derived from inversion of teleseismic broad-band waveforms, are used to construct a 3-D elastic model of the earthquake based on the boundary elements method, resulting in the full 3-D displacement and stress fields induced by the earthquake. In the absence of sufficient Global Positioning System data, the only other constraints on the geometry and slip distribution of the rupture are provided by interferometric synthetic aperture radar (InSAR) measurements spanning the coseismic and early post-seismic period. We calculate simulated interferograms by transforming the calculated surface displacement field into the satellite coordinate system and comparing them with the observed interferograms. The model parameters are then iteratively modified until a best-fitting model is obtained, providing a refined set of static source parameters for the mainshock. This model is then used to calculate the static Coulomb stress changes induced by the mainshock on the step-over faults, suggesting that the major (Mw≥ 5) aftershocks in the first eight post-seismic months were triggered by small changes (<1 bar) in the left-lateral Coulomb stress, with effective friction coefficient not higher than 0.2. Aftershock distribution and mechanisms indicate that the available Coulomb stress dropped below the frictional strength of the fault but was not complete.
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The Dead Sea Transform Fault constitutes the northwestern boundary of the Arabian plate, accommodating the plate’s lateral movement relative to the African plate. A complete and homogeneous catalogue of historical earthquakes has been compiled and used in the subdivision of the fault area into the following segments: 1) Araba segment, which extends along Wadi Araba and the southernmost part of the Dead Sea (29.5°-31.3°N) and trends SSW-NNE with scarce historical and instrumental seismicity; 2) Jordan-valley segment, which extends along the central and northern parts of the Dead Sea and the Jordan valley to the Huleh depression (31.3°-33.1° N) and trends S-N with moderate historical seismicity; 3) Beqa’a segment, which extends along the western margin of the Beqa’a valley in Lebanon (33.1°-34.5°N) and trends SSW-NNE with strong historical seismicity; 4) El-Ghab segment, which extends along the eastern flank of the coastal mountain range of Syria (34.5°-35.8°N) and trends S-N with moderate historical seismicity; 5) Karasu segment, which extends along the Karasu valley in SE Turkey (35.8°-37.3°N) and trends SSW-NNE, exhibiting the strongest historical seismicity of the area. Probabilities for the generation of strong (M > 6.0) earthquakes in these segments during the next decade are given, by the application of the regional time and magnitude predictable model.
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The long-term recurrence patterns of past earthquakes are of considerable consequence for hazard assessments, and have implications for earthquake physics. We introduce a rigorously dated record of earthquakes from an extensive number of well-preserved preseismic and postseismic precipitates from caves located off the Dead Sea transform. We dated events directly at the paleoseismic contact by means of a novel correlation method with the oxygen isotope record of the speleothems recovered in one of the caves. Within the 185 k.y. covered, we dated 38 seismite samples. These stem from 13 18 earthquakes with a mean recurrence interval of ˜10 14 k.y. We show that the deformational events dated in the study caves complement independent near-fault paleoseismic records by temporal correlation with the earthquakes recorded therein. This opens up a significant new avenue of earthquake research that will provide precise dating and observational constraints on large infrequent earthquakes.
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A preliminary survey of microearthquake activity along the central part of the Dead Sea Jordan Valley Rift in Israel revealed the occurrence of events -0.5 to 1.5 in magnitude, clustered in the structurally more complex zones. These microearthquakes appear to confirm the existence of recent crustal activity in this region, as inferred from geologic, geomorphologic, geodetic, and archeologic evidence. This note reports the first results of a survey of microearthquake activity between the Mediterranean Sea and the Dead Sea Rift. The data presented below were recorded mainly along the central part of the rift zone in Israel, during the period of September 1972 through February 1973.
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We discuss the implications of 56 kyr of paleoseismic data from a fault on the southern segment of the Arava Fault system in Israel. At least nine events are evident, beginning 37 ka. We study in detail the frequency-magnitude relation for the fault and develop a Bayesian analysis to compare the characteristic earthquake (CE) model and the Gutenberg-Richter (GR) model. Our analysis leads to the con-clusion that there was a change in seismic behavior at about 14 ka. From -37 ka to 14 ka, the seismic activity is best described by the CE model. From -14 ka to the present, there is no strong indication favoring one model over the other; the earth-quake record is somewhat more consistent with the classical GR equation than with the CE model. If one does assume that the CE model is appropriate for the younger episode, then there is evidence of a change in the characteristic magnitude. Thus, there is evidence of a change in earthquake behavior on the fault segment --14 ka.
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Recent surface and subsurface geological investigations in Israel and Jordan provide new data for the re-examination of Dubertret's (1932) hypothesis of the left-hand shear along the Dead Sea rift. It is found that while none of the pre-Tertiary sedimentary or igneous rock units extend right across the rift, all of them resume a reasonable palaeographical configuration once the east side of the rift is placed 105 km south of its present position. It is therefore concluded that the 105 km post-Cretaceous, left-hand shear along the Dead Sea rift is well established. The 40 to 45 km offset of Miocene rocks and smaller offsets of younger features indicate an average shear movement rate of 0.4 to 0.6 cm a-1 during the last 7 to 10 Ma. Unfortunately, the 60 km pre-Miocene movement cannot be dated yet. Along the Arava and Gulf of Aqaba and in Lebanon the shear is divided over a wide fault zone within and outside the rift.
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Linear and quadratic scaling relations between potency P 0 and local magnitude M L for southern California earthquakes are derived using observed data of small events (1.0 < M L < 3.5) recorded in the Cajon Pass borehole and moderate events (3.5 < M L < 6.0) recorded by the broad-band TERRAscope/TriNet network. The derived relations are extended to M L = 7.0 and compared with observed potency-magnitude values of four earthquakes in the extended range. The results indicate that a linear scaling relation can describe accurately data extending only over 2-3 orders of magnitudes. The best-fitting slope of a linear log P 0 vs M L scaling for the small Cajon Pass events is about 1.0, while the slope for the 3.5 < M L < 6.0 events is about 1.34. A quadratic relation can fit the data well over the entire 1.0 < M L < 7.0 magnitude range. The results may be explained in terms of a continuous transition from a limiting scaling P 0 ~ (rupture area) for highly disordered small events, to a limiting scaling P 0 ~ (rupture area times slip) for crack-like large events. Such a transition is expected to characterize evolving seismicity on heterogeneous faults, where small events propagate in (and are arrested by) a rough fluctuating stress field, while large events propagate across a relatively smooth correlated field.