{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:4NKDTV2XXXS3KOCK2NLTXXXFZT","short_pith_number":"pith:4NKDTV2X","schema_version":"1.0","canonical_sha256":"e35439d757bde5b5384ad3573bdee5ccebfa1b74ce80fbe5bacb69d4ea88b188","source":{"kind":"arxiv","id":"1609.09011","version":3},"attestation_state":"computed","paper":{"title":"Fixed energy universality for Dyson Brownian motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.PR","authors_text":"Benjamin Landon, Horng-Tzer Yau, Philippe Sosoe","submitted_at":"2016-09-28T17:24:26Z","abstract_excerpt":"We consider Dyson Brownian motion for classical values of $\\beta$ with deterministic initial data $V$. We prove that the local eigenvalue statistics coincide with the GOE/GUE in the fixed energy sense after time $t \\gtrsim 1/N$ if the density of states of $V$ is bounded above and below down to scales $\\eta \\ll t$ in a window of size $L \\gg \\sqrt{t}.$ Our results imply that fixed energy universality holds for essentially any random matrix ensemble for which averaged energy universality was previously known. Our methodology builds on the homogenization theory developed in [BEYY] which reduces th"},"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":"1609.09011","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2016-09-28T17:24:26Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"82125e34e9cc3ba54ad755c27b30ced719ad82e2a8ae9bd313ac786b9e93d83d","abstract_canon_sha256":"a1c053fcde77d78118f817c00a28b52b8d52c53bbc37f64a78d9a7e6f8b3fd08"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:56:30.418600Z","signature_b64":"dDdMGV1dCAMZlDSWLvxTYPUC8c62+ZDNTv07M47WjZaIbTT2fCO8WFqa8ZQV77+PNqKEEainEFT0vIxblH6XAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e35439d757bde5b5384ad3573bdee5ccebfa1b74ce80fbe5bacb69d4ea88b188","last_reissued_at":"2026-05-17T23:56:30.418235Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:56:30.418235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fixed energy universality for Dyson Brownian motion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"math.PR","authors_text":"Benjamin Landon, Horng-Tzer Yau, Philippe Sosoe","submitted_at":"2016-09-28T17:24:26Z","abstract_excerpt":"We consider Dyson Brownian motion for classical values of $\\beta$ with deterministic initial data $V$. We prove that the local eigenvalue statistics coincide with the GOE/GUE in the fixed energy sense after time $t \\gtrsim 1/N$ if the density of states of $V$ is bounded above and below down to scales $\\eta \\ll t$ in a window of size $L \\gg \\sqrt{t}.$ Our results imply that fixed energy universality holds for essentially any random matrix ensemble for which averaged energy universality was previously known. Our methodology builds on the homogenization theory developed in [BEYY] which reduces th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.09011","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1609.09011","created_at":"2026-05-17T23:56:30.418295+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.09011v3","created_at":"2026-05-17T23:56:30.418295+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.09011","created_at":"2026-05-17T23:56:30.418295+00:00"},{"alias_kind":"pith_short_12","alias_value":"4NKDTV2XXXS3","created_at":"2026-05-18T12:29:58.707656+00:00"},{"alias_kind":"pith_short_16","alias_value":"4NKDTV2XXXS3KOCK","created_at":"2026-05-18T12:29:58.707656+00:00"},{"alias_kind":"pith_short_8","alias_value":"4NKDTV2X","created_at":"2026-05-18T12:29:58.707656+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/4NKDTV2XXXS3KOCK2NLTXXXFZT","json":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT.json","graph_json":"https://pith.science/api/pith-number/4NKDTV2XXXS3KOCK2NLTXXXFZT/graph.json","events_json":"https://pith.science/api/pith-number/4NKDTV2XXXS3KOCK2NLTXXXFZT/events.json","paper":"https://pith.science/paper/4NKDTV2X"},"agent_actions":{"view_html":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT","download_json":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT.json","view_paper":"https://pith.science/paper/4NKDTV2X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.09011&json=true","fetch_graph":"https://pith.science/api/pith-number/4NKDTV2XXXS3KOCK2NLTXXXFZT/graph.json","fetch_events":"https://pith.science/api/pith-number/4NKDTV2XXXS3KOCK2NLTXXXFZT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT/action/storage_attestation","attest_author":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT/action/author_attestation","sign_citation":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT/action/citation_signature","submit_replication":"https://pith.science/pith/4NKDTV2XXXS3KOCK2NLTXXXFZT/action/replication_record"}},"created_at":"2026-05-17T23:56:30.418295+00:00","updated_at":"2026-05-17T23:56:30.418295+00:00"}