{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:SODJJP67HXZWIMDYCTVWAUQW6J","short_pith_number":"pith:SODJJP67","schema_version":"1.0","canonical_sha256":"938694bfdf3df364307814eb605216f26bfda1628adf5588fad90f86d1e153fe","source":{"kind":"arxiv","id":"1202.2553","version":1},"attestation_state":"computed","paper":{"title":"Evolution of burst distribution in fiber bundle model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"A. A. Snarskii, I. V. Bezsudnov","submitted_at":"2012-02-12T18:38:31Z","abstract_excerpt":"We consider a fiber bundle model with a equal load sharing and uniformly distributed breakdown thresholds. A unified probability-theoretic approach was used to describe bundle under continuous and discrete load increase. It was shown that the ratio of distribution D(d) of avalanches of sizes d to the number of bundle load steps exactly corresponds to burst probability of size d. Evolution of s - power law distribution exponent of D(d) was studied as a function of loading step and bundle size. It was shown that s does not depend on bundle size. In the numerical experiment, dependence s on loadi"},"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":"1202.2553","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-02-12T18:38:31Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"d2aeadd0aba41a163292a2bbf37cebaec34495b646957f419d7b3421f8686354","abstract_canon_sha256":"0a99e626645c26c405bdec61517c7328c36fc37ce5be5590a3c9e7b7082ceacc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:02:26.219523Z","signature_b64":"zkCl6qIg3kPf7Au03TgZPfo3gi8XQPrUKpl8UiQ3/mlw/t7m4HcnJvjs8goP4IF3c/6pSmDPoKKEURiWu24BDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"938694bfdf3df364307814eb605216f26bfda1628adf5588fad90f86d1e153fe","last_reissued_at":"2026-05-18T04:02:26.218911Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:02:26.218911Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evolution of burst distribution in fiber bundle model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"A. A. Snarskii, I. V. Bezsudnov","submitted_at":"2012-02-12T18:38:31Z","abstract_excerpt":"We consider a fiber bundle model with a equal load sharing and uniformly distributed breakdown thresholds. A unified probability-theoretic approach was used to describe bundle under continuous and discrete load increase. It was shown that the ratio of distribution D(d) of avalanches of sizes d to the number of bundle load steps exactly corresponds to burst probability of size d. Evolution of s - power law distribution exponent of D(d) was studied as a function of loading step and bundle size. It was shown that s does not depend on bundle size. In the numerical experiment, dependence s on loadi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.2553","kind":"arxiv","version":1},"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":"1202.2553","created_at":"2026-05-18T04:02:26.219000+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.2553v1","created_at":"2026-05-18T04:02:26.219000+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.2553","created_at":"2026-05-18T04:02:26.219000+00:00"},{"alias_kind":"pith_short_12","alias_value":"SODJJP67HXZW","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_16","alias_value":"SODJJP67HXZWIMDY","created_at":"2026-05-18T12:27:20.899486+00:00"},{"alias_kind":"pith_short_8","alias_value":"SODJJP67","created_at":"2026-05-18T12:27:20.899486+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/SODJJP67HXZWIMDYCTVWAUQW6J","json":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J.json","graph_json":"https://pith.science/api/pith-number/SODJJP67HXZWIMDYCTVWAUQW6J/graph.json","events_json":"https://pith.science/api/pith-number/SODJJP67HXZWIMDYCTVWAUQW6J/events.json","paper":"https://pith.science/paper/SODJJP67"},"agent_actions":{"view_html":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J","download_json":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J.json","view_paper":"https://pith.science/paper/SODJJP67","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.2553&json=true","fetch_graph":"https://pith.science/api/pith-number/SODJJP67HXZWIMDYCTVWAUQW6J/graph.json","fetch_events":"https://pith.science/api/pith-number/SODJJP67HXZWIMDYCTVWAUQW6J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J/action/storage_attestation","attest_author":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J/action/author_attestation","sign_citation":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J/action/citation_signature","submit_replication":"https://pith.science/pith/SODJJP67HXZWIMDYCTVWAUQW6J/action/replication_record"}},"created_at":"2026-05-18T04:02:26.219000+00:00","updated_at":"2026-05-18T04:02:26.219000+00:00"}