{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:2VJAWFI7HQDQA7VGPTRY5SZALH","short_pith_number":"pith:2VJAWFI7","schema_version":"1.0","canonical_sha256":"d5520b151f3c07007ea67ce38ecb2059cdb5e2346dc980b13fe43a6fcafa7578","source":{"kind":"arxiv","id":"2111.05760","version":2},"attestation_state":"computed","paper":{"title":"Inflationary epoch in the presence of holographic dark energy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"astro-ph.CO","authors_text":"Alexander Ganz, Chunshan Lin, Paola C. M. Delgado","submitted_at":"2021-11-10T16:05:35Z","abstract_excerpt":"We analyze the effects of the holographic dark energy model in a single field slow-roll inflation, taking into account both the holographic and the dark radiation components. In particular, we obtain the background evolution and compute the scalar and tensor power spectra. For the scalar sector we show that the power spectrum of the curvature perturbation encompasses the standard single field result and a correction proportional to $\\Omega_{\\rm hde}/\\epsilon$, where $\\Omega_{\\rm hde}$ is the fractional density of the holographic component and $\\epsilon$ is the first slow-roll parameter. This c"},"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":"2111.05760","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.CO","submitted_at":"2021-11-10T16:05:35Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"dcb87fe3771804cadcdce6027c55d689b106eeb99525abc40ff675aa5d170069","abstract_canon_sha256":"3c011296ab7673e8d76240f451e0e48cca9679d900ad1802d982eacc515a2b1f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:54:16.724245Z","signature_b64":"cyk/rZhCRt/OROr5saOWnc45DuTu0p8JDRHYharWIFJdhYCL24qn2SU84Cm5ha3h+PgOhYd1Km/i/fyOm5JEAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d5520b151f3c07007ea67ce38ecb2059cdb5e2346dc980b13fe43a6fcafa7578","last_reissued_at":"2026-07-05T04:54:16.723827Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:54:16.723827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflationary epoch in the presence of holographic dark energy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"astro-ph.CO","authors_text":"Alexander Ganz, Chunshan Lin, Paola C. M. Delgado","submitted_at":"2021-11-10T16:05:35Z","abstract_excerpt":"We analyze the effects of the holographic dark energy model in a single field slow-roll inflation, taking into account both the holographic and the dark radiation components. In particular, we obtain the background evolution and compute the scalar and tensor power spectra. For the scalar sector we show that the power spectrum of the curvature perturbation encompasses the standard single field result and a correction proportional to $\\Omega_{\\rm hde}/\\epsilon$, where $\\Omega_{\\rm hde}$ is the fractional density of the holographic component and $\\epsilon$ is the first slow-roll parameter. This c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.05760","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2111.05760/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":"2111.05760","created_at":"2026-07-05T04:54:16.723880+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.05760v2","created_at":"2026-07-05T04:54:16.723880+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.05760","created_at":"2026-07-05T04:54:16.723880+00:00"},{"alias_kind":"pith_short_12","alias_value":"2VJAWFI7HQDQ","created_at":"2026-07-05T04:54:16.723880+00:00"},{"alias_kind":"pith_short_16","alias_value":"2VJAWFI7HQDQA7VG","created_at":"2026-07-05T04:54:16.723880+00:00"},{"alias_kind":"pith_short_8","alias_value":"2VJAWFI7","created_at":"2026-07-05T04:54:16.723880+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/2VJAWFI7HQDQA7VGPTRY5SZALH","json":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH.json","graph_json":"https://pith.science/api/pith-number/2VJAWFI7HQDQA7VGPTRY5SZALH/graph.json","events_json":"https://pith.science/api/pith-number/2VJAWFI7HQDQA7VGPTRY5SZALH/events.json","paper":"https://pith.science/paper/2VJAWFI7"},"agent_actions":{"view_html":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH","download_json":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH.json","view_paper":"https://pith.science/paper/2VJAWFI7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.05760&json=true","fetch_graph":"https://pith.science/api/pith-number/2VJAWFI7HQDQA7VGPTRY5SZALH/graph.json","fetch_events":"https://pith.science/api/pith-number/2VJAWFI7HQDQA7VGPTRY5SZALH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH/action/storage_attestation","attest_author":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH/action/author_attestation","sign_citation":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH/action/citation_signature","submit_replication":"https://pith.science/pith/2VJAWFI7HQDQA7VGPTRY5SZALH/action/replication_record"}},"created_at":"2026-07-05T04:54:16.723880+00:00","updated_at":"2026-07-05T04:54:16.723880+00:00"}