{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:TU3HAZAFNDENGHAFMI4MU2FW5L","short_pith_number":"pith:TU3HAZAF","canonical_record":{"source":{"id":"1802.05389","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2018-02-15T02:26:40Z","cross_cats_sorted":["nlin.AO"],"title_canon_sha256":"75acc81edb3a8997b94940f10832855eb888e0d28e4f4bcc0ff8ff5f2877c62e","abstract_canon_sha256":"905a5370d19175c5ad59802027a1f90620ff7db673243f6a5571b237ae6fb07e"},"schema_version":"1.0"},"canonical_sha256":"9d3670640568c8d31c056238ca68b6eae001179eaf1e75a778f0212c9432a9ae","source":{"kind":"arxiv","id":"1802.05389","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.05389","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"arxiv_version","alias_value":"1802.05389v3","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.05389","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"pith_short_12","alias_value":"TU3HAZAFNDEN","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"TU3HAZAFNDENGHAF","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"TU3HAZAF","created_at":"2026-05-18T12:32:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:TU3HAZAFNDENGHAFMI4MU2FW5L","target":"record","payload":{"canonical_record":{"source":{"id":"1802.05389","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2018-02-15T02:26:40Z","cross_cats_sorted":["nlin.AO"],"title_canon_sha256":"75acc81edb3a8997b94940f10832855eb888e0d28e4f4bcc0ff8ff5f2877c62e","abstract_canon_sha256":"905a5370d19175c5ad59802027a1f90620ff7db673243f6a5571b237ae6fb07e"},"schema_version":"1.0"},"canonical_sha256":"9d3670640568c8d31c056238ca68b6eae001179eaf1e75a778f0212c9432a9ae","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:17:32.785768Z","signature_b64":"yJ3HGbo8Z3JkVDeHWzOufxf0SbMCJuoi6uKxNMMf3ea2dWbF26MAFEfRMJm9po8ZjwpG2MUnq9C6l3X7UMRkBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d3670640568c8d31c056238ca68b6eae001179eaf1e75a778f0212c9432a9ae","last_reissued_at":"2026-05-18T00:17:32.785117Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:17:32.785117Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1802.05389","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:17:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XRTmjdVMqGQQl4B2rTmiZS8UqtKjMBToTf53DCyCJotprw493hMaX6+WH4MVXwtss080HML+/9l4ZVINt2FrDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T02:33:33.181272Z"},"content_sha256":"cb41b43bfb8f213c4da28eab8fbe63071824290a135228076ee8522e4fe85313","schema_version":"1.0","event_id":"sha256:cb41b43bfb8f213c4da28eab8fbe63071824290a135228076ee8522e4fe85313"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:TU3HAZAFNDENGHAFMI4MU2FW5L","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Galam model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO"],"primary_cat":"physics.soc-ph","authors_text":"Serge Galam, Taksu Cheon","submitted_at":"2018-02-15T02:26:40Z","abstract_excerpt":"We introduce a model of temporal evolution of political opinions which amounts to a dynamical extension of Galam model in which the proportions of inflexibles are treated as dynamical variables. We find that the critical value of inflexibles in the original Galam model now turns into a fixed point of the system whose stability controls the phase trajectory of the political opinions. The appearance of two phases, in which majority-preserving and regime-changing limit cycles are respectively dominant, is found, and also the transition between them is observed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.05389","kind":"arxiv","version":3},"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":"2026-05-18T00:17:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D5YKiLf7sswfJtvaD7Kml5OiGY06O7QPwCeBx8W95HqvMBnypiSAjiAjWsfSBMCskfCw3mtGwboHLg2jk3RlAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T02:33:33.182014Z"},"content_sha256":"3ae41c8a9ffe0a381da0e0cf38666e0a96322cf24ef5d60b41021060c612f58f","schema_version":"1.0","event_id":"sha256:3ae41c8a9ffe0a381da0e0cf38666e0a96322cf24ef5d60b41021060c612f58f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/bundle.json","state_url":"https://pith.science/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/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":"2026-05-20T02:33:33Z","links":{"resolver":"https://pith.science/pith/TU3HAZAFNDENGHAFMI4MU2FW5L","bundle":"https://pith.science/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/bundle.json","state":"https://pith.science/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TU3HAZAFNDENGHAFMI4MU2FW5L/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:TU3HAZAFNDENGHAFMI4MU2FW5L","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":"905a5370d19175c5ad59802027a1f90620ff7db673243f6a5571b237ae6fb07e","cross_cats_sorted":["nlin.AO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2018-02-15T02:26:40Z","title_canon_sha256":"75acc81edb3a8997b94940f10832855eb888e0d28e4f4bcc0ff8ff5f2877c62e"},"schema_version":"1.0","source":{"id":"1802.05389","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.05389","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"arxiv_version","alias_value":"1802.05389v3","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.05389","created_at":"2026-05-18T00:17:32Z"},{"alias_kind":"pith_short_12","alias_value":"TU3HAZAFNDEN","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_16","alias_value":"TU3HAZAFNDENGHAF","created_at":"2026-05-18T12:32:56Z"},{"alias_kind":"pith_short_8","alias_value":"TU3HAZAF","created_at":"2026-05-18T12:32:56Z"}],"graph_snapshots":[{"event_id":"sha256:3ae41c8a9ffe0a381da0e0cf38666e0a96322cf24ef5d60b41021060c612f58f","target":"graph","created_at":"2026-05-18T00:17:32Z","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 introduce a model of temporal evolution of political opinions which amounts to a dynamical extension of Galam model in which the proportions of inflexibles are treated as dynamical variables. We find that the critical value of inflexibles in the original Galam model now turns into a fixed point of the system whose stability controls the phase trajectory of the political opinions. The appearance of two phases, in which majority-preserving and regime-changing limit cycles are respectively dominant, is found, and also the transition between them is observed.","authors_text":"Serge Galam, Taksu Cheon","cross_cats":["nlin.AO"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2018-02-15T02:26:40Z","title":"Dynamical Galam model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.05389","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:cb41b43bfb8f213c4da28eab8fbe63071824290a135228076ee8522e4fe85313","target":"record","created_at":"2026-05-18T00:17:32Z","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":"905a5370d19175c5ad59802027a1f90620ff7db673243f6a5571b237ae6fb07e","cross_cats_sorted":["nlin.AO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2018-02-15T02:26:40Z","title_canon_sha256":"75acc81edb3a8997b94940f10832855eb888e0d28e4f4bcc0ff8ff5f2877c62e"},"schema_version":"1.0","source":{"id":"1802.05389","kind":"arxiv","version":3}},"canonical_sha256":"9d3670640568c8d31c056238ca68b6eae001179eaf1e75a778f0212c9432a9ae","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9d3670640568c8d31c056238ca68b6eae001179eaf1e75a778f0212c9432a9ae","first_computed_at":"2026-05-18T00:17:32.785117Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:17:32.785117Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yJ3HGbo8Z3JkVDeHWzOufxf0SbMCJuoi6uKxNMMf3ea2dWbF26MAFEfRMJm9po8ZjwpG2MUnq9C6l3X7UMRkBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:17:32.785768Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.05389","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cb41b43bfb8f213c4da28eab8fbe63071824290a135228076ee8522e4fe85313","sha256:3ae41c8a9ffe0a381da0e0cf38666e0a96322cf24ef5d60b41021060c612f58f"],"state_sha256":"c9e22f51d4cbe5ad0487bc48c2c50df1522d29dc511b04bc9d62d934206f7b33"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ViEAMdyWAqVCAdBTtbQOCM0xwOKqNGS7KjuseS5Tu0VmHeE6e5Rtagv9WJR730bOtlbXxP4/YKGblXzkidnWBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T02:33:33.186358Z","bundle_sha256":"ee81f5978ce0046882a7268487054b2707b1f5e53062d3fca63902b6ee659cd6"}}