{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:V2U6VC2I3ODEXK7CGIHZD3UFOX","short_pith_number":"pith:V2U6VC2I","schema_version":"1.0","canonical_sha256":"aea9ea8b48db864babe2320f91ee8575ea055c671c4069a8e225f2eb94130d9d","source":{"kind":"arxiv","id":"1502.05559","version":2},"attestation_state":"computed","paper":{"title":"Nonequilibrium inhomogeneous steady state distribution in disordered, mean-field rotator systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO","nlin.CD"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alessandro Campa, Shamik Gupta, Stefano Ruffo","submitted_at":"2015-02-19T13:11:49Z","abstract_excerpt":"We present a novel method to compute the phase space distribution in the nonequilibrium stationary state of a wide class of mean-field systems involving rotators subject to quenched disordered external drive and dissipation. The method involves a series expansion of the stationary distribution in inverse of the damping coefficient; the expansion coefficients satisfy recursion relations whose solution requires computing a sparse matrix, making numerical evaluation simple and efficient. We illustrate our method for the paradigmatic Kuramoto model of spontaneous collective synchronization and for"},"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":"1502.05559","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-02-19T13:11:49Z","cross_cats_sorted":["nlin.AO","nlin.CD"],"title_canon_sha256":"5226a542c73e3d1e7118661d8dd5dc78349a26a40dcdcf15681d4f0eec053fbe","abstract_canon_sha256":"34d05c749018088bcb25d3f9db6ef6011c339f513358971585500234d83a7f6a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:06.989945Z","signature_b64":"O08XX0kZGuOqJ3KgdgSDgKiSPmqmJqpB3saV8hrBOFZsyPpg7S1X4rWtYvGQSPXbO4mf1U6JfmZzwSdFo5q8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aea9ea8b48db864babe2320f91ee8575ea055c671c4069a8e225f2eb94130d9d","last_reissued_at":"2026-05-18T01:55:06.989462Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:06.989462Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonequilibrium inhomogeneous steady state distribution in disordered, mean-field rotator systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.AO","nlin.CD"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alessandro Campa, Shamik Gupta, Stefano Ruffo","submitted_at":"2015-02-19T13:11:49Z","abstract_excerpt":"We present a novel method to compute the phase space distribution in the nonequilibrium stationary state of a wide class of mean-field systems involving rotators subject to quenched disordered external drive and dissipation. The method involves a series expansion of the stationary distribution in inverse of the damping coefficient; the expansion coefficients satisfy recursion relations whose solution requires computing a sparse matrix, making numerical evaluation simple and efficient. We illustrate our method for the paradigmatic Kuramoto model of spontaneous collective synchronization and for"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.05559","kind":"arxiv","version":2},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1502.05559","created_at":"2026-05-18T01:55:06.989530+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.05559v2","created_at":"2026-05-18T01:55:06.989530+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.05559","created_at":"2026-05-18T01:55:06.989530+00:00"},{"alias_kind":"pith_short_12","alias_value":"V2U6VC2I3ODE","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"V2U6VC2I3ODEXK7C","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"V2U6VC2I","created_at":"2026-05-18T12:29:44.643036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX","json":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX.json","graph_json":"https://pith.science/api/pith-number/V2U6VC2I3ODEXK7CGIHZD3UFOX/graph.json","events_json":"https://pith.science/api/pith-number/V2U6VC2I3ODEXK7CGIHZD3UFOX/events.json","paper":"https://pith.science/paper/V2U6VC2I"},"agent_actions":{"view_html":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX","download_json":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX.json","view_paper":"https://pith.science/paper/V2U6VC2I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.05559&json=true","fetch_graph":"https://pith.science/api/pith-number/V2U6VC2I3ODEXK7CGIHZD3UFOX/graph.json","fetch_events":"https://pith.science/api/pith-number/V2U6VC2I3ODEXK7CGIHZD3UFOX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX/action/storage_attestation","attest_author":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX/action/author_attestation","sign_citation":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX/action/citation_signature","submit_replication":"https://pith.science/pith/V2U6VC2I3ODEXK7CGIHZD3UFOX/action/replication_record"}},"created_at":"2026-05-18T01:55:06.989530+00:00","updated_at":"2026-05-18T01:55:06.989530+00:00"}