{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ANAIIUJSSJGGXRK5Y4JMIGAAFA","short_pith_number":"pith:ANAIIUJS","canonical_record":{"source":{"id":"1303.6621","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2013-03-26T19:48:39Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"8f2a6e5cc2160791fecde2f5eaf9197a6e868125f9d7fe4536c320ef32786fe3","abstract_canon_sha256":"a1c87cc6a7f5ac1ed3b2e817fb676752dee0485dcb19ad757794ce91e7486310"},"schema_version":"1.0"},"canonical_sha256":"0340845132924c6bc55dc712c418002824b2f186bfefa3ecfd75825b584cc34a","source":{"kind":"arxiv","id":"1303.6621","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.6621","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"arxiv_version","alias_value":"1303.6621v1","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6621","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"pith_short_12","alias_value":"ANAIIUJSSJGG","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ANAIIUJSSJGGXRK5","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ANAIIUJS","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ANAIIUJSSJGGXRK5Y4JMIGAAFA","target":"record","payload":{"canonical_record":{"source":{"id":"1303.6621","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2013-03-26T19:48:39Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"8f2a6e5cc2160791fecde2f5eaf9197a6e868125f9d7fe4536c320ef32786fe3","abstract_canon_sha256":"a1c87cc6a7f5ac1ed3b2e817fb676752dee0485dcb19ad757794ce91e7486310"},"schema_version":"1.0"},"canonical_sha256":"0340845132924c6bc55dc712c418002824b2f186bfefa3ecfd75825b584cc34a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:48.857143Z","signature_b64":"yH+7o2DAsS+G6AXnq3KA2LIQqrYOYGYj9hiuxbwLlrLijznDa9tuxtuQkFrAQRYViY+riWBp6saKHzrgWy7tCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0340845132924c6bc55dc712c418002824b2f186bfefa3ecfd75825b584cc34a","last_reissued_at":"2026-05-18T03:29:48.856596Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:48.856596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.6621","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":"2026-05-18T03:29:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"729Tc9DyJfG59dMlFxPxMzSbHcr1+xdHDluPR9LYS35CXmO6hFoBBmxT8yyZBfEyy3H4PDcj5gy27z+iyfAgAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:20:28.367137Z"},"content_sha256":"4954aa47b5bd28617301c990a3dcae9cf82ba3b247e1ed3afd94cd548dfe7c9f","schema_version":"1.0","event_id":"sha256:4954aa47b5bd28617301c990a3dcae9cf82ba3b247e1ed3afd94cd548dfe7c9f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ANAIIUJSSJGGXRK5Y4JMIGAAFA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A unified model for the dynamics of driven ribbon with strain and magnetic order parameters","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"nlin.CD","authors_text":"G. Ananthakrishna, Ritupan Sarmah","submitted_at":"2013-03-26T19:48:39Z","abstract_excerpt":"We develop a unified model to explain the dynamics of driven one dimensional ribbon for materials with strain and magnetic order parameters. We show that the model equations in their most general form explain several results on driven magnetostrictive metallic glass ribbons such as the period doubling route to chaos as a function of a dc magnetic field in the presence of a sinusoidal field, the quasiperiodic route to chaos as a function of the sinusoidal field for a fixed dc field, and induced and suppressed chaos in the presence of an additional low amplitude near resonant sinusoidal field. W"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6621","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":"2026-05-18T03:29:48Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eERMrrifa916uh7U234VtnFTtOVtlFQnVkF3sx/EwwHFFsAYcz/uFcaUxKRG7OCtWiaerDCkwYVuTcU9mHihDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T06:20:28.367493Z"},"content_sha256":"5bc25ec9c764ad75aae5c7824a8d15c2b57f2c748872e4ace4af321ee10674f1","schema_version":"1.0","event_id":"sha256:5bc25ec9c764ad75aae5c7824a8d15c2b57f2c748872e4ace4af321ee10674f1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/bundle.json","state_url":"https://pith.science/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/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":"2026-06-01T06:20:28Z","links":{"resolver":"https://pith.science/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA","bundle":"https://pith.science/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/bundle.json","state":"https://pith.science/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ANAIIUJSSJGGXRK5Y4JMIGAAFA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ANAIIUJSSJGGXRK5Y4JMIGAAFA","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":"a1c87cc6a7f5ac1ed3b2e817fb676752dee0485dcb19ad757794ce91e7486310","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2013-03-26T19:48:39Z","title_canon_sha256":"8f2a6e5cc2160791fecde2f5eaf9197a6e868125f9d7fe4536c320ef32786fe3"},"schema_version":"1.0","source":{"id":"1303.6621","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.6621","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"arxiv_version","alias_value":"1303.6621v1","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6621","created_at":"2026-05-18T03:29:48Z"},{"alias_kind":"pith_short_12","alias_value":"ANAIIUJSSJGG","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"ANAIIUJSSJGGXRK5","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"ANAIIUJS","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:5bc25ec9c764ad75aae5c7824a8d15c2b57f2c748872e4ace4af321ee10674f1","target":"graph","created_at":"2026-05-18T03:29:48Z","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":"We develop a unified model to explain the dynamics of driven one dimensional ribbon for materials with strain and magnetic order parameters. We show that the model equations in their most general form explain several results on driven magnetostrictive metallic glass ribbons such as the period doubling route to chaos as a function of a dc magnetic field in the presence of a sinusoidal field, the quasiperiodic route to chaos as a function of the sinusoidal field for a fixed dc field, and induced and suppressed chaos in the presence of an additional low amplitude near resonant sinusoidal field. W","authors_text":"G. Ananthakrishna, Ritupan Sarmah","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2013-03-26T19:48:39Z","title":"A unified model for the dynamics of driven ribbon with strain and magnetic order parameters"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6621","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":"sha256:4954aa47b5bd28617301c990a3dcae9cf82ba3b247e1ed3afd94cd548dfe7c9f","target":"record","created_at":"2026-05-18T03:29:48Z","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":"a1c87cc6a7f5ac1ed3b2e817fb676752dee0485dcb19ad757794ce91e7486310","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.CD","submitted_at":"2013-03-26T19:48:39Z","title_canon_sha256":"8f2a6e5cc2160791fecde2f5eaf9197a6e868125f9d7fe4536c320ef32786fe3"},"schema_version":"1.0","source":{"id":"1303.6621","kind":"arxiv","version":1}},"canonical_sha256":"0340845132924c6bc55dc712c418002824b2f186bfefa3ecfd75825b584cc34a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0340845132924c6bc55dc712c418002824b2f186bfefa3ecfd75825b584cc34a","first_computed_at":"2026-05-18T03:29:48.856596Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:29:48.856596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yH+7o2DAsS+G6AXnq3KA2LIQqrYOYGYj9hiuxbwLlrLijznDa9tuxtuQkFrAQRYViY+riWBp6saKHzrgWy7tCA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:29:48.857143Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.6621","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4954aa47b5bd28617301c990a3dcae9cf82ba3b247e1ed3afd94cd548dfe7c9f","sha256:5bc25ec9c764ad75aae5c7824a8d15c2b57f2c748872e4ace4af321ee10674f1"],"state_sha256":"235a26c49cb102adb6b04b7448819b1d92b39da00fd9c2be1b9803ae8748fb96"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cDSqcRWeOCDdU/QEcZq8pRVVR34peRwjKUAd9SfhtoC3Mz2CChrR3fz6jhkhdwBQGTajhZ4bKNjpscAJ8HnDBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T06:20:28.369448Z","bundle_sha256":"d7df73317561b56ccbe6bcf7b1f0f1548a4c04934d3f10832d553a6dc2d79f1e"}}