{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ZWUOIGSJC2W3FI2FVROWJFDQPM","short_pith_number":"pith:ZWUOIGSJ","schema_version":"1.0","canonical_sha256":"cda8e41a4916adb2a345ac5d6494707b37f9a1a2561082fc04eaabe00cc3e140","source":{"kind":"arxiv","id":"1309.3269","version":3},"attestation_state":"computed","paper":{"title":"Warm Intermediate Inflation in $F(T)$ Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Davood Momeni, Mubasher Jamil, Ratbay Myrzakulov","submitted_at":"2013-09-12T04:45:53Z","abstract_excerpt":"We investigate warm intermediate scenario of the cosmological inflation in $F(T)$ gravity in the limit of high dissipation. The inflationary expansion is driven by the scalar inflaton while the gravitational dynamics follow from the $F(T)$ gravity. We calculate the relevant inflationary observables such as scalar-tensor ratio, power-spectrum indices of density perturbations and gravitational waves and the e-folding parameter. We obtain a ratio of slow-roll parameters to be constant. Our calculations support the warm-intermediate inflationary scenario in a spacetime with torsion. Moreover our r"},"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":"1309.3269","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-09-12T04:45:53Z","cross_cats_sorted":[],"title_canon_sha256":"9c1c5e465708c1d5509c9f9d33d2d5068f54a3f14eb16c755adb40d1ac2f7eee","abstract_canon_sha256":"05738b759a879116844e6ba0fdd11b1648f7cd81cfa2da7a1db8ddd9c333aa16"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:53.622584Z","signature_b64":"ny2iTIydl6VcmsI+inV9LNk3sljaAf1lMOvXpaf1kOTzxG31CR8ZotPN1AjT/5ySLXf2L9DBkwVgiWaY+6GMCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cda8e41a4916adb2a345ac5d6494707b37f9a1a2561082fc04eaabe00cc3e140","last_reissued_at":"2026-05-18T01:55:53.622121Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:53.622121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Warm Intermediate Inflation in $F(T)$ Gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Davood Momeni, Mubasher Jamil, Ratbay Myrzakulov","submitted_at":"2013-09-12T04:45:53Z","abstract_excerpt":"We investigate warm intermediate scenario of the cosmological inflation in $F(T)$ gravity in the limit of high dissipation. The inflationary expansion is driven by the scalar inflaton while the gravitational dynamics follow from the $F(T)$ gravity. We calculate the relevant inflationary observables such as scalar-tensor ratio, power-spectrum indices of density perturbations and gravitational waves and the e-folding parameter. We obtain a ratio of slow-roll parameters to be constant. Our calculations support the warm-intermediate inflationary scenario in a spacetime with torsion. Moreover our r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.3269","kind":"arxiv","version":3},"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":"1309.3269","created_at":"2026-05-18T01:55:53.622196+00:00"},{"alias_kind":"arxiv_version","alias_value":"1309.3269v3","created_at":"2026-05-18T01:55:53.622196+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.3269","created_at":"2026-05-18T01:55:53.622196+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZWUOIGSJC2W3","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZWUOIGSJC2W3FI2F","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZWUOIGSJ","created_at":"2026-05-18T12:28:09.283467+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/ZWUOIGSJC2W3FI2FVROWJFDQPM","json":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM.json","graph_json":"https://pith.science/api/pith-number/ZWUOIGSJC2W3FI2FVROWJFDQPM/graph.json","events_json":"https://pith.science/api/pith-number/ZWUOIGSJC2W3FI2FVROWJFDQPM/events.json","paper":"https://pith.science/paper/ZWUOIGSJ"},"agent_actions":{"view_html":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM","download_json":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM.json","view_paper":"https://pith.science/paper/ZWUOIGSJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1309.3269&json=true","fetch_graph":"https://pith.science/api/pith-number/ZWUOIGSJC2W3FI2FVROWJFDQPM/graph.json","fetch_events":"https://pith.science/api/pith-number/ZWUOIGSJC2W3FI2FVROWJFDQPM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM/action/storage_attestation","attest_author":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM/action/author_attestation","sign_citation":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM/action/citation_signature","submit_replication":"https://pith.science/pith/ZWUOIGSJC2W3FI2FVROWJFDQPM/action/replication_record"}},"created_at":"2026-05-18T01:55:53.622196+00:00","updated_at":"2026-05-18T01:55:53.622196+00:00"}