GPS OBSERVATIONS OF POSTSEISMIC CRUSTAL MOVEMENTS IN THE FOCAL REGIONOF THE 1995 HYOGO-KEN-NANBU EARTHQUAKE - STATIC AND REAL-TIME KINEMATIC GPS OBSERVATIONS
K. Hirahara et al., GPS OBSERVATIONS OF POSTSEISMIC CRUSTAL MOVEMENTS IN THE FOCAL REGIONOF THE 1995 HYOGO-KEN-NANBU EARTHQUAKE - STATIC AND REAL-TIME KINEMATIC GPS OBSERVATIONS, Journal of Physics of the Earth, 44(4), 1996, pp. 301-315
Post-seismic deformations in the focal region of the 1995 Hyogo-ken Na
nbu earthquake (M=7.2), in southwest Japan, which occurred on January
17 (JST), were observed with GPS observations. We deployed more than 3
0 GPS stations in and around the area of aftershock activity within se
veral days after the occurrence of the earthquake. First the data were
stored and manually collected at the observation sites, but by the mi
ddle of February the data at most of sites were started to be telemete
red through public phone lines to data centers. GPS observations conti
nued until the end of March, except for 4 sites left active for monito
ring long-term deformations. We used two types of GPS observations, us
ual static and real-time kinematic GPS observations. Static day-by-day
analyses, which are based on 24-h data sampled every 30 s, show the d
eformation associated with post-seismic readjustment with a relaxation
time of about 70 days and with an amplitude of 1-2 cm in the area clo
se to the epicenter. Also, rapid movements were observed just after th
e occurrence of the earthquake. However, since our analyses are only p
reliminary, further analyses are needed to clarify these observations
and to investigate models of post-seismic deformations. Real-time kine
matic GPS observations, which is a new type of GPS observations, were
made every is from February 9 to March 22 for detecting possible rapid
relative movements between two sites across the surface fault trace o
n Awaji Island and across the other fault, the Arima-Takatsuki Tectoni
c Fault on the Kobe side. Present real-time kinematic GPS observations
show scatters with the amplitude of 0.5-3.0 cm depending on component
s and baseline lengths. Any motions with amplitudes larger than these
noise levels could not be detected during the observation period.