{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:QB4VAOHXUAVZYVLV7NK5VILT5R","short_pith_number":"pith:QB4VAOHX","schema_version":"1.0","canonical_sha256":"80795038f7a02b9c5575fb55daa173ec4b29bb0914979d4a780831719c8050f0","source":{"kind":"arxiv","id":"1603.04439","version":2},"attestation_state":"computed","paper":{"title":"SaxiGUTs and their Predictions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Francesco D'Eramo, Lawrence J. Hall, Raymond T. Co","submitted_at":"2016-03-14T20:00:01Z","abstract_excerpt":"We introduce a class of unified supersymmetric axion theories with unified and PQ symmetries broken by the same set of fields at a scale $\\sim 2\\times 10^{16}$ GeV. A typical domain wall number of order 30 leads to an axion decay constant $f_a$ of order $10^{15}$ GeV. Inflation generates a large saxion condensate giving a reheat temperature $T_R$ below the QCD scale for supersymmetry breaking of order $1-10$ TeV. Axion field oscillations commence in the saxion matter-dominated era near the QCD scale, and recent lattice computations of the temperature dependence of the axion mass in this era al"},"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":"1603.04439","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-14T20:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"72913a3e11679f052964314803c4b39320ab5defb4d14bf08505e457cfd2d49e","abstract_canon_sha256":"3dfce786771e84471340ea42432e392089d800503597d114bb4823016734b2ad"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:01:57.980452Z","signature_b64":"7rdDH0vSvQcCHhSpoT68NpD0O9kfqan4nvi2NSRwgcgPPiZlCgyWCK+Er4RS2H/y7/nLFLjIO/avwhjIUQzJCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"80795038f7a02b9c5575fb55daa173ec4b29bb0914979d4a780831719c8050f0","last_reissued_at":"2026-05-18T01:01:57.979767Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:01:57.979767Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SaxiGUTs and their Predictions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Francesco D'Eramo, Lawrence J. Hall, Raymond T. Co","submitted_at":"2016-03-14T20:00:01Z","abstract_excerpt":"We introduce a class of unified supersymmetric axion theories with unified and PQ symmetries broken by the same set of fields at a scale $\\sim 2\\times 10^{16}$ GeV. A typical domain wall number of order 30 leads to an axion decay constant $f_a$ of order $10^{15}$ GeV. Inflation generates a large saxion condensate giving a reheat temperature $T_R$ below the QCD scale for supersymmetry breaking of order $1-10$ TeV. Axion field oscillations commence in the saxion matter-dominated era near the QCD scale, and recent lattice computations of the temperature dependence of the axion mass in this era al"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.04439","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":"1603.04439","created_at":"2026-05-18T01:01:57.979905+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.04439v2","created_at":"2026-05-18T01:01:57.979905+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.04439","created_at":"2026-05-18T01:01:57.979905+00:00"},{"alias_kind":"pith_short_12","alias_value":"QB4VAOHXUAVZ","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"QB4VAOHXUAVZYVLV","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"QB4VAOHX","created_at":"2026-05-18T12:30:39.010887+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.01772","citing_title":"The QCD Axion and Unification","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R","json":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R.json","graph_json":"https://pith.science/api/pith-number/QB4VAOHXUAVZYVLV7NK5VILT5R/graph.json","events_json":"https://pith.science/api/pith-number/QB4VAOHXUAVZYVLV7NK5VILT5R/events.json","paper":"https://pith.science/paper/QB4VAOHX"},"agent_actions":{"view_html":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R","download_json":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R.json","view_paper":"https://pith.science/paper/QB4VAOHX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.04439&json=true","fetch_graph":"https://pith.science/api/pith-number/QB4VAOHXUAVZYVLV7NK5VILT5R/graph.json","fetch_events":"https://pith.science/api/pith-number/QB4VAOHXUAVZYVLV7NK5VILT5R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R/action/storage_attestation","attest_author":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R/action/author_attestation","sign_citation":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R/action/citation_signature","submit_replication":"https://pith.science/pith/QB4VAOHXUAVZYVLV7NK5VILT5R/action/replication_record"}},"created_at":"2026-05-18T01:01:57.979905+00:00","updated_at":"2026-05-18T01:01:57.979905+00:00"}