{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:QS5PMCIXCI5YJ7PIQURSH362RW","short_pith_number":"pith:QS5PMCIX","schema_version":"1.0","canonical_sha256":"84baf60917123b84fde8852323efda8d903dfcd7dddc59faffe22188ce64cb2e","source":{"kind":"arxiv","id":"hep-ph/0305010","version":1},"attestation_state":"computed","paper":{"title":"Cosmological bounds on large extra dimensions from non-thermal production of Kaluza-Klein modes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chris Bird, Maxim Pospelov, Rouzbeh Allahverdi, Stefan Groot Nibbelink","submitted_at":"2003-05-01T19:04:06Z","abstract_excerpt":"The existing cosmological constraints on theories with large extra dimensions rely on the thermal production of the Kaluza-Klein modes of gravitons and radions in the early Universe. Successful inflation and reheating, as well as baryogenesis, typically requires the existence of a TeV-scale field in the bulk, most notably the inflaton. The non-thermal production of KK modes with masses of order 100 GeV accompanying the inflaton decay sets the lower bounds on the fundamental scale M_*. For a 1 TeV inflaton, the late decay of these modes distort the successful predictions of Big Bang Nucleosynth"},"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-ph/0305010","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-05-01T19:04:06Z","cross_cats_sorted":[],"title_canon_sha256":"c2459dc05d62f17ad105b3be920356bf2642516f58defbf383304dd003b70d98","abstract_canon_sha256":"362ae1f877060d1ceba9dc4db3a3b4a97527ad63718954ad1f5e5e77ba7895f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:11:18.688150Z","signature_b64":"Q8o+0yyvXeO0BPkV4E1CGhQgPdac9Xm4noPng6RqalrHJG/0RjZAWCJPzyHx9b1lJs5yeQ554ojbxSiORR0WDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84baf60917123b84fde8852323efda8d903dfcd7dddc59faffe22188ce64cb2e","last_reissued_at":"2026-05-18T04:11:18.687493Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:11:18.687493Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cosmological bounds on large extra dimensions from non-thermal production of Kaluza-Klein modes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chris Bird, Maxim Pospelov, Rouzbeh Allahverdi, Stefan Groot Nibbelink","submitted_at":"2003-05-01T19:04:06Z","abstract_excerpt":"The existing cosmological constraints on theories with large extra dimensions rely on the thermal production of the Kaluza-Klein modes of gravitons and radions in the early Universe. Successful inflation and reheating, as well as baryogenesis, typically requires the existence of a TeV-scale field in the bulk, most notably the inflaton. The non-thermal production of KK modes with masses of order 100 GeV accompanying the inflaton decay sets the lower bounds on the fundamental scale M_*. For a 1 TeV inflaton, the late decay of these modes distort the successful predictions of Big Bang Nucleosynth"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0305010","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":"hep-ph/0305010","created_at":"2026-05-18T04:11:18.687572+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0305010v1","created_at":"2026-05-18T04:11:18.687572+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0305010","created_at":"2026-05-18T04:11:18.687572+00:00"},{"alias_kind":"pith_short_12","alias_value":"QS5PMCIXCI5Y","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"QS5PMCIXCI5YJ7PI","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"QS5PMCIX","created_at":"2026-05-18T12:25:52.051335+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/QS5PMCIXCI5YJ7PIQURSH362RW","json":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW.json","graph_json":"https://pith.science/api/pith-number/QS5PMCIXCI5YJ7PIQURSH362RW/graph.json","events_json":"https://pith.science/api/pith-number/QS5PMCIXCI5YJ7PIQURSH362RW/events.json","paper":"https://pith.science/paper/QS5PMCIX"},"agent_actions":{"view_html":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW","download_json":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW.json","view_paper":"https://pith.science/paper/QS5PMCIX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0305010&json=true","fetch_graph":"https://pith.science/api/pith-number/QS5PMCIXCI5YJ7PIQURSH362RW/graph.json","fetch_events":"https://pith.science/api/pith-number/QS5PMCIXCI5YJ7PIQURSH362RW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW/action/storage_attestation","attest_author":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW/action/author_attestation","sign_citation":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW/action/citation_signature","submit_replication":"https://pith.science/pith/QS5PMCIXCI5YJ7PIQURSH362RW/action/replication_record"}},"created_at":"2026-05-18T04:11:18.687572+00:00","updated_at":"2026-05-18T04:11:18.687572+00:00"}