The new Swedish Seismic Network
Reynir Böðvarsson
Introduction
The history of instrumental seismology in Sweden began
1904 when the 1000 kg Wiechert
horizontal pendulum was installed in Uppsala.
Fig. 1. Station locations in the new Swedish network.
The new Swedish National Seismic
Network (SNSN), which is a digital broadband seismic network, is now under
construction.
The first part of the network was put into operation in 1998. This part
of the network consists of six station at approximately the same locations
as the stations in the old analog network constructed by Marcus Båth
in the 1960s and are shown red squares in figure 1.
Additionally twelve stations are under construction along the coast of the
Gulf of Bothnia. This is a separate project financed by the Swedish Natural
Science Research Council (NFR), the Knut and Alice Wallenberg Foundation and
the Swedish Nuclear Fuel and Waste Management Co (SKB). The main purpose of
this network is to study microearthquake activity along the Coast of the
Gulf of Bothnia to gain better understanding of the ongoing deformation
processes in that area. These stations are shown as blue triangles in figure 1.
All stations are equipped
with Güralp CMG-3ESPD broadband seismometers with digital output.
These seismometers are flat to velocity in the period range from 0.02 to
30 seconds. The digital data is time stamped within the sensor using the
GPS satellite system. The sampling frequency will be 100 sps at all stations.
The data acquisition system
used is the so called SIL system which was developed within the SIL project,
a joint Nordic project for earthquake prediction research in Iceland, 1988
through 1992 (Stefánsson et al 1993, Böðvarsson et al 1996,
1999). The main achievement of the SIL-project was to establish an automatic
earthquake data acquisition and evaluation system, the SIL-system. As detailed
plans were made for the SIL project, the importance of microearthquakes
for understanding the ongoing deformation processes within the crust were
recognized. It was recognized that the recording of earthquakes down to
magnitude and retrieval of source information
from these events would require a new seismic network design (Stefánsson
et al 1986, Böðvarsson 1987). The rapid evolution in computer
and communication technology and the introduction of inexpensive but powerful
personal computers allowed for such a design of the SIL network (Böðvarsson
et al 1996, 1999).
The network operation scheme
Teleseismic events will primary
be recorded at the old 6 station locations. During some periods, teleseismic
events will probably also be recorded at the remaining stations when research
funds are available. Teleseismic events will primary be recorded using
information available on Internet. The so called ``E'' type messages from
USGS and NEIC, containing a single line of hypocenter and magnitude information
on recent earthquakes, are received via electronic mail. Event information
from different European networks will also be used for earthquakes occurring
at closer distances. A selection programme reads the messages and selects
events that fulfill certain criteria of magnitude and epicentral distance.
The programme will use the iasp91 traveltime tables (Kennett and Engdahl,
1991) to compute the first arrival time at each station. The teleseismic
body wave data are fetched with a sampling rate of 20 samples per seconds
and the surface wave data with a sampling rate of 4 samples per second.
Regarding local and regional
earthquakes, all 18 stations will be operated as a single seismological
network providing automatic location and fault plane solution of all located
earthquakes. As in the SIL system in Iceland the automatic analysis performed
by the system will be divided into four categories: single- and multi-station
analysis, multi-event analysis and the alert analysis. Single-station analysis
is performed at each site on data recorded by that station. Multi-station
and multi-event analysis is done at the center where data from more than
one station are available. The alert monitoring is also done at the center,
using parameters derived from the single- and multi-station analysis. A
schematic description of the data flow in the system is given in figure 2.
Fig. 2, Processes and data flow in the SIL data acquisition system.
From Böðvarsson et al (1999).
The software at the site can
be divided into two categories: utility processes and application processes.
The utility processes are general data management processes, designed for
flexibility and valid for any type of data acquisition. The application
processes read a channel of data stream as if it were an endless file.
Channels are opened as regular files would be, by a call to the specific
function in the utility library. The most recent part of the data are kept
in shared memory for fastest possible access.
The communication between
the center and the stations is designed to be independent of the physical
way it is realized. Unix utilities are used throughout, providing the best
possible portability of the software. To minimize data transmission costs
the SIL system uses single-station phase detections and multi-station event
selection. The basis of this concept is to treat all transients detected
at the stations as if they were phases associated with real earthquakes.
The detector uses a simple comparison of power in two adjacent windows
in six frequency bands of the seismic trace. This is similar to the STA/LTA
approach but in our case the time-windows used are short and both of the
same length. Selected windows around the detected transients are processed
in a manner one would process a true seismic phase and the results stored
in a compact structure, called a phase log. Each phase log entry is only
128 bytes long and is therefore inexpensive to transmit to the center.
The detection thresholds can therefore be set very low, allowing smaller
earthquakes to be detected. The phase logs will be transmitted to the center
once every hour. Each phase log includes onset time, duration, reference
to previous and following phases, type of phase (P or S), signal and noise
averages, maximum amplitude, azimuth and coherency (Roberts et al 1989)
and spectral parameters including DC-level and corner frequency.
Selection of waveform data to be transferred
from the stations is carried out automatically by the selector software
at the center. At the center, the phase logs from different stations are
merged into a single time-ordered list. The first step of the selection
process is to search for time intervals which contain two or more phase
detections that may originate from the same seismic source. The phase detections
in this time interval are then submitted to the iterative location, phase
association and phase truncation procedure as explained below.
The principles for the step from
a list of phase detections to a list of earthquakes or seismic events are
described by (Slunga 1980, Böðvarsson et al 1999). In short each
combination of three observations (onset times of P or S phases and azimuths
of P phases) is taken as defining the initial location of an earthquake
and is then followed by iterative location and phase association and truncation.
This procedure may lead to a ''kinematic event`` (no dynamic constrains)
defined by three or more observations. The list of kinematic events contains
a large proportion of false events due to random coincidences of observations.
Therefore each event is assigned a quality measure. Ideally the quality
of an event should measure the probability that the event is a true seismic
event. The computation of quality is based on both kinematic considerations
and analysis of the amplitudes of the detected phases (dynamic information).
Apart from locating the earthquake, the routine analysis
performed on every recorded event will include estimation of the fault
plane solutions for the earthquake. The estimation of focal mechanism and
source parameters are based on results of the spectral analysis of short
data segments containing the direct P and S wave arrivals. The spectral
estimation is done at the site stations, using windows around the automatic
time picks, and repeated at the center after manual refinement of arrival
time readings. The low frequency amplitude of each phase is determined
by fitting a three parameter model to the observed spectra (Boatwright
1978). To estimate the fault plane solution for the earthquake a systematic
search over strike, dip and rake is performed. For each combination of
the three source angles, the misfit between observed and predicted spectral
amplitudes is calculated. In addition to the single best fitting solution,
all solutions that fit the observed polarities and have amplitude misfit
less than a predefined threshold value are taken as acceptable (Slunga
1981).
The alert system is a collection
of routines for monitoring extracted parameters in selected regions and
sites. For this purpose, Sweden will be divided into a number of regions
and different alert thresholds assigned to each region. The parameters
are extracted from the results of the analysis described above and from
dedicated alert detectors at the sites. The alert system will be started
at regular intervals and for each event defined by the multi-station analysis.
Five parameters will be monitored for each region. These are M , the local
magnitude of individual earthquakes, N , the number of earthquakes in a
time interval, S, a dimensionless measure of moment release during the
same time interval and time-weighted measures of the number of events and
accumulated moment release (Böðvarsson et al 1999). The purpose
of the SNSN alert system is to provide information about the seismic activity
in different regions for increased attention of the network operators.
At the SNSN center the algorithm
described by Slunga et al (1995) will be used to simultaneously determine
absolute and accurate relative locations of clusters of similar earthquakes.
An example of the application of the relative location algorithm to a group
of earthquakes in the Tjörnes fracture zone in Iceland is shown in
Figure 3. After relocation the epicenters of the 18 successfully located
events lie on an approximately 1 km long line segment (Figure 3.a). Assuming
that all the earthquakes occurred on the same fault, the attitude of the
fault can be estimated by fitting a plane through the accurately determined
hypocenters. The strike of the best fitting plane through the group is
,
similar to the strike of the main transform faults of the TFZ.
Fig. 3. The relative location
of a group of 18 earthquakes in the Tjörnes fracture zone. (a) shows
a mapview of the epicenters after relocation, X is east, Y is north. In
(b) the hypocenters are viewed along the strike of the best fitting plane
through the group. Z is depth and X' is horizontal and orthogonal to the
strike. (c) shows the poles to all planes through the hypocenter group,
such that the mean distance of the 18 earthquakes from the plane is less
than 50~m, plotted on an equal area projection of the lower hemisphere.
From Böðvarsson et al (1999).
I would like to thank my colleagues
Ragnar Slunga, Björn Lund, Conny Holmqvist, Sverker Olsson, Hans Palm
and Stefán Böðvarsson who participate actively in the network
construction process. Special thanks to the land-owners and others that are
housing our stations.
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