{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:PSW4PSG5WK4BHVIB2WQQZLRYVV","short_pith_number":"pith:PSW4PSG5","schema_version":"1.0","canonical_sha256":"7cadc7c8ddb2b813d501d5a10cae38ad7e952bcdbfc9245692936f9a9d571c8f","source":{"kind":"arxiv","id":"hep-th/0406217","version":1},"attestation_state":"computed","paper":{"title":"Alpha-states in de Sitter space","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Djordje Minic, Jan de Boer, Vishnu Jejjala","submitted_at":"2004-06-23T21:31:57Z","abstract_excerpt":"Field theory in de Sitter space admits a one-parameter family of vacua determined by a superselection parameter alpha. Of these vacua, the Euclidean vacuum uniquely extrapolates to the vacuum of flat Minkowski space. States which resemble the alpha-vacua can be constructed as excitations above the Euclidean vacuum. Such states have modes alpha(k) which decay faster that k^{(1-d)/2}. Fields in such states exhibit non-local correlations when examined from the perspective of fields in the Euclidean vacuum. The dynamics of such entangled states are fully consistent. If an alpha-state with properti"},"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":"hep-th/0406217","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-06-23T21:31:57Z","cross_cats_sorted":[],"title_canon_sha256":"5b4f454e2d3917b989b8a4ba3f38eed5e97ef313cf2fcbead512e2cefcf58a34","abstract_canon_sha256":"2b0c5739a217f3540d9d5d4f3bc1eb9f1aabf9be884fd048b75b79e92bb174a8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:48:57.578505Z","signature_b64":"AGrvOyGv9rVA1Dt//fvNWbQMHztrmVywKXOGOIuZPipBNaxQYqDGOLN0mnwbGBoZLp70AKVpvoCV85EHvVsaCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7cadc7c8ddb2b813d501d5a10cae38ad7e952bcdbfc9245692936f9a9d571c8f","last_reissued_at":"2026-07-04T16:48:57.578100Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:48:57.578100Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Alpha-states in de Sitter space","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Djordje Minic, Jan de Boer, Vishnu Jejjala","submitted_at":"2004-06-23T21:31:57Z","abstract_excerpt":"Field theory in de Sitter space admits a one-parameter family of vacua determined by a superselection parameter alpha. Of these vacua, the Euclidean vacuum uniquely extrapolates to the vacuum of flat Minkowski space. States which resemble the alpha-vacua can be constructed as excitations above the Euclidean vacuum. Such states have modes alpha(k) which decay faster that k^{(1-d)/2}. Fields in such states exhibit non-local correlations when examined from the perspective of fields in the Euclidean vacuum. The dynamics of such entangled states are fully consistent. If an alpha-state with properti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0406217","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/hep-th/0406217/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":"hep-th/0406217","created_at":"2026-07-04T16:48:57.578160+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0406217v1","created_at":"2026-07-04T16:48:57.578160+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0406217","created_at":"2026-07-04T16:48:57.578160+00:00"},{"alias_kind":"pith_short_12","alias_value":"PSW4PSG5WK4B","created_at":"2026-07-04T16:48:57.578160+00:00"},{"alias_kind":"pith_short_16","alias_value":"PSW4PSG5WK4BHVIB","created_at":"2026-07-04T16:48:57.578160+00:00"},{"alias_kind":"pith_short_8","alias_value":"PSW4PSG5","created_at":"2026-07-04T16:48:57.578160+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2608.08837","citing_title":"Holography in flipped AdS/$\\mathbb{Z}$: Another approach to dS holography","ref_index":62,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV","json":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV.json","graph_json":"https://pith.science/api/pith-number/PSW4PSG5WK4BHVIB2WQQZLRYVV/graph.json","events_json":"https://pith.science/api/pith-number/PSW4PSG5WK4BHVIB2WQQZLRYVV/events.json","paper":"https://pith.science/paper/PSW4PSG5"},"agent_actions":{"view_html":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV","download_json":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV.json","view_paper":"https://pith.science/paper/PSW4PSG5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0406217&json=true","fetch_graph":"https://pith.science/api/pith-number/PSW4PSG5WK4BHVIB2WQQZLRYVV/graph.json","fetch_events":"https://pith.science/api/pith-number/PSW4PSG5WK4BHVIB2WQQZLRYVV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV/action/storage_attestation","attest_author":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV/action/author_attestation","sign_citation":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV/action/citation_signature","submit_replication":"https://pith.science/pith/PSW4PSG5WK4BHVIB2WQQZLRYVV/action/replication_record"}},"created_at":"2026-07-04T16:48:57.578160+00:00","updated_at":"2026-07-04T16:48:57.578160+00:00"}