{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:LXJ3KDHBD3WQ77CYWC72XFPDUU","short_pith_number":"pith:LXJ3KDHB","schema_version":"1.0","canonical_sha256":"5dd3b50ce11eed0ffc58b0bfab95e3a51150668c1f2b7f45d596647b521a5f4d","source":{"kind":"arxiv","id":"1204.5464","version":2},"attestation_state":"computed","paper":{"title":"Phase Transitions and Gauge Artifacts in an Abelian Higgs Plus Singlet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Carroll L. Wainwright, Michael J. Ramsey-Musolf, Stefano Profumo","submitted_at":"2012-04-24T19:26:46Z","abstract_excerpt":"While the finite-temperature effective potential in a gauge theory is a gauge-dependent quantity, in several instances a first-order phase transition can be triggered by gauge-independent terms. A particularly interesting case occurs when the potential barrier separating the broken and symmetric vacua of a spontaneously broken symmetry is produced by tree-level terms in the potential. Here, we study this scenario in a simple Abelian Higgs model, for which the gauge-invariant potential is known, augmented with a singlet real scalar. We analyze the possible symmetry breaking patterns in the mode"},"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":"1204.5464","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-04-24T19:26:46Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"bb22423477533071145e50d945a7730a61251a6be4c08826a4bf6157fb6ccb90","abstract_canon_sha256":"9b3b09ee9621620955b2bef6e812446f8bc08f8c33d40340336414de81e15033"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:41.866613Z","signature_b64":"+MqBCp2iX4oi6V7wANE3GgWMRIcYUCBzVMQf/gTEUhNAHmnlhzRmST3AgbwVf7XdV6sHQpXnyB9RNfSz/UGCAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5dd3b50ce11eed0ffc58b0bfab95e3a51150668c1f2b7f45d596647b521a5f4d","last_reissued_at":"2026-05-18T03:22:41.865999Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:41.865999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase Transitions and Gauge Artifacts in an Abelian Higgs Plus Singlet Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"Carroll L. Wainwright, Michael J. Ramsey-Musolf, Stefano Profumo","submitted_at":"2012-04-24T19:26:46Z","abstract_excerpt":"While the finite-temperature effective potential in a gauge theory is a gauge-dependent quantity, in several instances a first-order phase transition can be triggered by gauge-independent terms. A particularly interesting case occurs when the potential barrier separating the broken and symmetric vacua of a spontaneously broken symmetry is produced by tree-level terms in the potential. Here, we study this scenario in a simple Abelian Higgs model, for which the gauge-invariant potential is known, augmented with a singlet real scalar. We analyze the possible symmetry breaking patterns in the mode"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.5464","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":"1204.5464","created_at":"2026-05-18T03:22:41.866110+00:00"},{"alias_kind":"arxiv_version","alias_value":"1204.5464v2","created_at":"2026-05-18T03:22:41.866110+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.5464","created_at":"2026-05-18T03:22:41.866110+00:00"},{"alias_kind":"pith_short_12","alias_value":"LXJ3KDHBD3WQ","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"LXJ3KDHBD3WQ77CY","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"LXJ3KDHB","created_at":"2026-05-18T12:27:14.488303+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/LXJ3KDHBD3WQ77CYWC72XFPDUU","json":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU.json","graph_json":"https://pith.science/api/pith-number/LXJ3KDHBD3WQ77CYWC72XFPDUU/graph.json","events_json":"https://pith.science/api/pith-number/LXJ3KDHBD3WQ77CYWC72XFPDUU/events.json","paper":"https://pith.science/paper/LXJ3KDHB"},"agent_actions":{"view_html":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU","download_json":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU.json","view_paper":"https://pith.science/paper/LXJ3KDHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1204.5464&json=true","fetch_graph":"https://pith.science/api/pith-number/LXJ3KDHBD3WQ77CYWC72XFPDUU/graph.json","fetch_events":"https://pith.science/api/pith-number/LXJ3KDHBD3WQ77CYWC72XFPDUU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU/action/storage_attestation","attest_author":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU/action/author_attestation","sign_citation":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU/action/citation_signature","submit_replication":"https://pith.science/pith/LXJ3KDHBD3WQ77CYWC72XFPDUU/action/replication_record"}},"created_at":"2026-05-18T03:22:41.866110+00:00","updated_at":"2026-05-18T03:22:41.866110+00:00"}