{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2008:KAVZHTU4RTGBXSRFPKMK65U7JC","short_pith_number":"pith:KAVZHTU4","canonical_record":{"source":{"id":"0801.3020","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.class-ph","submitted_at":"2008-01-19T07:50:44Z","cross_cats_sorted":["math.DS"],"title_canon_sha256":"016878f0fa025c76484267b8734d937cd9b4ed8fbe2e5178240dbc638af4d063","abstract_canon_sha256":"2103e45aa1458bc12143df799559f21886ac571fc8dfb2a705f9ce9c40df6bd0"},"schema_version":"1.0"},"canonical_sha256":"502b93ce9c8ccc1bca257a98af769f48b1cc2bf1802bde578f999789b0bacb6d","source":{"kind":"arxiv","id":"0801.3020","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0801.3020","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"arxiv_version","alias_value":"0801.3020v1","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0801.3020","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"pith_short_12","alias_value":"KAVZHTU4RTGB","created_at":"2026-05-18T12:25:57Z"},{"alias_kind":"pith_short_16","alias_value":"KAVZHTU4RTGBXSRF","created_at":"2026-05-18T12:25:57Z"},{"alias_kind":"pith_short_8","alias_value":"KAVZHTU4","created_at":"2026-05-18T12:25:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2008:KAVZHTU4RTGBXSRFPKMK65U7JC","target":"record","payload":{"canonical_record":{"source":{"id":"0801.3020","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.class-ph","submitted_at":"2008-01-19T07:50:44Z","cross_cats_sorted":["math.DS"],"title_canon_sha256":"016878f0fa025c76484267b8734d937cd9b4ed8fbe2e5178240dbc638af4d063","abstract_canon_sha256":"2103e45aa1458bc12143df799559f21886ac571fc8dfb2a705f9ce9c40df6bd0"},"schema_version":"1.0"},"canonical_sha256":"502b93ce9c8ccc1bca257a98af769f48b1cc2bf1802bde578f999789b0bacb6d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:36.716113Z","signature_b64":"37EAAsWIemHIuB13355jq4cDw9ymzx//R3uL4N1hj6GpAFnpO36EQrePe392zAdjaiu0GsSzViJ7Ai6Dfut2Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"502b93ce9c8ccc1bca257a98af769f48b1cc2bf1802bde578f999789b0bacb6d","last_reissued_at":"2026-05-18T03:44:36.715348Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:36.715348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0801.3020","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:44:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xohYKUnKYKoOeWxHbvYREYkpNtxGp6h+CAvclRTdvdBf7tUep6aWtJUS6B92bVUUKgi/I4l+rRViCHBJhKQrDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T12:59:45.283021Z"},"content_sha256":"2cf154322f70360dbd0d2af6329c88d5d20b3f7ba3dc663a9dc7e9dec27be1f2","schema_version":"1.0","event_id":"sha256:2cf154322f70360dbd0d2af6329c88d5d20b3f7ba3dc663a9dc7e9dec27be1f2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2008:KAVZHTU4RTGBXSRFPKMK65U7JC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The invariant manifold approach applied to nonlinear dynamics of a rotor-bearing system","license":"","headline":"","cross_cats":["math.DS"],"primary_cat":"physics.class-ph","authors_text":"Cristiano Villa (LTDS), Fabrice Thouverez (LTDS), Jean-Jacques Sinou (LTDS)","submitted_at":"2008-01-19T07:50:44Z","abstract_excerpt":"The invariant manifold approach is used to explore the dynamics of a nonlinear rotor, by determining the nonlinear normal modes, constructing a reduced order model and evaluating its performance in the case of response to an initial condition. The procedure to determine the approximation of the invariant manifolds is discussed and a strategy to retain the speed dependent effects on the manifolds without solving the eigenvalue problem for each spin speed is presented. The performance of the reduced system is analysed in function of the spin speed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0801.3020","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:44:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"e9vWkffeNcmFC0ze2z25suXGyrhPt7SRsDQ8+z3XL2VuA8Us+7QgvoPgzw/c/OrjWzkh5CmqCS+7nmNoht7bDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T12:59:45.283377Z"},"content_sha256":"b0801a5efa7cd9c75d4e59caad0ad24d583757c1285a4bfd26b051f61e9d6257","schema_version":"1.0","event_id":"sha256:b0801a5efa7cd9c75d4e59caad0ad24d583757c1285a4bfd26b051f61e9d6257"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/bundle.json","state_url":"https://pith.science/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-22T12:59:45Z","links":{"resolver":"https://pith.science/pith/KAVZHTU4RTGBXSRFPKMK65U7JC","bundle":"https://pith.science/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/bundle.json","state":"https://pith.science/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KAVZHTU4RTGBXSRFPKMK65U7JC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2008:KAVZHTU4RTGBXSRFPKMK65U7JC","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":"2103e45aa1458bc12143df799559f21886ac571fc8dfb2a705f9ce9c40df6bd0","cross_cats_sorted":["math.DS"],"license":"","primary_cat":"physics.class-ph","submitted_at":"2008-01-19T07:50:44Z","title_canon_sha256":"016878f0fa025c76484267b8734d937cd9b4ed8fbe2e5178240dbc638af4d063"},"schema_version":"1.0","source":{"id":"0801.3020","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0801.3020","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"arxiv_version","alias_value":"0801.3020v1","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0801.3020","created_at":"2026-05-18T03:44:36Z"},{"alias_kind":"pith_short_12","alias_value":"KAVZHTU4RTGB","created_at":"2026-05-18T12:25:57Z"},{"alias_kind":"pith_short_16","alias_value":"KAVZHTU4RTGBXSRF","created_at":"2026-05-18T12:25:57Z"},{"alias_kind":"pith_short_8","alias_value":"KAVZHTU4","created_at":"2026-05-18T12:25:57Z"}],"graph_snapshots":[{"event_id":"sha256:b0801a5efa7cd9c75d4e59caad0ad24d583757c1285a4bfd26b051f61e9d6257","target":"graph","created_at":"2026-05-18T03:44:36Z","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 invariant manifold approach is used to explore the dynamics of a nonlinear rotor, by determining the nonlinear normal modes, constructing a reduced order model and evaluating its performance in the case of response to an initial condition. The procedure to determine the approximation of the invariant manifolds is discussed and a strategy to retain the speed dependent effects on the manifolds without solving the eigenvalue problem for each spin speed is presented. The performance of the reduced system is analysed in function of the spin speed.","authors_text":"Cristiano Villa (LTDS), Fabrice Thouverez (LTDS), Jean-Jacques Sinou (LTDS)","cross_cats":["math.DS"],"headline":"","license":"","primary_cat":"physics.class-ph","submitted_at":"2008-01-19T07:50:44Z","title":"The invariant manifold approach applied to nonlinear dynamics of a rotor-bearing system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0801.3020","kind":"arxiv","version":1},"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":"sha256:2cf154322f70360dbd0d2af6329c88d5d20b3f7ba3dc663a9dc7e9dec27be1f2","target":"record","created_at":"2026-05-18T03:44:36Z","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":"2103e45aa1458bc12143df799559f21886ac571fc8dfb2a705f9ce9c40df6bd0","cross_cats_sorted":["math.DS"],"license":"","primary_cat":"physics.class-ph","submitted_at":"2008-01-19T07:50:44Z","title_canon_sha256":"016878f0fa025c76484267b8734d937cd9b4ed8fbe2e5178240dbc638af4d063"},"schema_version":"1.0","source":{"id":"0801.3020","kind":"arxiv","version":1}},"canonical_sha256":"502b93ce9c8ccc1bca257a98af769f48b1cc2bf1802bde578f999789b0bacb6d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"502b93ce9c8ccc1bca257a98af769f48b1cc2bf1802bde578f999789b0bacb6d","first_computed_at":"2026-05-18T03:44:36.715348Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:44:36.715348Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"37EAAsWIemHIuB13355jq4cDw9ymzx//R3uL4N1hj6GpAFnpO36EQrePe392zAdjaiu0GsSzViJ7Ai6Dfut2Cg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:44:36.716113Z","signed_message":"canonical_sha256_bytes"},"source_id":"0801.3020","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2cf154322f70360dbd0d2af6329c88d5d20b3f7ba3dc663a9dc7e9dec27be1f2","sha256:b0801a5efa7cd9c75d4e59caad0ad24d583757c1285a4bfd26b051f61e9d6257"],"state_sha256":"a03a3c2ad3fb04d3ef9728c67ab5c39f8ae682875d045548f906efc54896d5d3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cvYbsv67F3Vcv+GB6ofzeu6ZmQaDyj3QYWwfnfMmEgP1id7JszvxA+0cSjvsU8KIl1D3E95jjzodwK3oVtWvCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T12:59:45.285264Z","bundle_sha256":"1d877de0350ef4e2ad7bacc73ee786921d1f58001d540c3569a93fef292fe7e3"}}