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1
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0022190020
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P. W. Lipman, J. P. Lockwood, R. T. Okamura, D. A. Swanson, K. M. Yamashita, U.S. Geol. Surv. Prof. Pap. 1276, 1 (1985).
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(1985)
U.S. Geol. Surv. Prof. Pap.
, vol.1276
, pp. 1
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Lipman, P.W.1
Lockwood, J.P.2
Okamura, R.T.3
Swanson, D.A.4
Yamashita, K.M.5
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2
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0342931845
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Between June 1976 and December 1982, 24 intrusion events occurred, but only 5 led to eruptions
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Between June 1976 and December 1982, 24 intrusion events occurred, but only 5 led to eruptions.
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5
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0023508876
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F. W. Klein, R. Y. Koyanagi, J. S. Nakata, W. R. Tanigawa, U.S. Geol. Surv. Prof. Pap. 1350, 1019 (1987).
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(1987)
U.S. Geol. Surv. Prof. Pap.
, vol.1350
, pp. 1019
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Klein, F.W.1
Koyanagi, R.Y.2
Nakata, J.S.3
Tanigawa, W.R.4
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11
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0025244711
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P. T. Delaney, R. S. Fiske, A. Miklius, A. T. Okamura, M. K. Sako, Science 247, 1311 (1990).
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(1990)
Science
, vol.247
, pp. 1311
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Delaney, P.T.1
Fiske, R.S.2
Miklius, A.3
Okamura, A.T.4
Sako, M.K.5
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17
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0027884372
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P. T. Delaney, A. Miklius, T. Árnadóttir, A. T. Okamura, M. Sako, J. Geophys. Res. 98, 17801 (1993).
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(1993)
J. Geophys. Res.
, vol.98
, pp. 17801
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Delaney, P.T.1
Miklius, A.2
Árnadóttir, T.3
Okamura, A.T.4
Sako, M.5
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18
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0028837794
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S. Owen et al., Science 267, 1328 (1995).
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(1995)
Science
, vol.267
, pp. 1328
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Owen, S.1
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24
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0342497650
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note
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i are the measurement errors. By using the relative displacements rather than displacement vectors derived from relative displacements, we ensure that the influence of anomalous measurements remains confined to the baselines.
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25
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0024231584
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This method [P. Segall and M. V. Matthews, J. Geophys. Res. 93, 14954 (1988)] consists of adjusting the unknown rigid body motion of the velocity field with reference to an assumed deformation model.
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(1988)
J. Geophys. Res.
, vol.93
, pp. 14954
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Segall, P.1
Matthews, M.V.2
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26
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0019561477
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This sharp subsidence in level profile BB′ is associated with surface cracking that occurred during the August 1981 southwest intrusion. The discontinuity of the profile cannot be explained by a simple dike model and is attributed to inelastic deformations and faulting [D. D. Pollard, P. T. Delaney, W. A. Duffield, E. T. Endo, A. T. Okamura, Tectonophysics 94, 541 (1983)]. As our study focuses on the deep magma system, we did not attempt to model this event.
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(1983)
Tectonophysics
, vol.94
, pp. 541
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Pollard, D.D.1
Delaney, P.T.2
Duffield, W.A.3
Endo, E.T.4
Okamura, A.T.5
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30
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0343802839
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note
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Coulomb stress changes are defined as ΔS = Δτ -μ′Δσ, where Δτ is the shear stress change on a given failure plane (positive in the direction of fault slip), Δσ is the change in effective normal stress (positive in compression), and μ′ is the effective friction coefficient = 0.35.
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31
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0342497644
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P. T. Delaney, A. Miklius, T. Árnadóttir, A. T. Okamura, M. Sako, U.S. Geol. Surv. Open File Rep. 94-567 (1994).
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(1994)
U.S. Geol. Surv. Open File Rep. 94-567
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Delaney, P.T.1
Miklius, A.2
Árnadóttir, T.3
Okamura, A.T.4
Sako, M.5
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32
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0342497647
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note
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We thank the staff of the Hawaiian Volcano Observatory for providing us with the data; P. Okubo and M. Lisowski for useful discussions; P. Okubo for the earthquake summary data; P. Delaney, P. Segall, S. Owen, R. Simpson, and W. Prescott for very useful comments on this manuscript; and P. Segall for the program for computing trilateration station displacements. This research was supported by the U.S. Geological Survey Volcano Hazards Program.
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