{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:VJAJFZ4O3EJFEHAB2MFZ34WEHJ","short_pith_number":"pith:VJAJFZ4O","canonical_record":{"source":{"id":"2605.17627","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-05-17T19:48:32Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"d8854d7dd699be4ac0fb63edf19eb6b3fd760f0fde036ce318df877a483b5d32","abstract_canon_sha256":"df4be56fd42ff0019219aea3461ed73afb510dcda314ca6c3342225c0a6fe5d6"},"schema_version":"1.0"},"canonical_sha256":"aa4092e78ed912521c01d30b9df2c43a61cd9a86162104858571542dd29a5315","source":{"kind":"arxiv","id":"2605.17627","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.17627","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"arxiv_version","alias_value":"2605.17627v1","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.17627","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_12","alias_value":"VJAJFZ4O3EJF","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_16","alias_value":"VJAJFZ4O3EJFEHAB","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_8","alias_value":"VJAJFZ4O","created_at":"2026-05-20T00:04:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:VJAJFZ4O3EJFEHAB2MFZ34WEHJ","target":"record","payload":{"canonical_record":{"source":{"id":"2605.17627","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-05-17T19:48:32Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"d8854d7dd699be4ac0fb63edf19eb6b3fd760f0fde036ce318df877a483b5d32","abstract_canon_sha256":"df4be56fd42ff0019219aea3461ed73afb510dcda314ca6c3342225c0a6fe5d6"},"schema_version":"1.0"},"canonical_sha256":"aa4092e78ed912521c01d30b9df2c43a61cd9a86162104858571542dd29a5315","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:04:49.411124Z","signature_b64":"Gvk2zI0u0TlalsSK+/jzEPdJi5X8hGQHFcSHmxY2gx/HJaC552WJBZZ7a9QYaAK3gHcayP03g9FKPaeoyAUYDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa4092e78ed912521c01d30b9df2c43a61cd9a86162104858571542dd29a5315","last_reissued_at":"2026-05-20T00:04:49.410237Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:04:49.410237Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.17627","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":"2026-05-20T00:04:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QH+DV3UHovGDzi+mqMiwiPUtgoVDt2IKjETkuYwhOw2W2K3SjsoVg10vo4+77jcy0PXK/bmMkP+V7KgpsB92CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T12:08:41.701650Z"},"content_sha256":"85937d057be1fc9a956c4a3b2aabe3d5b047f5cf5a7e3128df38ea4d9ac2a5f1","schema_version":"1.0","event_id":"sha256:85937d057be1fc9a956c4a3b2aabe3d5b047f5cf5a7e3128df38ea4d9ac2a5f1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:VJAJFZ4O3EJFEHAB2MFZ34WEHJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Collective dynamics of active matter with orientation-weighted alignment","license":"http://creativecommons.org/licenses/by/4.0/","headline":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone.","cross_cats":["nlin.PS"],"primary_cat":"cond-mat.soft","authors_text":"Alexander Yakimenko, Bohdan Dobosh","submitted_at":"2026-05-17T19:48:32Z","abstract_excerpt":"We study an agent-based model of self-propelled particles with a velocity-dependent alignment rule. This interaction is orientation weighted and acts along the line connecting neighboring particles. Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model."},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The model assumes that the alignment interaction is strictly orientation-weighted and acts exactly along the line connecting neighboring particles; if this geometric and directional weighting is not physically realized or if boundary/periodic conditions dominate the observed phases, the claimed breadth of regimes would not follow from the stated rule.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"An agent-based model with orientation-weighted velocity-dependent alignment generates disordered, flocking, jammed, and active-crystal-like collective phases by varying alignment strength.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"4fcb4816393d5050e5197a206c1c278259d223513eb27f13d2edaab579320d9c"},"source":{"id":"2605.17627","kind":"arxiv","version":1},"verdict":{"id":"2fa58746-08a0-4e4a-85fa-ea2b6aa476d2","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T22:03:43.481744Z","strongest_claim":"Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model.","one_line_summary":"An agent-based model with orientation-weighted velocity-dependent alignment generates disordered, flocking, jammed, and active-crystal-like collective phases by varying alignment strength.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The model assumes that the alignment interaction is strictly orientation-weighted and acts exactly along the line connecting neighboring particles; if this geometric and directional weighting is not physically realized or if boundary/periodic conditions dominate the observed phases, the claimed breadth of regimes would not follow from the stated rule.","pith_extraction_headline":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.17627/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"cited_work_retraction","ran_at":"2026-05-19T22:52:44.297974Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T22:31:19.518217Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T22:12:15.524773Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T21:33:23.561534Z","status":"skipped","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T21:21:57.486375Z","status":"completed","version":"1.0.0","findings_count":0}],"snapshot_sha256":"04fcce70a577f6e50f9c8b4a098a756ce1fba8ba3309860c893c3a062d0db274"},"references":{"count":38,"sample":[{"doi":"","year":2010,"title":"Ramaswamy, The mechanics and statistics of active matter, Annual Review of Condensed Matter Physics1, 323 (2010)","work_id":"b3b2186e-e36d-46a4-a2f7-075ad1efb3af","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2018,"title":"´Etienne Fodor and M. C. Marchetti, The statistical physics of active matter: From self-catalytic colloids to living cells, Physica A: Statistical Mechanics and its Ap- plications504, 106 (2018), lect","work_id":"6e08c83f-2ad7-4259-8571-6ca5c0e4fbf5","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2013,"title":"M. C. Marchetti, J.-F. Joanny, S. Ramaswamy, T. B. Liverpool, J. Prost, M. Rao, and R. A. Simha, Hydrody- namics of soft active matter, Rev. Mod. Phys.85, 1143 (2013)","work_id":"0040683a-151d-4e43-9853-51dde584192f","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2012,"title":"T. Sanchez, D. T. N. Chen, S. J. DeCamp, M. Heymann, and Z. Dogic, Spontaneous motion in hierarchically as- sembled active matter, Nature491, 431 (2012)","work_id":"c5f23fe3-a7d7-4317-91b4-db79d93d8d4e","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2013,"title":"A. Bricard, J.-B. Caussin, N. Desreumaux, O. Dauchot, and D. Bartolo, Emergence of macroscopic directed mo- tion in populations of motile colloids, Nature503, 95 (2013)","work_id":"931cf8d5-9aa2-4950-aec4-2435ca9042f7","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":38,"snapshot_sha256":"9aa4b32b2441d91d352138cb9a615d0b6f9dbdd53cab183d9181effae489b73a","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":"2fa58746-08a0-4e4a-85fa-ea2b6aa476d2"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:04:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fop1jJt+jUdyP5oBvhGY681GV9rtk6q+SFH9GLzrBMpelEciXwwAlVCMy69TR4KuXXh+6QAUp6h8JL4ZOpuBDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T12:08:41.702884Z"},"content_sha256":"fd6e2a43c80bed333623a8c5b6150e7a16ee67c5ac494ad68ab62fb22568920d","schema_version":"1.0","event_id":"sha256:fd6e2a43c80bed333623a8c5b6150e7a16ee67c5ac494ad68ab62fb22568920d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/bundle.json","state_url":"https://pith.science/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/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":"2026-05-22T12:08:41Z","links":{"resolver":"https://pith.science/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ","bundle":"https://pith.science/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/bundle.json","state":"https://pith.science/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VJAJFZ4O3EJFEHAB2MFZ34WEHJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:VJAJFZ4O3EJFEHAB2MFZ34WEHJ","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":"df4be56fd42ff0019219aea3461ed73afb510dcda314ca6c3342225c0a6fe5d6","cross_cats_sorted":["nlin.PS"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-05-17T19:48:32Z","title_canon_sha256":"d8854d7dd699be4ac0fb63edf19eb6b3fd760f0fde036ce318df877a483b5d32"},"schema_version":"1.0","source":{"id":"2605.17627","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.17627","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"arxiv_version","alias_value":"2605.17627v1","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.17627","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_12","alias_value":"VJAJFZ4O3EJF","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_16","alias_value":"VJAJFZ4O3EJFEHAB","created_at":"2026-05-20T00:04:49Z"},{"alias_kind":"pith_short_8","alias_value":"VJAJFZ4O","created_at":"2026-05-20T00:04:49Z"}],"graph_snapshots":[{"event_id":"sha256:fd6e2a43c80bed333623a8c5b6150e7a16ee67c5ac494ad68ab62fb22568920d","target":"graph","created_at":"2026-05-20T00:04:49Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The model assumes that the alignment interaction is strictly orientation-weighted and acts exactly along the line connecting neighboring particles; if this geometric and directional weighting is not physically realized or if boundary/periodic conditions dominate the observed phases, the claimed breadth of regimes would not follow from the stated rule."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"An agent-based model with orientation-weighted velocity-dependent alignment generates disordered, flocking, jammed, and active-crystal-like collective phases by varying alignment strength."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone."}],"snapshot_sha256":"4fcb4816393d5050e5197a206c1c278259d223513eb27f13d2edaab579320d9c"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"cited_work_retraction","ran_at":"2026-05-19T22:52:44.297974Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_title_agreement","ran_at":"2026-05-19T22:31:19.518217Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T22:12:15.524773Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T21:33:23.561534Z","status":"skipped","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T21:21:57.486375Z","status":"completed","version":"1.0.0"}],"endpoint":"/pith/2605.17627/integrity.json","findings":[],"snapshot_sha256":"04fcce70a577f6e50f9c8b4a098a756ce1fba8ba3309860c893c3a062d0db274","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study an agent-based model of self-propelled particles with a velocity-dependent alignment rule. This interaction is orientation weighted and acts along the line connecting neighboring particles. Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model.","authors_text":"Alexander Yakimenko, Bohdan Dobosh","cross_cats":["nlin.PS"],"headline":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-05-17T19:48:32Z","title":"Collective dynamics of active matter with orientation-weighted alignment"},"references":{"count":38,"internal_anchors":0,"resolved_work":38,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Ramaswamy, The mechanics and statistics of active matter, Annual Review of Condensed Matter Physics1, 323 (2010)","work_id":"b3b2186e-e36d-46a4-a2f7-075ad1efb3af","year":2010},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"´Etienne Fodor and M. C. Marchetti, The statistical physics of active matter: From self-catalytic colloids to living cells, Physica A: Statistical Mechanics and its Ap- plications504, 106 (2018), lect","work_id":"6e08c83f-2ad7-4259-8571-6ca5c0e4fbf5","year":2018},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"M. C. Marchetti, J.-F. Joanny, S. Ramaswamy, T. B. Liverpool, J. Prost, M. Rao, and R. A. Simha, Hydrody- namics of soft active matter, Rev. Mod. Phys.85, 1143 (2013)","work_id":"0040683a-151d-4e43-9853-51dde584192f","year":2013},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"T. Sanchez, D. T. N. Chen, S. J. DeCamp, M. Heymann, and Z. Dogic, Spontaneous motion in hierarchically as- sembled active matter, Nature491, 431 (2012)","work_id":"c5f23fe3-a7d7-4317-91b4-db79d93d8d4e","year":2012},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"A. Bricard, J.-B. Caussin, N. Desreumaux, O. Dauchot, and D. Bartolo, Emergence of macroscopic directed mo- tion in populations of motile colloids, Nature503, 95 (2013)","work_id":"931cf8d5-9aa2-4950-aec4-2435ca9042f7","year":2013}],"snapshot_sha256":"9aa4b32b2441d91d352138cb9a615d0b6f9dbdd53cab183d9181effae489b73a"},"source":{"id":"2605.17627","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T22:03:43.481744Z","id":"2fa58746-08a0-4e4a-85fa-ea2b6aa476d2","model_set":{"reader":"grok-4.3"},"one_line_summary":"An agent-based model with orientation-weighted velocity-dependent alignment generates disordered, flocking, jammed, and active-crystal-like collective phases by varying alignment strength.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"A simple orientation-weighted alignment rule generates multiple collective regimes in self-propelled particles by tuning its strength alone.","strongest_claim":"Tuning the alignment strength produces several distinct collective regimes, including disordered gas-like motion, coherent flocking, jammed high-density states, and densely ordered moving clusters with active-crystal-like behavior. These results show that a simple local alignment rule can generate a broad range of nonequilibrium collective dynamics within a single microscopic model.","weakest_assumption":"The model assumes that the alignment interaction is strictly orientation-weighted and acts exactly along the line connecting neighboring particles; if this geometric and directional weighting is not physically realized or if boundary/periodic conditions dominate the observed phases, the claimed breadth of regimes would not follow from the stated rule."}},"verdict_id":"2fa58746-08a0-4e4a-85fa-ea2b6aa476d2"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:85937d057be1fc9a956c4a3b2aabe3d5b047f5cf5a7e3128df38ea4d9ac2a5f1","target":"record","created_at":"2026-05-20T00:04:49Z","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":"df4be56fd42ff0019219aea3461ed73afb510dcda314ca6c3342225c0a6fe5d6","cross_cats_sorted":["nlin.PS"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.soft","submitted_at":"2026-05-17T19:48:32Z","title_canon_sha256":"d8854d7dd699be4ac0fb63edf19eb6b3fd760f0fde036ce318df877a483b5d32"},"schema_version":"1.0","source":{"id":"2605.17627","kind":"arxiv","version":1}},"canonical_sha256":"aa4092e78ed912521c01d30b9df2c43a61cd9a86162104858571542dd29a5315","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"aa4092e78ed912521c01d30b9df2c43a61cd9a86162104858571542dd29a5315","first_computed_at":"2026-05-20T00:04:49.410237Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:04:49.410237Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Gvk2zI0u0TlalsSK+/jzEPdJi5X8hGQHFcSHmxY2gx/HJaC552WJBZZ7a9QYaAK3gHcayP03g9FKPaeoyAUYDg==","signature_status":"signed_v1","signed_at":"2026-05-20T00:04:49.411124Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.17627","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:85937d057be1fc9a956c4a3b2aabe3d5b047f5cf5a7e3128df38ea4d9ac2a5f1","sha256:fd6e2a43c80bed333623a8c5b6150e7a16ee67c5ac494ad68ab62fb22568920d"],"state_sha256":"3dd5805291837b45dfeb425d8eaafe80c47ac904ea61c8044ffecfefbb5ea067"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mZk+9yjHvKVbEu/kTsfS68WiTvP2XrBAYh3yDDm4y0jIqAi4YYIu/7GyVgWFIW14Nvg76DDaoN38QNLhFYlADw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T12:08:41.707904Z","bundle_sha256":"8772a010b9210bf7cce2b7ee2d318a2ae1c0e2f7182c5f60e0a5f6c52389cfc1"}}