{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:NJVI3BCTNHZQYJQ3KTKIN35J4D","short_pith_number":"pith:NJVI3BCT","schema_version":"1.0","canonical_sha256":"6a6a8d845369f30c261b54d486efa9e0c81727d65c1d6e64177ac0e2fef0b345","source":{"kind":"arxiv","id":"2012.08428","version":2},"attestation_state":"computed","paper":{"title":"The free and safe fate of symmetry non-restoration","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Adrian Lugo, Borut Bajc, Francesco Sannino","submitted_at":"2020-12-15T17:10:09Z","abstract_excerpt":"We investigate the high temperature fate of four dimensional gauge-Yukawa theories featuring short distance conformality of either interacting or non-interacting nature. The latter is known as complete asymptotic freedom and, as templates, we consider non-abelian gauge theories featuring either two singlet scalars coupled to gauged fermions via Yukawa interactions or two gauged scalars with(out) fermions. For theories with interacting fixed points at short distance, known as asymptotically safe, we consider two calculable examples.\n  Exploring the landscape of safe and free theories above we d"},"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":"2012.08428","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2020-12-15T17:10:09Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"6e3119842cd355ce2213bab47dace6d8ce362a88d4a9ea41062aa2645d30a3ec","abstract_canon_sha256":"dfe28383d6e94f850aad65c2cc7e8510543e64c507230ea635510a6b85449041"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:43:13.815557Z","signature_b64":"0QoIdQ0ZTNz40jeMV5WTrN1hjjFhtKvEkVi2w0qhDBNfHEd/KW87+WDzX5ZHhGMwZA3zufersMJV8RmhvHMZCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a6a8d845369f30c261b54d486efa9e0c81727d65c1d6e64177ac0e2fef0b345","last_reissued_at":"2026-07-05T02:43:13.815061Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:43:13.815061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The free and safe fate of symmetry non-restoration","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Adrian Lugo, Borut Bajc, Francesco Sannino","submitted_at":"2020-12-15T17:10:09Z","abstract_excerpt":"We investigate the high temperature fate of four dimensional gauge-Yukawa theories featuring short distance conformality of either interacting or non-interacting nature. The latter is known as complete asymptotic freedom and, as templates, we consider non-abelian gauge theories featuring either two singlet scalars coupled to gauged fermions via Yukawa interactions or two gauged scalars with(out) fermions. For theories with interacting fixed points at short distance, known as asymptotically safe, we consider two calculable examples.\n  Exploring the landscape of safe and free theories above we d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.08428","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/2012.08428/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":"2012.08428","created_at":"2026-07-05T02:43:13.815121+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.08428v2","created_at":"2026-07-05T02:43:13.815121+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.08428","created_at":"2026-07-05T02:43:13.815121+00:00"},{"alias_kind":"pith_short_12","alias_value":"NJVI3BCTNHZQ","created_at":"2026-07-05T02:43:13.815121+00:00"},{"alias_kind":"pith_short_16","alias_value":"NJVI3BCTNHZQYJQ3","created_at":"2026-07-05T02:43:13.815121+00:00"},{"alias_kind":"pith_short_8","alias_value":"NJVI3BCT","created_at":"2026-07-05T02:43:13.815121+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.18694","citing_title":"Exploring Entropic Orders: High Temperature Continuous Symmetry Breaking, Chiral Topological States and Local Commuting Projector Models","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D","json":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D.json","graph_json":"https://pith.science/api/pith-number/NJVI3BCTNHZQYJQ3KTKIN35J4D/graph.json","events_json":"https://pith.science/api/pith-number/NJVI3BCTNHZQYJQ3KTKIN35J4D/events.json","paper":"https://pith.science/paper/NJVI3BCT"},"agent_actions":{"view_html":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D","download_json":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D.json","view_paper":"https://pith.science/paper/NJVI3BCT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.08428&json=true","fetch_graph":"https://pith.science/api/pith-number/NJVI3BCTNHZQYJQ3KTKIN35J4D/graph.json","fetch_events":"https://pith.science/api/pith-number/NJVI3BCTNHZQYJQ3KTKIN35J4D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D/action/storage_attestation","attest_author":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D/action/author_attestation","sign_citation":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D/action/citation_signature","submit_replication":"https://pith.science/pith/NJVI3BCTNHZQYJQ3KTKIN35J4D/action/replication_record"}},"created_at":"2026-07-05T02:43:13.815121+00:00","updated_at":"2026-07-05T02:43:13.815121+00:00"}