{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:V3DMEH7HSLCUC6XIY4TQ7ECS6V","short_pith_number":"pith:V3DMEH7H","schema_version":"1.0","canonical_sha256":"aec6c21fe792c5417ae8c7270f9052f54c48b01f7c850d4854cdb5e45f5eace3","source":{"kind":"arxiv","id":"2506.01585","version":1},"attestation_state":"computed","paper":{"title":"An Effective Sphaleron Awakens","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael J. Ramsey-Musolf, Tuomas V. I. Tenkanen, Xu-Xiang Li, Yanda Wu","submitted_at":"2025-06-02T12:18:06Z","abstract_excerpt":"Using thermal effective field theory, we present a self-consistent perturbative formulation of the Higgs phase sphaleron rate after a radiatively-induced first-order phase transition. This gauge-invariant formulation is based on dimensionally reduced effective field theory (3D EFT) at high temperatures and paves a way for including higher order corrections within the 3D EFT perturbation theory without double counting. Concretely, we compute the Higgs phase sphaleron rate in a semi-classical approximation within the two-loop resummed 3D EFT. We find compact results for the sphaleron rate and th"},"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":"2506.01585","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-06-02T12:18:06Z","cross_cats_sorted":[],"title_canon_sha256":"866dafe0cf12901659c9cb6c7a9822539a5b7e5ec964025988c2fb4205316a6b","abstract_canon_sha256":"e75bf466826807174f6bb90b6954700f85b76bb28a5cb336f97d7d0159368a28"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:14:16.212874Z","signature_b64":"XYpJVY0DECNr+x1gBscG7vb01tm7WgwCwjYblbeUh+BxZfbJex46KWgYh6cH2bmYcwXwq3gTmI7u4SsNOHyzBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aec6c21fe792c5417ae8c7270f9052f54c48b01f7c850d4854cdb5e45f5eace3","last_reissued_at":"2026-07-05T11:14:16.212458Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:14:16.212458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Effective Sphaleron Awakens","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael J. Ramsey-Musolf, Tuomas V. I. Tenkanen, Xu-Xiang Li, Yanda Wu","submitted_at":"2025-06-02T12:18:06Z","abstract_excerpt":"Using thermal effective field theory, we present a self-consistent perturbative formulation of the Higgs phase sphaleron rate after a radiatively-induced first-order phase transition. This gauge-invariant formulation is based on dimensionally reduced effective field theory (3D EFT) at high temperatures and paves a way for including higher order corrections within the 3D EFT perturbation theory without double counting. Concretely, we compute the Higgs phase sphaleron rate in a semi-classical approximation within the two-loop resummed 3D EFT. We find compact results for the sphaleron rate and th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.01585","kind":"arxiv","version":1},"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/2506.01585/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":"2506.01585","created_at":"2026-07-05T11:14:16.212514+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.01585v1","created_at":"2026-07-05T11:14:16.212514+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.01585","created_at":"2026-07-05T11:14:16.212514+00:00"},{"alias_kind":"pith_short_12","alias_value":"V3DMEH7HSLCU","created_at":"2026-07-05T11:14:16.212514+00:00"},{"alias_kind":"pith_short_16","alias_value":"V3DMEH7HSLCUC6XI","created_at":"2026-07-05T11:14:16.212514+00:00"},{"alias_kind":"pith_short_8","alias_value":"V3DMEH7H","created_at":"2026-07-05T11:14:16.212514+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.12533","citing_title":"Constraining the real scalar singlet extension of the SM","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21972","citing_title":"Matchotter: An Automated Tool for Dimensional Reduction at Finite Temperature","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06775","citing_title":"SIRENA -- Sum-Integral REductioN Algorithm","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16603","citing_title":"Baryon Asymmetry from Electroweak-Symmetric Domain Walls","ref_index":34,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V","json":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V.json","graph_json":"https://pith.science/api/pith-number/V3DMEH7HSLCUC6XIY4TQ7ECS6V/graph.json","events_json":"https://pith.science/api/pith-number/V3DMEH7HSLCUC6XIY4TQ7ECS6V/events.json","paper":"https://pith.science/paper/V3DMEH7H"},"agent_actions":{"view_html":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V","download_json":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V.json","view_paper":"https://pith.science/paper/V3DMEH7H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.01585&json=true","fetch_graph":"https://pith.science/api/pith-number/V3DMEH7HSLCUC6XIY4TQ7ECS6V/graph.json","fetch_events":"https://pith.science/api/pith-number/V3DMEH7HSLCUC6XIY4TQ7ECS6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V/action/storage_attestation","attest_author":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V/action/author_attestation","sign_citation":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V/action/citation_signature","submit_replication":"https://pith.science/pith/V3DMEH7HSLCUC6XIY4TQ7ECS6V/action/replication_record"}},"created_at":"2026-07-05T11:14:16.212514+00:00","updated_at":"2026-07-05T11:14:16.212514+00:00"}