{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:LIXMHE7S5WT3FIKJPH3LZF4Y2Q","short_pith_number":"pith:LIXMHE7S","canonical_record":{"source":{"id":"1006.3509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2010-06-17T16:30:44Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"89056815e2be0ad64f4aed014d46d73869bde0ce90fa9b8dc248df1477d6577b","abstract_canon_sha256":"1e98e6c39e8b24389a155fb39b85e8b135b2aabd9030d57bdec2d48886f5c8d5"},"schema_version":"1.0"},"canonical_sha256":"5a2ec393f2eda7b2a14979f6bc9798d429013c6bf162b759b0988c252a4c6826","source":{"kind":"arxiv","id":"1006.3509","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1006.3509","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"arxiv_version","alias_value":"1006.3509v1","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.3509","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"pith_short_12","alias_value":"LIXMHE7S5WT3","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"LIXMHE7S5WT3FIKJ","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"LIXMHE7S","created_at":"2026-05-18T12:26:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:LIXMHE7S5WT3FIKJPH3LZF4Y2Q","target":"record","payload":{"canonical_record":{"source":{"id":"1006.3509","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2010-06-17T16:30:44Z","cross_cats_sorted":["physics.optics","quant-ph"],"title_canon_sha256":"89056815e2be0ad64f4aed014d46d73869bde0ce90fa9b8dc248df1477d6577b","abstract_canon_sha256":"1e98e6c39e8b24389a155fb39b85e8b135b2aabd9030d57bdec2d48886f5c8d5"},"schema_version":"1.0"},"canonical_sha256":"5a2ec393f2eda7b2a14979f6bc9798d429013c6bf162b759b0988c252a4c6826","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:00:28.551711Z","signature_b64":"hPf3fP9CIqKZ9V3Mbkq3zY9ueUNPA26MAe1zzfI4TpACWdZumg9gFZsMx1LhpJaSwxNFcJvX+80MbgwLvbLhAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5a2ec393f2eda7b2a14979f6bc9798d429013c6bf162b759b0988c252a4c6826","last_reissued_at":"2026-05-18T04:00:28.551225Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:00:28.551225Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1006.3509","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":"2026-05-18T04:00:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XlbobrL1nnKAYwGp/+k3576lkA/f5PKnko/CTpYV12NH/nZulWUzfhny2WyNMAMuR5LKjIjDsyI1VNcYA7A6BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:37:46.653933Z"},"content_sha256":"40848dec7c49673013093d88e59046097b7f726be502a3e713221d4aa25d1a32","schema_version":"1.0","event_id":"sha256:40848dec7c49673013093d88e59046097b7f726be502a3e713221d4aa25d1a32"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:LIXMHE7S5WT3FIKJPH3LZF4Y2Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Chaotically spiking attractors in suspended mirror optical cavities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics","quant-ph"],"primary_cat":"nlin.CD","authors_text":"Francesco Marin, Francesco Marino","submitted_at":"2010-06-17T16:30:44Z","abstract_excerpt":"A high-finesse suspended mirror Fabry-Perot cavity is experimentally studied in a regime where radiation pressure and photothermal effect are both relevant. The competition between these phenomena, operating at different time scales, produces unobserved dynamical scenarios where an initial Hopf instability is followed by the birth of small-amplitude chaotic attractors which erratically but deterministically trigger optical spikes. The observed dynamical regimes are well reproduced by a detailed physical model of the system."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.3509","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":"2026-05-18T04:00:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aTYUjR4VVKgtTZ6czLjxFnR581sBCsVtwzOoAuEUSR6mSbryEHleZzGlHvVSkO3xQ7kT85ogFcv2aT5TRSkMBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:37:46.654352Z"},"content_sha256":"c3535747a573fb5230a3d631ad784d66bacf59a863e44b61097d53a1c9610453","schema_version":"1.0","event_id":"sha256:c3535747a573fb5230a3d631ad784d66bacf59a863e44b61097d53a1c9610453"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/bundle.json","state_url":"https://pith.science/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/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":"2026-05-27T05:37:46Z","links":{"resolver":"https://pith.science/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q","bundle":"https://pith.science/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/bundle.json","state":"https://pith.science/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LIXMHE7S5WT3FIKJPH3LZF4Y2Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:LIXMHE7S5WT3FIKJPH3LZF4Y2Q","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":"1e98e6c39e8b24389a155fb39b85e8b135b2aabd9030d57bdec2d48886f5c8d5","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2010-06-17T16:30:44Z","title_canon_sha256":"89056815e2be0ad64f4aed014d46d73869bde0ce90fa9b8dc248df1477d6577b"},"schema_version":"1.0","source":{"id":"1006.3509","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1006.3509","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"arxiv_version","alias_value":"1006.3509v1","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.3509","created_at":"2026-05-18T04:00:28Z"},{"alias_kind":"pith_short_12","alias_value":"LIXMHE7S5WT3","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_16","alias_value":"LIXMHE7S5WT3FIKJ","created_at":"2026-05-18T12:26:10Z"},{"alias_kind":"pith_short_8","alias_value":"LIXMHE7S","created_at":"2026-05-18T12:26:10Z"}],"graph_snapshots":[{"event_id":"sha256:c3535747a573fb5230a3d631ad784d66bacf59a863e44b61097d53a1c9610453","target":"graph","created_at":"2026-05-18T04:00:28Z","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":"A high-finesse suspended mirror Fabry-Perot cavity is experimentally studied in a regime where radiation pressure and photothermal effect are both relevant. The competition between these phenomena, operating at different time scales, produces unobserved dynamical scenarios where an initial Hopf instability is followed by the birth of small-amplitude chaotic attractors which erratically but deterministically trigger optical spikes. The observed dynamical regimes are well reproduced by a detailed physical model of the system.","authors_text":"Francesco Marin, Francesco Marino","cross_cats":["physics.optics","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2010-06-17T16:30:44Z","title":"Chaotically spiking attractors in suspended mirror optical cavities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.3509","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":"sha256:40848dec7c49673013093d88e59046097b7f726be502a3e713221d4aa25d1a32","target":"record","created_at":"2026-05-18T04:00:28Z","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":"1e98e6c39e8b24389a155fb39b85e8b135b2aabd9030d57bdec2d48886f5c8d5","cross_cats_sorted":["physics.optics","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2010-06-17T16:30:44Z","title_canon_sha256":"89056815e2be0ad64f4aed014d46d73869bde0ce90fa9b8dc248df1477d6577b"},"schema_version":"1.0","source":{"id":"1006.3509","kind":"arxiv","version":1}},"canonical_sha256":"5a2ec393f2eda7b2a14979f6bc9798d429013c6bf162b759b0988c252a4c6826","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5a2ec393f2eda7b2a14979f6bc9798d429013c6bf162b759b0988c252a4c6826","first_computed_at":"2026-05-18T04:00:28.551225Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:00:28.551225Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hPf3fP9CIqKZ9V3Mbkq3zY9ueUNPA26MAe1zzfI4TpACWdZumg9gFZsMx1LhpJaSwxNFcJvX+80MbgwLvbLhAw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:00:28.551711Z","signed_message":"canonical_sha256_bytes"},"source_id":"1006.3509","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:40848dec7c49673013093d88e59046097b7f726be502a3e713221d4aa25d1a32","sha256:c3535747a573fb5230a3d631ad784d66bacf59a863e44b61097d53a1c9610453"],"state_sha256":"fd0c1f56dd5ace22a18cacdf874e365082cf743182969f6c9a4a146eca41e679"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UXZhrkwN0kAtKTyqTsqUjpTCYBLv+kCSu1FDHsKjhVY1MRRe8OzKOIPVyxZLpMRnPTiSSuVp9nNSTBONtTBAAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T05:37:46.656855Z","bundle_sha256":"223e7dc3f111926fad161453b84ab47331b3fbde8baa892f7dcaf6cd35486ce1"}}