{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:CPJG7NEOAN64F42HXXJ7LGUIDD","short_pith_number":"pith:CPJG7NEO","schema_version":"1.0","canonical_sha256":"13d26fb48e037dc2f347bdd3f59a8818cf2517758bbadbe354db974f296c3b53","source":{"kind":"arxiv","id":"1412.3544","version":1},"attestation_state":"computed","paper":{"title":"Numerical calcultaion of e-fold number from hilltop with two inflatons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Doh Young Mo, Jihn E. Kim","submitted_at":"2014-12-11T05:27:22Z","abstract_excerpt":"We consider a cosmological inflation with two inflatons, $\\phi$ and $X$. The inflation potential is a hilltop form in the $\\phi$ space and $X$ is a sideway down-fall field in the region $\\phi\\ge m$. In this model, we calculate the $e$-fold number numerically starting from the intitial point which is in the vicinity of the hilltop point. Firstly, by varying parameters and initial conditions the inflaton path field $\\varphi$ for the BICEP2 point, $\\varphi_{\\rm BCP2}$, is found to give $ n_s\\simeq 0.96$ and $r\\simeq 0.16$. Next, from the point $\\varphi_{\\rm BCP2}$ to the end of inflation the e-fo"},"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":"1412.3544","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-12-11T05:27:22Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"856ef7b326f67e40362dfd4387531c84480bc998128973b038fbb481b42f1359","abstract_canon_sha256":"6cde75ad75ada056ad60f1aa136962d350d89d5851aaf813b53ad83b12ed1ca4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:31:30.839016Z","signature_b64":"ANiPlKyZPj1oTpEjeNZxaH4+1XXjcTtLaR9+jpKgqiPJjp3BLrPr2ZoPU8qcIuAkr1aKyOqF0e8/jVM/dkSsDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13d26fb48e037dc2f347bdd3f59a8818cf2517758bbadbe354db974f296c3b53","last_reissued_at":"2026-05-18T02:31:30.838632Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:31:30.838632Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Numerical calcultaion of e-fold number from hilltop with two inflatons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Doh Young Mo, Jihn E. Kim","submitted_at":"2014-12-11T05:27:22Z","abstract_excerpt":"We consider a cosmological inflation with two inflatons, $\\phi$ and $X$. The inflation potential is a hilltop form in the $\\phi$ space and $X$ is a sideway down-fall field in the region $\\phi\\ge m$. In this model, we calculate the $e$-fold number numerically starting from the intitial point which is in the vicinity of the hilltop point. Firstly, by varying parameters and initial conditions the inflaton path field $\\varphi$ for the BICEP2 point, $\\varphi_{\\rm BCP2}$, is found to give $ n_s\\simeq 0.96$ and $r\\simeq 0.16$. Next, from the point $\\varphi_{\\rm BCP2}$ to the end of inflation the e-fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3544","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":"1412.3544","created_at":"2026-05-18T02:31:30.838689+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.3544v1","created_at":"2026-05-18T02:31:30.838689+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3544","created_at":"2026-05-18T02:31:30.838689+00:00"},{"alias_kind":"pith_short_12","alias_value":"CPJG7NEOAN64","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"CPJG7NEOAN64F42H","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"CPJG7NEO","created_at":"2026-05-18T12:28:22.404517+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/CPJG7NEOAN64F42HXXJ7LGUIDD","json":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD.json","graph_json":"https://pith.science/api/pith-number/CPJG7NEOAN64F42HXXJ7LGUIDD/graph.json","events_json":"https://pith.science/api/pith-number/CPJG7NEOAN64F42HXXJ7LGUIDD/events.json","paper":"https://pith.science/paper/CPJG7NEO"},"agent_actions":{"view_html":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD","download_json":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD.json","view_paper":"https://pith.science/paper/CPJG7NEO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.3544&json=true","fetch_graph":"https://pith.science/api/pith-number/CPJG7NEOAN64F42HXXJ7LGUIDD/graph.json","fetch_events":"https://pith.science/api/pith-number/CPJG7NEOAN64F42HXXJ7LGUIDD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD/action/storage_attestation","attest_author":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD/action/author_attestation","sign_citation":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD/action/citation_signature","submit_replication":"https://pith.science/pith/CPJG7NEOAN64F42HXXJ7LGUIDD/action/replication_record"}},"created_at":"2026-05-18T02:31:30.838689+00:00","updated_at":"2026-05-18T02:31:30.838689+00:00"}