{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:2QQD4VKJ5ESVJDA7XSYVSPXKWI","short_pith_number":"pith:2QQD4VKJ","schema_version":"1.0","canonical_sha256":"d4203e5549e925548c1fbcb1593eeab2130bda5bbb906c57d93dc41f330c1c86","source":{"kind":"arxiv","id":"hep-ph/9508352","version":2},"attestation_state":"computed","paper":{"title":"Nonperturbative Condensates in the Electroweak Phase-Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bastian Bergerhoff, Christof Wetterich","submitted_at":"1995-08-23T12:12:39Z","abstract_excerpt":"We discuss the electroweak phase-transition in the early universe, using non-perturbative flow equations for a computation of the free energy. For a scalar mass above $\\sim 70$ GeV, high-temperature perturbation theory cannot describe this transition reliably. This is due to the dominance of three-dimensional physics at high temperatures which implies that the effective gauge coupling grows strong in the symmetric phase. We give an order of magnitude-estimate of nonperturbative effects in reasonable agreement with recent results from electroweak lattice simulations.\n (Talk given by C. Wetteric"},"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":"hep-ph/9508352","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1995-08-23T12:12:39Z","cross_cats_sorted":[],"title_canon_sha256":"9a2db0a9eaff5786ffc8356b003a64d8f03d0edfd26ee8be7dd317d54bf4f67e","abstract_canon_sha256":"9c3d85cc875f91f2d236e90e7e35cf59128c7631e982294616d347421d155520"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:30.037192Z","signature_b64":"4LHJGkx0r4XqwLe+B+PksEyynCkTuHja+bCq9QedUaR1wYDdH6jtl+iKpWy+O5BrkYWf2RPbd0KYuT2AW+uQAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4203e5549e925548c1fbcb1593eeab2130bda5bbb906c57d93dc41f330c1c86","last_reissued_at":"2026-05-18T01:06:30.036576Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:30.036576Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonperturbative Condensates in the Electroweak Phase-Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bastian Bergerhoff, Christof Wetterich","submitted_at":"1995-08-23T12:12:39Z","abstract_excerpt":"We discuss the electroweak phase-transition in the early universe, using non-perturbative flow equations for a computation of the free energy. For a scalar mass above $\\sim 70$ GeV, high-temperature perturbation theory cannot describe this transition reliably. This is due to the dominance of three-dimensional physics at high temperatures which implies that the effective gauge coupling grows strong in the symmetric phase. We give an order of magnitude-estimate of nonperturbative effects in reasonable agreement with recent results from electroweak lattice simulations.\n (Talk given by C. Wetteric"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9508352","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":"hep-ph/9508352","created_at":"2026-05-18T01:06:30.036680+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9508352v2","created_at":"2026-05-18T01:06:30.036680+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9508352","created_at":"2026-05-18T01:06:30.036680+00:00"},{"alias_kind":"pith_short_12","alias_value":"2QQD4VKJ5ESV","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"2QQD4VKJ5ESVJDA7","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"2QQD4VKJ","created_at":"2026-05-18T12:25:47.102015+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/2QQD4VKJ5ESVJDA7XSYVSPXKWI","json":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI.json","graph_json":"https://pith.science/api/pith-number/2QQD4VKJ5ESVJDA7XSYVSPXKWI/graph.json","events_json":"https://pith.science/api/pith-number/2QQD4VKJ5ESVJDA7XSYVSPXKWI/events.json","paper":"https://pith.science/paper/2QQD4VKJ"},"agent_actions":{"view_html":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI","download_json":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI.json","view_paper":"https://pith.science/paper/2QQD4VKJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9508352&json=true","fetch_graph":"https://pith.science/api/pith-number/2QQD4VKJ5ESVJDA7XSYVSPXKWI/graph.json","fetch_events":"https://pith.science/api/pith-number/2QQD4VKJ5ESVJDA7XSYVSPXKWI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI/action/storage_attestation","attest_author":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI/action/author_attestation","sign_citation":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI/action/citation_signature","submit_replication":"https://pith.science/pith/2QQD4VKJ5ESVJDA7XSYVSPXKWI/action/replication_record"}},"created_at":"2026-05-18T01:06:30.036680+00:00","updated_at":"2026-05-18T01:06:30.036680+00:00"}