{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:QCRJ3WGKR4JX2AUCDETYLLVBPH","short_pith_number":"pith:QCRJ3WGK","schema_version":"1.0","canonical_sha256":"80a29dd8ca8f137d0282192785aea179e47717e80320c1340950f4e14ed64175","source":{"kind":"arxiv","id":"hep-ph/9806453","version":2},"attestation_state":"computed","paper":{"title":"A Consistent Calculation of Bubble-Nucleation Rates","license":"","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"A. Strumia, N. Tetradis","submitted_at":"1998-06-23T11:36:10Z","abstract_excerpt":"We present a consistent picture of tunnelling in field theory. Our results apply both to high-temperature field theories in four dimensions and to zero-temperature three-dimensional ones. Our approach is based on the notion of a coarse-grained potential U_k that incorporates the effect of fluctuations with characteristic momenta above a given scale k. U_k is non-convex and becomes equal to the convex effective potential for k --> 0. We demonstrate that a consistent calculation of the nucleation rate must be performed at non-zero values of k, larger than the typical scale of the saddle-point co"},"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/9806453","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-06-23T11:36:10Z","cross_cats_sorted":["cond-mat.stat-mech","hep-lat","hep-th"],"title_canon_sha256":"e432fea9b3443d162fe564d8c70ef246cff23494d3d8cf648cd0f7e4e4261357","abstract_canon_sha256":"149edf14fab40c7bd5adf17e07c71c4ffab93728f2f0e0fe5b1ca9bc1aad531d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:10.342693Z","signature_b64":"qm2e68YFvYordH/CZLsPttx1cNlalrWBeLge4LzzhDOMgul1TnXgZCS6t4SlLWbXUq8GOWvFQxH28WQ7Ze3dCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"80a29dd8ca8f137d0282192785aea179e47717e80320c1340950f4e14ed64175","last_reissued_at":"2026-07-04T15:54:10.342263Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:10.342263Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Consistent Calculation of Bubble-Nucleation Rates","license":"","headline":"","cross_cats":["cond-mat.stat-mech","hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"A. Strumia, N. Tetradis","submitted_at":"1998-06-23T11:36:10Z","abstract_excerpt":"We present a consistent picture of tunnelling in field theory. Our results apply both to high-temperature field theories in four dimensions and to zero-temperature three-dimensional ones. Our approach is based on the notion of a coarse-grained potential U_k that incorporates the effect of fluctuations with characteristic momenta above a given scale k. U_k is non-convex and becomes equal to the convex effective potential for k --> 0. We demonstrate that a consistent calculation of the nucleation rate must be performed at non-zero values of k, larger than the typical scale of the saddle-point co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9806453","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/hep-ph/9806453/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":"hep-ph/9806453","created_at":"2026-07-04T15:54:10.342323+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9806453v2","created_at":"2026-07-04T15:54:10.342323+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9806453","created_at":"2026-07-04T15:54:10.342323+00:00"},{"alias_kind":"pith_short_12","alias_value":"QCRJ3WGKR4JX","created_at":"2026-07-04T15:54:10.342323+00:00"},{"alias_kind":"pith_short_16","alias_value":"QCRJ3WGKR4JX2AUC","created_at":"2026-07-04T15:54:10.342323+00:00"},{"alias_kind":"pith_short_8","alias_value":"QCRJ3WGK","created_at":"2026-07-04T15:54:10.342323+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.11622","citing_title":"Testing the effective action approach to bubble nucleation in holography","ref_index":29,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH","json":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH.json","graph_json":"https://pith.science/api/pith-number/QCRJ3WGKR4JX2AUCDETYLLVBPH/graph.json","events_json":"https://pith.science/api/pith-number/QCRJ3WGKR4JX2AUCDETYLLVBPH/events.json","paper":"https://pith.science/paper/QCRJ3WGK"},"agent_actions":{"view_html":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH","download_json":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH.json","view_paper":"https://pith.science/paper/QCRJ3WGK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9806453&json=true","fetch_graph":"https://pith.science/api/pith-number/QCRJ3WGKR4JX2AUCDETYLLVBPH/graph.json","fetch_events":"https://pith.science/api/pith-number/QCRJ3WGKR4JX2AUCDETYLLVBPH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH/action/storage_attestation","attest_author":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH/action/author_attestation","sign_citation":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH/action/citation_signature","submit_replication":"https://pith.science/pith/QCRJ3WGKR4JX2AUCDETYLLVBPH/action/replication_record"}},"created_at":"2026-07-04T15:54:10.342323+00:00","updated_at":"2026-07-04T15:54:10.342323+00:00"}