{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:PG2DAJHVE2F4LKMM4OG4VNSFPR","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":"c1bf7302f71fb34b5b415272bc511409286c793869bcb06d0bb1021d9b00d6ab","cross_cats_sorted":["math-ph","math.MP","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T13:52:45Z","title_canon_sha256":"f6af7c9364c91ab3d3067a19f47692367c7d2925d47dd3021ced09a2c5d926b5"},"schema_version":"1.0","source":{"id":"2204.06391","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.06391","created_at":"2026-07-05T04:59:21Z"},{"alias_kind":"arxiv_version","alias_value":"2204.06391v3","created_at":"2026-07-05T04:59:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.06391","created_at":"2026-07-05T04:59:21Z"},{"alias_kind":"pith_short_12","alias_value":"PG2DAJHVE2F4","created_at":"2026-07-05T04:59:21Z"},{"alias_kind":"pith_short_16","alias_value":"PG2DAJHVE2F4LKMM","created_at":"2026-07-05T04:59:21Z"},{"alias_kind":"pith_short_8","alias_value":"PG2DAJHV","created_at":"2026-07-05T04:59:21Z"}],"graph_snapshots":[{"event_id":"sha256:e53b9030d5cd493cb756dba456974686e091d5d9105b16e3588608d40bbff23c","target":"graph","created_at":"2026-07-05T04:59:21Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2204.06391/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Chaotic scattering is a manifestation of transient chaos realized by the scattering with non-integrable potential. When the initial position is taken in the potential, a particle initially exhibits chaotic motion, but escapes outside after a certain period of time. The time to stay inside the potential can be seen as lifetime and this escape process may be regarded as a kind of instability. The process of this type exists in the Banks-Fischler-Shenker-Susskind (BFSS) matrix model in which the potential has flat directions. We discuss this chaotic instability by reducing the system with an ansa","authors_text":"Kentaroh Yoshida, Osamu Fukushima","cross_cats":["math-ph","math.MP","nlin.CD"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T13:52:45Z","title":"Chaotic instability in the BFSS matrix model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.06391","kind":"arxiv","version":3},"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":"sha256:7318d4252ef61fbd4cb2eb41385ef3f14643bf59ee219f654f2b83b53a7e552f","target":"record","created_at":"2026-07-05T04:59:21Z","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":"c1bf7302f71fb34b5b415272bc511409286c793869bcb06d0bb1021d9b00d6ab","cross_cats_sorted":["math-ph","math.MP","nlin.CD"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-04-13T13:52:45Z","title_canon_sha256":"f6af7c9364c91ab3d3067a19f47692367c7d2925d47dd3021ced09a2c5d926b5"},"schema_version":"1.0","source":{"id":"2204.06391","kind":"arxiv","version":3}},"canonical_sha256":"79b43024f5268bc5a98ce38dcab6457c5e2a390b41c32e43890b8ef5601852db","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"79b43024f5268bc5a98ce38dcab6457c5e2a390b41c32e43890b8ef5601852db","first_computed_at":"2026-07-05T04:59:21.543657Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:59:21.543657Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"re3JWhkANxiB1RzyEbU07Px3Sz/wGYDCDS0BmgGWBElDsNCUGi9NiTrjc4wtkwdz2m6kj05Q0IJvsBxxz0yfCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:59:21.544080Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.06391","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7318d4252ef61fbd4cb2eb41385ef3f14643bf59ee219f654f2b83b53a7e552f","sha256:e53b9030d5cd493cb756dba456974686e091d5d9105b16e3588608d40bbff23c"],"state_sha256":"b92d658e3610d9b2cf6e390ef583a1d0b4106bc84e54bf860d640fca0bd515cd"}