{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:RE2A25XL7R2EX3XN7I6NYAXMK6","short_pith_number":"pith:RE2A25XL","schema_version":"1.0","canonical_sha256":"89340d76ebfc744beeedfa3cdc02ec57b16edaa5eceb8a7b3d140a13cbf5e86f","source":{"kind":"arxiv","id":"astro-ph/9702100","version":2},"attestation_state":"computed","paper":{"title":"Forecasting Cosmic Parameter Errors from Microwave Background Anisotropy Experiments","license":"","headline":"","cross_cats":[],"primary_cat":"astro-ph","authors_text":"George Efstathiou, J. Richard Bond, Max Tegmark","submitted_at":"1997-02-12T04:19:10Z","abstract_excerpt":"Accurate measurements of the cosmic microwave background (CMB) anisotropies with an angular resolution of a few arcminutes can be used to determine fundamental cosmological parameters such as the densities of baryons, cold and hot dark matter, and certain combinations of the cosmological constant and the curvature of the Universe to percent-level precision. Assuming the true theory is a variant of inflationary cold dark matter cosmologies, we calculate the accuracy with which cosmological parameters can be determined by the next generation of CMB satellites, MAP and Planck. We pay special atte"},"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":"astro-ph/9702100","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"astro-ph","submitted_at":"1997-02-12T04:19:10Z","cross_cats_sorted":[],"title_canon_sha256":"aef72c412a9ff439bf54a46e1aeb6e13c126048e0fbd9a04e8617da3e6b70585","abstract_canon_sha256":"9b00143cac215667431263453289a37904d31cb6c9262e83e7edec42aa71f6a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:58.818750Z","signature_b64":"crCO7WyRqymtEGtKYdKT73SU0VIGSiOe8qfXN+aJ3bu6tgUAUdYOKprL/GwNq/fJwGjIrG76ZjDzDHXv6Cz9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89340d76ebfc744beeedfa3cdc02ec57b16edaa5eceb8a7b3d140a13cbf5e86f","last_reissued_at":"2026-05-18T01:22:58.818068Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:58.818068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Forecasting Cosmic Parameter Errors from Microwave Background Anisotropy Experiments","license":"","headline":"","cross_cats":[],"primary_cat":"astro-ph","authors_text":"George Efstathiou, J. Richard Bond, Max Tegmark","submitted_at":"1997-02-12T04:19:10Z","abstract_excerpt":"Accurate measurements of the cosmic microwave background (CMB) anisotropies with an angular resolution of a few arcminutes can be used to determine fundamental cosmological parameters such as the densities of baryons, cold and hot dark matter, and certain combinations of the cosmological constant and the curvature of the Universe to percent-level precision. Assuming the true theory is a variant of inflationary cold dark matter cosmologies, we calculate the accuracy with which cosmological parameters can be determined by the next generation of CMB satellites, MAP and Planck. We pay special atte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"astro-ph/9702100","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":"astro-ph/9702100","created_at":"2026-05-18T01:22:58.818169+00:00"},{"alias_kind":"arxiv_version","alias_value":"astro-ph/9702100v2","created_at":"2026-05-18T01:22:58.818169+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.astro-ph/9702100","created_at":"2026-05-18T01:22:58.818169+00:00"},{"alias_kind":"pith_short_12","alias_value":"RE2A25XL7R2E","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"RE2A25XL7R2EX3XN","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"RE2A25XL","created_at":"2026-05-18T12:25:48.327863+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.23492","citing_title":"The open-Universe signal: A model artifact rather than genuine curvature","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6","json":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6.json","graph_json":"https://pith.science/api/pith-number/RE2A25XL7R2EX3XN7I6NYAXMK6/graph.json","events_json":"https://pith.science/api/pith-number/RE2A25XL7R2EX3XN7I6NYAXMK6/events.json","paper":"https://pith.science/paper/RE2A25XL"},"agent_actions":{"view_html":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6","download_json":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6.json","view_paper":"https://pith.science/paper/RE2A25XL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=astro-ph/9702100&json=true","fetch_graph":"https://pith.science/api/pith-number/RE2A25XL7R2EX3XN7I6NYAXMK6/graph.json","fetch_events":"https://pith.science/api/pith-number/RE2A25XL7R2EX3XN7I6NYAXMK6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6/action/storage_attestation","attest_author":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6/action/author_attestation","sign_citation":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6/action/citation_signature","submit_replication":"https://pith.science/pith/RE2A25XL7R2EX3XN7I6NYAXMK6/action/replication_record"}},"created_at":"2026-05-18T01:22:58.818169+00:00","updated_at":"2026-05-18T01:22:58.818169+00:00"}