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Annual Meeting - SCEC.org

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Poster Abstracts<br />

resolutions. Overall, coarsely parameterized source reduces storage drastically, though a gain in computational time requires<br />

an equivalent coarsening of the data, and the mean slip during the adjoint iterations converges towards the mean slip of the<br />

true source (projected in the coarser mesh) in about 9 iterations.<br />

DEVELOPING A PHYSICS-BASED RUPTURE MODEL GENERATOR BASED ON 1-POINT AND 2-POINT<br />

STATISTICS OF KINEMATIC SOURCE PARAMETERS (B-002)<br />

S. Song<br />

A finite-fault earthquake rupture model generator (SongRMG, Ver 1.0) has been developed, based on 1-point and 2-point<br />

statistics of key kinematic source parameters such as slip, rupture velocity, slip velocity and duration. 1-point statistics define<br />

a marginal probability density function for a certain source parameter at a given point on a fault. 2-point statistics, i.e. autoand<br />

cross-coherence between source parameters, control the heterogeneity of each source parameter and their coupling,<br />

respectively. Sequential Gaussian simulation with simple kriging (SK) was initially adopted to perform stochastic modeling<br />

(Song and Somerville, 2010), but it was replaced with a new algorithm based on the Cholesky factorization because it is<br />

conceptually simpler to implement and also more closely linked to earthquake source inversion in the Bayesian framework,<br />

which is an important tool in constraining the 1-point and 2-point statistics of source parameters from data. Currently the 1point<br />

variability of source parameters follows the Gaussian distribution, but it is straightforward to transform it to any other<br />

non-Gaussian distributions if desired. This transform will break the multi-Gaussian distribution assumed in the stochastic<br />

modeling, but the target covariance matrix (or correlation structure) will be preserved as long as the transformed distribution<br />

has a monotonically and smoothly increasing cumulative density function (CDF). The non-stationarity of the 1-point statistics<br />

can also be easily implemented if necessary, such as depth dependency of the 1-point variability. Following studies will focus<br />

on constraining input parameters in the stochastic model by dynamic rupture modeling, kinematic source inversion, and<br />

laboratory experiments, etc., and understanding their effects on near-fault ground motion characteristics. Additionally since<br />

the rupture model generator constrains a possible range of rupture scenarios for future events and quantify their variability<br />

within the range, it can be used as a basis to develop an extended earthquake rupture forecast model (eERF) for fullwaveform-simulation-based<br />

hazard analysis.<br />

236 | Southern California Earthquake Center

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