{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:KVEEDV4L3RLSRSGXZBGAHIWSBJ","short_pith_number":"pith:KVEEDV4L","schema_version":"1.0","canonical_sha256":"554841d78bdc5728c8d7c84c03a2d20a6e50d04d17dca1f35ea714627b96e7bd","source":{"kind":"arxiv","id":"0909.1047","version":1},"attestation_state":"computed","paper":{"title":"Large Deviation Principle for Non-Interacting Boson Random Point Processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Hiroshi Tamura, Valentin Zagrebnov (CPT)","submitted_at":"2009-09-05T18:41:41Z","abstract_excerpt":"Limit theorems, including the large deviation principle, are established for random point processes (fields), which describe the position distributions of the perfect boson gas in the regime of the Bose-Einstein condensation. We compare these results with those for the case of the normal phase."},"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":"0909.1047","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2009-09-05T18:41:41Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"10871dd8dfd815e88f0a6292db1053548c60053315abf5728b703f9b8bb19cf4","abstract_canon_sha256":"8e0d1813cce3ffacf7302f3c2e09ceda721cc3f2efbfeaffce28682b1da2b701"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:11:59.438869Z","signature_b64":"/XkaEicJ+D2b8Tvc7h2Cz1cdLf2TwSU7rnmxaFaN/cazoAgPVlSVIlJmDz3XFPdelFZ3JsXZnmb8Acxjf8vsDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"554841d78bdc5728c8d7c84c03a2d20a6e50d04d17dca1f35ea714627b96e7bd","last_reissued_at":"2026-05-18T02:11:59.437627Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:11:59.437627Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large Deviation Principle for Non-Interacting Boson Random Point Processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Hiroshi Tamura, Valentin Zagrebnov (CPT)","submitted_at":"2009-09-05T18:41:41Z","abstract_excerpt":"Limit theorems, including the large deviation principle, are established for random point processes (fields), which describe the position distributions of the perfect boson gas in the regime of the Bose-Einstein condensation. We compare these results with those for the case of the normal phase."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0909.1047","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":"0909.1047","created_at":"2026-05-18T02:11:59.438144+00:00"},{"alias_kind":"arxiv_version","alias_value":"0909.1047v1","created_at":"2026-05-18T02:11:59.438144+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0909.1047","created_at":"2026-05-18T02:11:59.438144+00:00"},{"alias_kind":"pith_short_12","alias_value":"KVEEDV4L3RLS","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"KVEEDV4L3RLSRSGX","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"KVEEDV4L","created_at":"2026-05-18T12:26:00.592388+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/KVEEDV4L3RLSRSGXZBGAHIWSBJ","json":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ.json","graph_json":"https://pith.science/api/pith-number/KVEEDV4L3RLSRSGXZBGAHIWSBJ/graph.json","events_json":"https://pith.science/api/pith-number/KVEEDV4L3RLSRSGXZBGAHIWSBJ/events.json","paper":"https://pith.science/paper/KVEEDV4L"},"agent_actions":{"view_html":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ","download_json":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ.json","view_paper":"https://pith.science/paper/KVEEDV4L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0909.1047&json=true","fetch_graph":"https://pith.science/api/pith-number/KVEEDV4L3RLSRSGXZBGAHIWSBJ/graph.json","fetch_events":"https://pith.science/api/pith-number/KVEEDV4L3RLSRSGXZBGAHIWSBJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ/action/storage_attestation","attest_author":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ/action/author_attestation","sign_citation":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ/action/citation_signature","submit_replication":"https://pith.science/pith/KVEEDV4L3RLSRSGXZBGAHIWSBJ/action/replication_record"}},"created_at":"2026-05-18T02:11:59.438144+00:00","updated_at":"2026-05-18T02:11:59.438144+00:00"}