{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:IVVSZMT3T2UBXRI6JSFB6LTF23","short_pith_number":"pith:IVVSZMT3","schema_version":"1.0","canonical_sha256":"456b2cb27b9ea81bc51e4c8a1f2e65d6e2aa62ce445fbd57a01250bc933a0d9b","source":{"kind":"arxiv","id":"2411.14851","version":1},"attestation_state":"computed","paper":{"title":"Effects of coupling range on the dynamics of swarmalators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nlin.AO","authors_text":"Dibakar Ghosh, Gourab Kumar Sar, Kevin O'Keeffe","submitted_at":"2024-11-22T10:56:39Z","abstract_excerpt":"We study a variant of the one-dimensional swarmalator model where the units' interactions have a controllable length scale or range. We tune the model from the long-range regime, which is well studied, into the short-range regime, which is understudied, and find diverse collective states: sync dots, where the swarmalators arrange themselves into k>1 delta points of perfect synchrony, q-waves, where the swarmalators form spatiotemporal waves with winding number q>1, and an active state where unsteady oscillations are found. We present the phase diagram and derive most of the threshold boundarie"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2411.14851","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nlin.AO","submitted_at":"2024-11-22T10:56:39Z","cross_cats_sorted":[],"title_canon_sha256":"40806a27977b63b5ce9d4075f0705eedc11a37206816720b32cd416c045cb1f9","abstract_canon_sha256":"67beb49d9a9b10adf951210cdccc1f62229349401a10e495b44ea45bd5dee11c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:39:12.712045Z","signature_b64":"efm2siP5UwinvH+lRaELnUJAEoggUbg1IM9ZCYhaCG1ZqS2EPwwjeiuueVrvAbFZO79C+PE+xTz7x/tdimikCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"456b2cb27b9ea81bc51e4c8a1f2e65d6e2aa62ce445fbd57a01250bc933a0d9b","last_reissued_at":"2026-07-05T09:39:12.711574Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:39:12.711574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of coupling range on the dynamics of swarmalators","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nlin.AO","authors_text":"Dibakar Ghosh, Gourab Kumar Sar, Kevin O'Keeffe","submitted_at":"2024-11-22T10:56:39Z","abstract_excerpt":"We study a variant of the one-dimensional swarmalator model where the units' interactions have a controllable length scale or range. We tune the model from the long-range regime, which is well studied, into the short-range regime, which is understudied, and find diverse collective states: sync dots, where the swarmalators arrange themselves into k>1 delta points of perfect synchrony, q-waves, where the swarmalators form spatiotemporal waves with winding number q>1, and an active state where unsteady oscillations are found. We present the phase diagram and derive most of the threshold boundarie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.14851","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.14851/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2411.14851","created_at":"2026-07-05T09:39:12.711629+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.14851v1","created_at":"2026-07-05T09:39:12.711629+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.14851","created_at":"2026-07-05T09:39:12.711629+00:00"},{"alias_kind":"pith_short_12","alias_value":"IVVSZMT3T2UB","created_at":"2026-07-05T09:39:12.711629+00:00"},{"alias_kind":"pith_short_16","alias_value":"IVVSZMT3T2UBXRI6","created_at":"2026-07-05T09:39:12.711629+00:00"},{"alias_kind":"pith_short_8","alias_value":"IVVSZMT3","created_at":"2026-07-05T09:39:12.711629+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.14851","citing_title":"Effects of coupling range on the dynamics of swarmalators","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23","json":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23.json","graph_json":"https://pith.science/api/pith-number/IVVSZMT3T2UBXRI6JSFB6LTF23/graph.json","events_json":"https://pith.science/api/pith-number/IVVSZMT3T2UBXRI6JSFB6LTF23/events.json","paper":"https://pith.science/paper/IVVSZMT3"},"agent_actions":{"view_html":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23","download_json":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23.json","view_paper":"https://pith.science/paper/IVVSZMT3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.14851&json=true","fetch_graph":"https://pith.science/api/pith-number/IVVSZMT3T2UBXRI6JSFB6LTF23/graph.json","fetch_events":"https://pith.science/api/pith-number/IVVSZMT3T2UBXRI6JSFB6LTF23/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23/action/storage_attestation","attest_author":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23/action/author_attestation","sign_citation":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23/action/citation_signature","submit_replication":"https://pith.science/pith/IVVSZMT3T2UBXRI6JSFB6LTF23/action/replication_record"}},"created_at":"2026-07-05T09:39:12.711629+00:00","updated_at":"2026-07-05T09:39:12.711629+00:00"}