{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:ARRYV2J6GF4UHZZIWXEZRIJHYU","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":"8d4e9042125addc26090ec4782b8d098228d98b39a26dd311e178b5f31cfc5a3","cross_cats_sorted":["math.DS","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-04-23T14:07:33Z","title_canon_sha256":"23a1919577a7db238e5cb891dcf417e0c4de0ac4f9a5a7c59c32b54660934f39"},"schema_version":"1.0","source":{"id":"1704.06924","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.06924","created_at":"2026-05-18T00:34:15Z"},{"alias_kind":"arxiv_version","alias_value":"1704.06924v2","created_at":"2026-05-18T00:34:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.06924","created_at":"2026-05-18T00:34:15Z"},{"alias_kind":"pith_short_12","alias_value":"ARRYV2J6GF4U","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_16","alias_value":"ARRYV2J6GF4UHZZI","created_at":"2026-05-18T12:31:08Z"},{"alias_kind":"pith_short_8","alias_value":"ARRYV2J6","created_at":"2026-05-18T12:31:08Z"}],"graph_snapshots":[{"event_id":"sha256:ee2c94d13b36f8335b1bf0f8bc5d80c2a20d2b9e89907d068d8410dee218590e","target":"graph","created_at":"2026-05-18T00:34:15Z","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":"The paper considers a process of escape of classical particle from a one-dimensional potential well by virtue of an external harmonic forcing. We address a particular model of the infinite-range potential well that allows independent adjustment of the well depth and of the frequency of small oscillations. The problem can be conveniently reformulated in terms of action-angle variables. Further averaging provides a nontrivial conservation law for the slow flow. Thus, one can consider the problem in terms of averaged dynamics on primary 1:1 resonance manifold. This simplification allows efficient","authors_text":"O.V.Gendelman","cross_cats":["math.DS","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-04-23T14:07:33Z","title":"Escape of harmonically forced classical particle from an infinite-range potential well"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.06924","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":"sha256:4cb5080ace4f7f9133e97442c257997fe91ceca1cbe426529eb286f8ebfe67c1","target":"record","created_at":"2026-05-18T00:34:15Z","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":"8d4e9042125addc26090ec4782b8d098228d98b39a26dd311e178b5f31cfc5a3","cross_cats_sorted":["math.DS","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2017-04-23T14:07:33Z","title_canon_sha256":"23a1919577a7db238e5cb891dcf417e0c4de0ac4f9a5a7c59c32b54660934f39"},"schema_version":"1.0","source":{"id":"1704.06924","kind":"arxiv","version":2}},"canonical_sha256":"04638ae93e317943e728b5c998a127c530ba8f9efbfa424b38129c711560f354","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"04638ae93e317943e728b5c998a127c530ba8f9efbfa424b38129c711560f354","first_computed_at":"2026-05-18T00:34:15.254515Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:34:15.254515Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"afou6rFn9lVuLbaqgLpoeeVYp8U3k2m6vdvJRv15oW9m+yATmeuqaH46WIdIG+N8I46IdE6BWs4owGphuNFhCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:34:15.255219Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.06924","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4cb5080ace4f7f9133e97442c257997fe91ceca1cbe426529eb286f8ebfe67c1","sha256:ee2c94d13b36f8335b1bf0f8bc5d80c2a20d2b9e89907d068d8410dee218590e"],"state_sha256":"16105ccc04b55b208e160559af5edb1fd8df883890691ca6215d3f2b7bf48637"}