{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:POKWXVLZ3SAKOT4OIR55347GK2","short_pith_number":"pith:POKWXVLZ","schema_version":"1.0","canonical_sha256":"7b956bd579dc80a74f8e447bddf3e656aa0ad2f1f6d223d9ca3304a3e214d29b","source":{"kind":"arxiv","id":"1405.3652","version":2},"attestation_state":"computed","paper":{"title":"The Powers of Monodromy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph"],"primary_cat":"hep-th","authors_text":"Alexander Westphal, Eva Silverstein, Liam McAllister, Timm Wrase","submitted_at":"2014-05-14T20:00:04Z","abstract_excerpt":"Flux couplings to string theory axions yield super-Planckian field ranges along which the axion potential energy grows. At the same time, other aspects of the physics remain essentially unchanged along these large displacements, respecting a discrete shift symmetry with a sub-Planckian period. After a general overview of this monodromy effect and its application to large-field inflation, we present new classes of specific models of monodromy inflation, with monomial potentials $\\mu^{4-p}\\phi^p$. A key simplification in these models is that the inflaton potential energy plays a leading role in "},"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":"1405.3652","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-05-14T20:00:04Z","cross_cats_sorted":["astro-ph.CO","hep-ph"],"title_canon_sha256":"3603e8ec269abfb2a4d5cb16c68afebabab57de9f771d92366205dfb1cbe9d6b","abstract_canon_sha256":"85762b86b3a3fa520dc9f1b11e3c6ae421798b27c5c383403258b1cc0d33611c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:41.410798Z","signature_b64":"x2VqAmyhYRtwMKq1yWeCACxAqRED9NmwzPYbSzcg39uXdZnr0DMhllNdd6I1OAxxiFaH9lv57tShO1g9mguxDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b956bd579dc80a74f8e447bddf3e656aa0ad2f1f6d223d9ca3304a3e214d29b","last_reissued_at":"2026-05-18T02:41:41.410248Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:41.410248Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Powers of Monodromy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-ph"],"primary_cat":"hep-th","authors_text":"Alexander Westphal, Eva Silverstein, Liam McAllister, Timm Wrase","submitted_at":"2014-05-14T20:00:04Z","abstract_excerpt":"Flux couplings to string theory axions yield super-Planckian field ranges along which the axion potential energy grows. At the same time, other aspects of the physics remain essentially unchanged along these large displacements, respecting a discrete shift symmetry with a sub-Planckian period. After a general overview of this monodromy effect and its application to large-field inflation, we present new classes of specific models of monodromy inflation, with monomial potentials $\\mu^{4-p}\\phi^p$. A key simplification in these models is that the inflaton potential energy plays a leading role in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.3652","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":""},"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":"1405.3652","created_at":"2026-05-18T02:41:41.410331+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.3652v2","created_at":"2026-05-18T02:41:41.410331+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.3652","created_at":"2026-05-18T02:41:41.410331+00:00"},{"alias_kind":"pith_short_12","alias_value":"POKWXVLZ3SAK","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"POKWXVLZ3SAKOT4O","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"POKWXVLZ","created_at":"2026-05-18T12:28:43.426989+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.21092","citing_title":"Audible Axion Magnetogenesis: Linking Intergalactic Magnetic Fields and Gravitational Waves","ref_index":149,"is_internal_anchor":true},{"citing_arxiv_id":"2510.24682","citing_title":"Harrison-Zeldovich attractor: From Planck to ACT results","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2","json":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2.json","graph_json":"https://pith.science/api/pith-number/POKWXVLZ3SAKOT4OIR55347GK2/graph.json","events_json":"https://pith.science/api/pith-number/POKWXVLZ3SAKOT4OIR55347GK2/events.json","paper":"https://pith.science/paper/POKWXVLZ"},"agent_actions":{"view_html":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2","download_json":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2.json","view_paper":"https://pith.science/paper/POKWXVLZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.3652&json=true","fetch_graph":"https://pith.science/api/pith-number/POKWXVLZ3SAKOT4OIR55347GK2/graph.json","fetch_events":"https://pith.science/api/pith-number/POKWXVLZ3SAKOT4OIR55347GK2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2/action/storage_attestation","attest_author":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2/action/author_attestation","sign_citation":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2/action/citation_signature","submit_replication":"https://pith.science/pith/POKWXVLZ3SAKOT4OIR55347GK2/action/replication_record"}},"created_at":"2026-05-18T02:41:41.410331+00:00","updated_at":"2026-05-18T02:41:41.410331+00:00"}