日本地球惑星科学連合2014年大会

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セッション記号 S (固体地球科学) » S-SS 地震学

[S-SS29_28PM1] 地震発生の物理・震源過程

2014年4月28日(月) 14:15 〜 16:00 416 (4F)

コンビーナ:*加瀬 祐子(産業技術総合研究所 活断層・地震研究センター)、座長:内出 崇彦(産業技術総合研究所 活断層・地震研究センター)、加藤 愛太郎(東京大学地震研究所)

15:45 〜 16:00

[SSS29-07] 震源過程とVere-Jonesの分枝モデル間の類似特性

庄 建倉1、*王 ?2 (1.統計数理研究所、2.東京大学地震研究所)

キーワード:分枝過程, グーテンベルグ・リヒター則, テーパーパレート分布, `震源過程

Vere-Jones' branching crack model was develop in 1970s. In this model, the earthquake source is regarded as the results of the total population of crack elements in a critical or near-critical branching process, where the crack does not propagate in a single continuous movement, but through a series of steps. At each step, each crack element simply terminates or generates several other crack elements nearby. Regarding the total number of steps (generation) as the duration time and the total number of crack elements as the total energy released, the following similarities are found between earthquake sources and this model:1. The distribution of energies is asymptotically a Pareto distribution (power law) for the critical case, or a tapered Pareto distribution (tapered power law, Kagan distribution) for the subcritical case. 2. The duration time of ruptures has a tapered inverse power distribution. 3. The number of crack elements at each generation (time step) show similar patterns of earthquake source time functions.Figure 1 (a) and (b): Plots of the numbers of crack elements at each time step in two simulation examples. (c): Distribution of half duration times in real earthquake catalog. (d): Distribution of duration times in synthetic catalogs.