{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2BMHHBNQAL5TCGVERX7RITEAMI","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"f8fd468be2b8018dba17a10f256688015ad348fd5081b7d223aa0ed55dfe5647","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-02-28T10:43:16Z","title_canon_sha256":"21bbce014cf788ac15c4cb8192ecdd333fac84c0248f5cce8cffdf84b7bf0958"},"schema_version":"1.0","source":{"id":"1402.7194","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.7194","created_at":"2026-05-18T01:35:40Z"},{"alias_kind":"arxiv_version","alias_value":"1402.7194v2","created_at":"2026-05-18T01:35:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.7194","created_at":"2026-05-18T01:35:40Z"},{"alias_kind":"pith_short_12","alias_value":"2BMHHBNQAL5T","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"2BMHHBNQAL5TCGVE","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"2BMHHBNQ","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:757644e9878434552e22ca56ce271297b346e192681ea3a60921c9512788742b","target":"graph","created_at":"2026-05-18T01:35:40Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Escape rate in the low-to-intermediate damping connecting the low damping with the intermediate damping is established for the power-law distribution on the basis of flux over population theory. We extend the escape rate in the low damping to the low-to-intermediate damping, and get an expression for the power-law distribution. Then we apply the escape rate for the power-law distribution to the experimental study of the excited-state isomerization, and show a good agreement with the experimental value. The extra current and the improvement of the absorbing boundary condition are discussed.","authors_text":"Jiulin Du, Yanjun Zhou","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-02-28T10:43:16Z","title":"Escape rate for the power-law distribution in low-to-intermediate damping"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.7194","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:3b6fb1a100100d23acc8cbf5609bbc17edb894cca88f1dd6893056da21b55d89","target":"record","created_at":"2026-05-18T01:35:40Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"f8fd468be2b8018dba17a10f256688015ad348fd5081b7d223aa0ed55dfe5647","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-02-28T10:43:16Z","title_canon_sha256":"21bbce014cf788ac15c4cb8192ecdd333fac84c0248f5cce8cffdf84b7bf0958"},"schema_version":"1.0","source":{"id":"1402.7194","kind":"arxiv","version":2}},"canonical_sha256":"d0587385b002fb311aa48dff144c80621bf49b4ec05ba97e9ddbbe0e695c7392","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d0587385b002fb311aa48dff144c80621bf49b4ec05ba97e9ddbbe0e695c7392","first_computed_at":"2026-05-18T01:35:40.428652Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:35:40.428652Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"A0QUABqE0iaT+yLTgl7ULOSz42Kjs4ckBKS7YsIT7ZW0aIh6c73dQ6d77aFpvJdkv8X2+hu1nQbuFha5hQNXCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:35:40.429429Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.7194","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3b6fb1a100100d23acc8cbf5609bbc17edb894cca88f1dd6893056da21b55d89","sha256:757644e9878434552e22ca56ce271297b346e192681ea3a60921c9512788742b"],"state_sha256":"baa2ec8cd49056c8c20015617a4770aa98c5b6fedb8ca64cb30af3a85d7199a2"}