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2
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0028862534
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R. M. Nadeau, W. Foxall, T. V. McEvilly, ibid. 267, 503 (1995); R. M. Nadeau and T. V. McEvilly, Bull. Seismol. Soc. Am. 87, 1463 (1997).
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Nadeau, R.M.1
Foxall, W.2
McEvilly, T.V.3
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3
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0031462641
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R. M. Nadeau, W. Foxall, T. V. McEvilly, ibid. 267, 503 (1995); R. M. Nadeau and T. V. McEvilly, Bull. Seismol. Soc. Am. 87, 1463 (1997).
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Bull. Seismol. Soc. Am.
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Nadeau, R.M.1
McEvilly, T.V.2
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5
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0039366205
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F. Y. Cheng and M. S. Sheu, Eds. Elsevier, Oxford
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W. L. Ellsworth, in Urban Disaster Mitigation: The Role of Science and Technology, F. Y. Cheng and M. S. Sheu, Eds. (Elsevier, Oxford, 1995); D. P. Schaff, G. C. Beroza, B. E. Shaw, Geophys. Res. Lett. 25, 4549 (1998). In sequences of similar aftershocks, seismic moment release and recurrence rates were related to measured surface deformation and loading rate at depth to investigate postseismic deformation. An aftershock sequence differs from the more nearly steady-state microearthquake occurrence seen at Parkfield.
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(1995)
Urban Disaster Mitigation: The Role of Science and Technology
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Ellsworth, W.L.1
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6
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0032535242
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In sequences of similar aftershocks, seismic moment release and recurrence rates were related to measured surface deformation and loading rate at depth to investigate postseismic deformation. An aftershock sequence differs from the more nearly steady-state microearthquake occurrence seen at Parkfield
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W. L. Ellsworth, in Urban Disaster Mitigation: The Role of Science and Technology, F. Y. Cheng and M. S. Sheu, Eds. (Elsevier, Oxford, 1995); D. P. Schaff, G. C. Beroza, B. E. Shaw, Geophys. Res. Lett. 25, 4549 (1998). In sequences of similar aftershocks, seismic moment release and recurrence rates were related to measured surface deformation and loading rate at depth to investigate postseismic deformation. An aftershock sequence differs from the more nearly steady-state microearthquake occurrence seen at Parkfield.
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(1998)
Geophys. Res. Lett.
, vol.25
, pp. 4549
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Schaff, D.P.1
Beroza, G.C.2
Shaw, B.E.3
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8
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0031445166
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E. Karageorgi, T. V. McEvilly, R. Clymer, Bull. Seismol. Soc. Am. 87, 39 (1997); E. G. Quilty and E. A. Roeloffs, ibid., p. 310.
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Bull. Seismol. Soc. Am.
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, pp. 39
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Karageorgi, E.1
McEvilly, T.V.2
Clymer, R.3
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11
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0345190625
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av, for subsets before and after 1992, broadens the peak. The combined effects are evident in Fig. 2
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av, for subsets before and after 1992, broadens the peak. The combined effects are evident in Fig. 2.
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-
-
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12
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0344328215
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av
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av.
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14
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0345622818
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unpublished data. Short baseline creep- meters do not measure the off-fault deformation present in the creep-to-locked transition zone
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J. Langbein, unpublished data. Short baseline creep- meters do not measure the off-fault deformation present in the creep-to-locked transition zone.
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Langbein, J.1
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15
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0345622817
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i is unknown because the next event in the sequence has not yet occurred
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i is unknown because the next event in the sequence has not yet occurred.
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18
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0000565130
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i, supporting a fault-heating process. Laboratory data suggest 3 to 8% for a 10-fold increase in recurrence interval [J. Dieterich, J. Geophys. Res. 77, 3690 (1972); C. Scholl, P. Molnar, T. Johnson, ibid., p. 6382; C. Scholz and T. Engelder, Int. J. Rock Mech. Miner. Sci. 13, 149 (1976)].
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(1972)
J. Geophys. Res.
, vol.77
, pp. 3690
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Dieterich, J.1
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19
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0041145543
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i, supporting a fault-heating process. Laboratory data suggest 3 to 8% for a 10-fold increase in recurrence interval [J. Dieterich, J. Geophys. Res. 77, 3690 (1972); C. Scholl, P. Molnar, T. Johnson, ibid., p. 6382; C. Scholz and T. Engelder, Int. J. Rock Mech. Miner. Sci. 13, 149 (1976)].
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J. Geophys. Res.
, pp. 6382
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Scholl, C.1
Molnar, P.2
Johnson, T.3
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20
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0016952610
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i, supporting a fault-heating process. Laboratory data suggest 3 to 8% for a 10-fold increase in recurrence interval [J. Dieterich, J. Geophys. Res. 77, 3690 (1972); C. Scholl, P. Molnar, T. Johnson, ibid., p. 6382; C. Scholz and T. Engelder, Int. J. Rock Mech. Miner. Sci. 13, 149 (1976)].
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(1976)
Int. J. Rock Mech. Miner. Sci.
, vol.13
, pp. 149
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Scholz, C.1
Engelder, T.2
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21
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0345190623
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note
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Supported by the U.S. Geological Survey through award 1434-95-G2540. Data processing at the Lawrence Berkeley National Laboratory was supported by the U.S. Department of Energy Office of Basic Energy Sciences. Partial support (R.N.) came from the Lawrence Livermore National Laboratory Institute of Geophysics and Planetary Physics Campus-Laboratory Collaboration project.
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