{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:2PHC37RVTLF4KWF72JMWWUHQCO","short_pith_number":"pith:2PHC37RV","schema_version":"1.0","canonical_sha256":"d3ce2dfe359acbc558bfd2596b50f013996c4c7ab6514ae6ac6c512ac710a105","source":{"kind":"arxiv","id":"1306.4277","version":1},"attestation_state":"computed","paper":{"title":"Eigenvectors of Sample Covariance Matrices: Universality of global fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.PR","authors_text":"Ali Bouferroum","submitted_at":"2013-06-18T17:40:40Z","abstract_excerpt":"In this paper, we prove a universality result of convergence for a bivariate random process defined by the eigenvectors of a sample covariance matrix. Let $V_n=(v_{ij})_{i \\leq n,\\, j\\leq m}$ be a $n\\times m$ random matrix, where $(n/m)\\to y > 0$ as $ n \\to \\infty$, and let $X_n=(1/m) V_n V^{*}_n $ be the sample covariance matrix associated to $V_n \\:$. Consider the spectral decomposition of $X_n$ given by $ U_n D_n U_n^{*}$, where $U_n=(u_{ij})_{n\\times n}$ is an eigenmatrix of $X_n$. We prove, under some moments conditions, that the bivariate random process $<B_{s,t}^{n} = \\underset{1\\leq j "},"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":"1306.4277","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2013-06-18T17:40:40Z","cross_cats_sorted":[],"title_canon_sha256":"14c603ef627651ae69edea700cd823bc8c0a1ff47ec5664180934847ecfae1d4","abstract_canon_sha256":"ec90e46b1a00a198e71fc036160d2f372430904df01ed40eac4a2710ddf7f362"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:20:36.590347Z","signature_b64":"lLqHBVEevP8T04Zs0ouHsFujK3oPxsxmE29DWatje+rKwPd/AQRIDHX63qscaZP8Ly19Ir2snlF9jGqxCOD8CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3ce2dfe359acbc558bfd2596b50f013996c4c7ab6514ae6ac6c512ac710a105","last_reissued_at":"2026-05-18T03:20:36.589449Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:20:36.589449Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Eigenvectors of Sample Covariance Matrices: Universality of global fluctuations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.PR","authors_text":"Ali Bouferroum","submitted_at":"2013-06-18T17:40:40Z","abstract_excerpt":"In this paper, we prove a universality result of convergence for a bivariate random process defined by the eigenvectors of a sample covariance matrix. Let $V_n=(v_{ij})_{i \\leq n,\\, j\\leq m}$ be a $n\\times m$ random matrix, where $(n/m)\\to y > 0$ as $ n \\to \\infty$, and let $X_n=(1/m) V_n V^{*}_n $ be the sample covariance matrix associated to $V_n \\:$. Consider the spectral decomposition of $X_n$ given by $ U_n D_n U_n^{*}$, where $U_n=(u_{ij})_{n\\times n}$ is an eigenmatrix of $X_n$. We prove, under some moments conditions, that the bivariate random process $<B_{s,t}^{n} = \\underset{1\\leq j "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.4277","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":""},"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":"1306.4277","created_at":"2026-05-18T03:20:36.589590+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.4277v1","created_at":"2026-05-18T03:20:36.589590+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.4277","created_at":"2026-05-18T03:20:36.589590+00:00"},{"alias_kind":"pith_short_12","alias_value":"2PHC37RVTLF4","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_16","alias_value":"2PHC37RVTLF4KWF7","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_8","alias_value":"2PHC37RV","created_at":"2026-05-18T12:27:32.513160+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01064","citing_title":"Functional Renormalization for Signal Detection: Dimensional Analysis and Dimensional Phase Transition for Nearly Continuous Spectra Effective Field Theory","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO","json":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO.json","graph_json":"https://pith.science/api/pith-number/2PHC37RVTLF4KWF72JMWWUHQCO/graph.json","events_json":"https://pith.science/api/pith-number/2PHC37RVTLF4KWF72JMWWUHQCO/events.json","paper":"https://pith.science/paper/2PHC37RV"},"agent_actions":{"view_html":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO","download_json":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO.json","view_paper":"https://pith.science/paper/2PHC37RV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.4277&json=true","fetch_graph":"https://pith.science/api/pith-number/2PHC37RVTLF4KWF72JMWWUHQCO/graph.json","fetch_events":"https://pith.science/api/pith-number/2PHC37RVTLF4KWF72JMWWUHQCO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO/action/storage_attestation","attest_author":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO/action/author_attestation","sign_citation":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO/action/citation_signature","submit_replication":"https://pith.science/pith/2PHC37RVTLF4KWF72JMWWUHQCO/action/replication_record"}},"created_at":"2026-05-18T03:20:36.589590+00:00","updated_at":"2026-05-18T03:20:36.589590+00:00"}