{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:2O6JDHD2SZB32QFRBWVP5CNFMS","short_pith_number":"pith:2O6JDHD2","schema_version":"1.0","canonical_sha256":"d3bc919c7a9643bd40b10daafe89a564a9b913aba3d7e41b3da527fe9a66e03b","source":{"kind":"arxiv","id":"1011.2794","version":1},"attestation_state":"computed","paper":{"title":"Entropy Production during Asymptotically Safe Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alfio Bonanno, Martin Reuter","submitted_at":"2010-11-11T23:24:28Z","abstract_excerpt":"The Asymptotic Safety scenario predicts that the deep ultraviolet of Quantum Einstein Gravity is governed by a nontrivial renormalization group fixed point. Analyzing its implications for cosmology using renormalization group improved Einstein equations we find that it can give rise to a phase of inflationary expansion in the early Universe. Inflation is a pure quantum effect here and requires no inflaton field. It is driven by the cosmological constant and ends automatically when the renormalization group evolution has reduced the vacuum energy to the level of the matter energy density. The q"},"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":"1011.2794","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-11-11T23:24:28Z","cross_cats_sorted":[],"title_canon_sha256":"cbadf251fbcdb85979963820dfaebebc3cb5966325066e9ad878b2d6e298826c","abstract_canon_sha256":"feb93da31c10b276993af1621bc5325e31372255e6476f6fe85ba2f9dcc41971"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:48.488549Z","signature_b64":"EcboNMZliSFY9c01FiSZEg38tNzUwdDC/gPqx5HkNWJ8eZabkDniPk0GxNdAGToUpFFwjWaKEPHTY6bGv9UTDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d3bc919c7a9643bd40b10daafe89a564a9b913aba3d7e41b3da527fe9a66e03b","last_reissued_at":"2026-05-18T02:04:48.487879Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:48.487879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Entropy Production during Asymptotically Safe Inflation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alfio Bonanno, Martin Reuter","submitted_at":"2010-11-11T23:24:28Z","abstract_excerpt":"The Asymptotic Safety scenario predicts that the deep ultraviolet of Quantum Einstein Gravity is governed by a nontrivial renormalization group fixed point. Analyzing its implications for cosmology using renormalization group improved Einstein equations we find that it can give rise to a phase of inflationary expansion in the early Universe. Inflation is a pure quantum effect here and requires no inflaton field. It is driven by the cosmological constant and ends automatically when the renormalization group evolution has reduced the vacuum energy to the level of the matter energy density. The q"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.2794","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":"1011.2794","created_at":"2026-05-18T02:04:48.487995+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.2794v1","created_at":"2026-05-18T02:04:48.487995+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.2794","created_at":"2026-05-18T02:04:48.487995+00:00"},{"alias_kind":"pith_short_12","alias_value":"2O6JDHD2SZB3","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"2O6JDHD2SZB32QFR","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"2O6JDHD2","created_at":"2026-05-18T12:26:03.138858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2205.07787","citing_title":"Horizon-scale tests of gravity theories and fundamental physics from the Event Horizon Telescope image of Sagittarius A$^*$","ref_index":73,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS","json":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS.json","graph_json":"https://pith.science/api/pith-number/2O6JDHD2SZB32QFRBWVP5CNFMS/graph.json","events_json":"https://pith.science/api/pith-number/2O6JDHD2SZB32QFRBWVP5CNFMS/events.json","paper":"https://pith.science/paper/2O6JDHD2"},"agent_actions":{"view_html":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS","download_json":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS.json","view_paper":"https://pith.science/paper/2O6JDHD2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.2794&json=true","fetch_graph":"https://pith.science/api/pith-number/2O6JDHD2SZB32QFRBWVP5CNFMS/graph.json","fetch_events":"https://pith.science/api/pith-number/2O6JDHD2SZB32QFRBWVP5CNFMS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS/action/storage_attestation","attest_author":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS/action/author_attestation","sign_citation":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS/action/citation_signature","submit_replication":"https://pith.science/pith/2O6JDHD2SZB32QFRBWVP5CNFMS/action/replication_record"}},"created_at":"2026-05-18T02:04:48.487995+00:00","updated_at":"2026-05-18T02:04:48.487995+00:00"}