{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:T6SCRVVBVSE52VGP2SLBV62RB3","short_pith_number":"pith:T6SCRVVB","schema_version":"1.0","canonical_sha256":"9fa428d6a1ac89dd54cfd4961afb510eedbbd9053313c6bd615cd39f56cb1563","source":{"kind":"arxiv","id":"2405.08060","version":2},"attestation_state":"computed","paper":{"title":"QCD Axion Strings or Seeds?","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Alberto Mariotti, Simone Blasi","submitted_at":"2024-05-13T18:00:00Z","abstract_excerpt":"We study the impact of QCD axion strings in the cosmological history of electroweak (EW) symmetry breaking, focussing on the minimal KSVZ axion model. We consider the case of the pure SM Higgs potential as well as a simple scenario with a first order EW phase transition. We capture the effect of the Peccei-Quinn (PQ) sector within an effective-theory approach for the Higgs field, where the axion string core and the heavy PQ states are integrated out. The relevant parameters in this effective theory are controlled by the size of the portal coupling between the Higgs and the PQ scalar, and the m"},"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":"2405.08060","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-13T18:00:00Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"c83c1c75f037c96deda875a783c365258a157ef20791a463c69838c12e9b201a","abstract_canon_sha256":"908def47f0723cc655cf440cc674a1a569cddeef61553ea7f6c91f2e537a3872"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:00:36.900983Z","signature_b64":"wNsB/bmm9N7g9mbw0gpyAukLHrQ4IQVsZF05hHSDPV2Si3x8Ywl0EvzoA6KcSzKkg51zqOQEpS7Dm7gD4XZwCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9fa428d6a1ac89dd54cfd4961afb510eedbbd9053313c6bd615cd39f56cb1563","last_reissued_at":"2026-07-05T10:00:36.900575Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:00:36.900575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"QCD Axion Strings or Seeds?","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Alberto Mariotti, Simone Blasi","submitted_at":"2024-05-13T18:00:00Z","abstract_excerpt":"We study the impact of QCD axion strings in the cosmological history of electroweak (EW) symmetry breaking, focussing on the minimal KSVZ axion model. We consider the case of the pure SM Higgs potential as well as a simple scenario with a first order EW phase transition. We capture the effect of the Peccei-Quinn (PQ) sector within an effective-theory approach for the Higgs field, where the axion string core and the heavy PQ states are integrated out. The relevant parameters in this effective theory are controlled by the size of the portal coupling between the Higgs and the PQ scalar, and the m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.08060","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/2405.08060/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":"2405.08060","created_at":"2026-07-05T10:00:36.900630+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.08060v2","created_at":"2026-07-05T10:00:36.900630+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.08060","created_at":"2026-07-05T10:00:36.900630+00:00"},{"alias_kind":"pith_short_12","alias_value":"T6SCRVVBVSE5","created_at":"2026-07-05T10:00:36.900630+00:00"},{"alias_kind":"pith_short_16","alias_value":"T6SCRVVBVSE52VGP","created_at":"2026-07-05T10:00:36.900630+00:00"},{"alias_kind":"pith_short_8","alias_value":"T6SCRVVB","created_at":"2026-07-05T10:00:36.900630+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21653","citing_title":"Globally Charged Vacuum Decay","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2605.31194","citing_title":"Seeded bubble nucleation on the lattice","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3","json":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3.json","graph_json":"https://pith.science/api/pith-number/T6SCRVVBVSE52VGP2SLBV62RB3/graph.json","events_json":"https://pith.science/api/pith-number/T6SCRVVBVSE52VGP2SLBV62RB3/events.json","paper":"https://pith.science/paper/T6SCRVVB"},"agent_actions":{"view_html":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3","download_json":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3.json","view_paper":"https://pith.science/paper/T6SCRVVB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.08060&json=true","fetch_graph":"https://pith.science/api/pith-number/T6SCRVVBVSE52VGP2SLBV62RB3/graph.json","fetch_events":"https://pith.science/api/pith-number/T6SCRVVBVSE52VGP2SLBV62RB3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3/action/storage_attestation","attest_author":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3/action/author_attestation","sign_citation":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3/action/citation_signature","submit_replication":"https://pith.science/pith/T6SCRVVBVSE52VGP2SLBV62RB3/action/replication_record"}},"created_at":"2026-07-05T10:00:36.900630+00:00","updated_at":"2026-07-05T10:00:36.900630+00:00"}