{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:C7UCAUEPCFD2XYTEWKRPWSDMT2","short_pith_number":"pith:C7UCAUEP","schema_version":"1.0","canonical_sha256":"17e820508f1147abe264b2a2fb486c9ea3e43cc523ecbd9621f05085644f3abf","source":{"kind":"arxiv","id":"1101.4665","version":2},"attestation_state":"computed","paper":{"title":"Baryon Washout, Electroweak Phase Transition, and Perturbation Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiren H. Patel, Michael J. Ramsey-Musolf","submitted_at":"2011-01-24T21:27:51Z","abstract_excerpt":"We analyze the conventional perturbative treatment of sphaleron-induced baryon number washout relevant for electroweak baryogenesis and show that it is not gauge-independent due to the failure of consistently implementing the Nielsen identities order-by-order in perturbation theory. We provide a gauge-independent criterion for baryon number preservation in place of the conventional (gauge-dependent) criterion needed for successful electroweak baryogenesis. We also review the arguments leading to the preservation criterion and analyze several sources of theoretical uncertainties in obtaining a "},"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":"1101.4665","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-01-24T21:27:51Z","cross_cats_sorted":[],"title_canon_sha256":"12eb35deaa429de616cc5e36129642f3c21b9e79236939a6067eda14f06eaa46","abstract_canon_sha256":"fdac97827a4c08f232e4779eeef6d935cb3d037dbc9e376a57e640feff7ee2e9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:48.000579Z","signature_b64":"Zj8l4ZxMlh0bRX0SW79pSRaniyQh7BlZC5T9i22HZeFNkVv9Sf4iY4GCcKa18Y8FDoYE56qinWT6Slkxjl2YDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17e820508f1147abe264b2a2fb486c9ea3e43cc523ecbd9621f05085644f3abf","last_reissued_at":"2026-05-18T01:25:48.000001Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:48.000001Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baryon Washout, Electroweak Phase Transition, and Perturbation Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hiren H. Patel, Michael J. Ramsey-Musolf","submitted_at":"2011-01-24T21:27:51Z","abstract_excerpt":"We analyze the conventional perturbative treatment of sphaleron-induced baryon number washout relevant for electroweak baryogenesis and show that it is not gauge-independent due to the failure of consistently implementing the Nielsen identities order-by-order in perturbation theory. We provide a gauge-independent criterion for baryon number preservation in place of the conventional (gauge-dependent) criterion needed for successful electroweak baryogenesis. We also review the arguments leading to the preservation criterion and analyze several sources of theoretical uncertainties in obtaining a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.4665","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":"1101.4665","created_at":"2026-05-18T01:25:48.000062+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.4665v2","created_at":"2026-05-18T01:25:48.000062+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.4665","created_at":"2026-05-18T01:25:48.000062+00:00"},{"alias_kind":"pith_short_12","alias_value":"C7UCAUEPCFD2","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"C7UCAUEPCFD2XYTE","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"C7UCAUEP","created_at":"2026-05-18T12:26:26.731475+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2404.19197","citing_title":"Does the Electron EDM Preclude Electroweak Baryogenesis ?","ref_index":61,"is_internal_anchor":true},{"citing_arxiv_id":"2511.00996","citing_title":"Measuring gravitational wave spectrum from electroweak phase transition and Higgs self-couplings","ref_index":64,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15259","citing_title":"TransitionListener v2.0 -- Robust gravitational wave predictions for cosmological phase transitions","ref_index":154,"is_internal_anchor":true},{"citing_arxiv_id":"2510.13770","citing_title":"Gauge-independent Gravitational Waves from Cogenesis in a $B-L$ Conserving Universe","ref_index":102,"is_internal_anchor":true},{"citing_arxiv_id":"2603.18583","citing_title":"Electroweak phase transitions in a $U(1)_D$ extension of the standard model with dimension-six operators: Gravitational waves and LHC signatures","ref_index":52,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2","json":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2.json","graph_json":"https://pith.science/api/pith-number/C7UCAUEPCFD2XYTEWKRPWSDMT2/graph.json","events_json":"https://pith.science/api/pith-number/C7UCAUEPCFD2XYTEWKRPWSDMT2/events.json","paper":"https://pith.science/paper/C7UCAUEP"},"agent_actions":{"view_html":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2","download_json":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2.json","view_paper":"https://pith.science/paper/C7UCAUEP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.4665&json=true","fetch_graph":"https://pith.science/api/pith-number/C7UCAUEPCFD2XYTEWKRPWSDMT2/graph.json","fetch_events":"https://pith.science/api/pith-number/C7UCAUEPCFD2XYTEWKRPWSDMT2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2/action/storage_attestation","attest_author":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2/action/author_attestation","sign_citation":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2/action/citation_signature","submit_replication":"https://pith.science/pith/C7UCAUEPCFD2XYTEWKRPWSDMT2/action/replication_record"}},"created_at":"2026-05-18T01:25:48.000062+00:00","updated_at":"2026-05-18T01:25:48.000062+00:00"}