{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:HH3XSQF45M52QBCGJDOJH2HCTA","short_pith_number":"pith:HH3XSQF4","schema_version":"1.0","canonical_sha256":"39f77940bceb3ba8044648dc93e8e29822c649446a6d6e55d42a1d4613eacd0c","source":{"kind":"arxiv","id":"1707.04119","version":2},"attestation_state":"computed","paper":{"title":"Critical nucleation length for accelerating frictional slip","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.geo-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Efim A. Brener, Eran Bouchbinder, Marc Weikamp, Michael Aldam, Robert Spatschek","submitted_at":"2017-07-13T13:45:51Z","abstract_excerpt":"The spontaneous nucleation of accelerating slip along slowly driven frictional interfaces is central to a broad range of geophysical, physical and engineering systems, with particularly far-reaching implications for earthquake physics. A common approach to this problem associates nucleation with an instability of an expanding creep patch upon surpassing a critical length $L_c$. The critical nucleation length $L_c$ is conventionally obtained from a spring-block linear stability analysis extended to interfaces separating elastically-deformable bodies using model-dependent fracture mechanics esti"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1707.04119","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-07-13T13:45:51Z","cross_cats_sorted":["cond-mat.soft","physics.geo-ph"],"title_canon_sha256":"70f8fe5d1bbcc03444fd36fc434e1e8e4f4a6cf7d995e434775d2b0254261296","abstract_canon_sha256":"2a393350b2d16be6fb1b72e69365c6926ae9a08b01fa0764cb91babea054b311"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:10:24.421055Z","signature_b64":"NoF0gLRfHX22fnBB3NrtP5edaNasHF/67i7E/S3JT5v2XylgUfQsHDOLon4c/52QKl1S9Jv6xRoOF4c3WHavAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39f77940bceb3ba8044648dc93e8e29822c649446a6d6e55d42a1d4613eacd0c","last_reissued_at":"2026-05-18T00:10:24.420480Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:10:24.420480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Critical nucleation length for accelerating frictional slip","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft","physics.geo-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Efim A. Brener, Eran Bouchbinder, Marc Weikamp, Michael Aldam, Robert Spatschek","submitted_at":"2017-07-13T13:45:51Z","abstract_excerpt":"The spontaneous nucleation of accelerating slip along slowly driven frictional interfaces is central to a broad range of geophysical, physical and engineering systems, with particularly far-reaching implications for earthquake physics. A common approach to this problem associates nucleation with an instability of an expanding creep patch upon surpassing a critical length $L_c$. The critical nucleation length $L_c$ is conventionally obtained from a spring-block linear stability analysis extended to interfaces separating elastically-deformable bodies using model-dependent fracture mechanics esti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.04119","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1707.04119","created_at":"2026-05-18T00:10:24.420565+00:00"},{"alias_kind":"arxiv_version","alias_value":"1707.04119v2","created_at":"2026-05-18T00:10:24.420565+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1707.04119","created_at":"2026-05-18T00:10:24.420565+00:00"},{"alias_kind":"pith_short_12","alias_value":"HH3XSQF45M52","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_16","alias_value":"HH3XSQF45M52QBCG","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_8","alias_value":"HH3XSQF4","created_at":"2026-05-18T12:31:18.294218+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA","json":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA.json","graph_json":"https://pith.science/api/pith-number/HH3XSQF45M52QBCGJDOJH2HCTA/graph.json","events_json":"https://pith.science/api/pith-number/HH3XSQF45M52QBCGJDOJH2HCTA/events.json","paper":"https://pith.science/paper/HH3XSQF4"},"agent_actions":{"view_html":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA","download_json":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA.json","view_paper":"https://pith.science/paper/HH3XSQF4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1707.04119&json=true","fetch_graph":"https://pith.science/api/pith-number/HH3XSQF45M52QBCGJDOJH2HCTA/graph.json","fetch_events":"https://pith.science/api/pith-number/HH3XSQF45M52QBCGJDOJH2HCTA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA/action/storage_attestation","attest_author":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA/action/author_attestation","sign_citation":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA/action/citation_signature","submit_replication":"https://pith.science/pith/HH3XSQF45M52QBCGJDOJH2HCTA/action/replication_record"}},"created_at":"2026-05-18T00:10:24.420565+00:00","updated_at":"2026-05-18T00:10:24.420565+00:00"}