{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1992:5MURFZCA54KPLNYK27AAMCKP67","short_pith_number":"pith:5MURFZCA","schema_version":"1.0","canonical_sha256":"eb2912e440ef14f5b70ad7c006094ff7d56feec99e4f993636344e0a7f487edf","source":{"kind":"arxiv","id":"hep-ph/9205205","version":1},"attestation_state":"computed","paper":{"title":"Field Theory Without Feynman Diagrams: One-Loop Effective Actions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matthew J. Strassler","submitted_at":"1992-05-05T18:25:00Z","abstract_excerpt":"In this paper the connection between standard perturbation theory techniques and the new Bern-Kosower calculational rules for gauge theory is clarified. For one-loop effective actions of scalars, Dirac spinors, and vector bosons in a background gauge field, Bern-Kosower-type rules are derived without the use of either string theory or Feynman diagrams. The effective action is written as a one-dimensional path integral, which can be calculated to any order in the gauge coupling; evaluation leads to Feynman parameter integrals directly, bypassing the usual algebra required from Feynman diagrams,"},"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/9205205","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1992-05-05T18:25:00Z","cross_cats_sorted":[],"title_canon_sha256":"9b7d86a0fd918731c63e49dfdfd1934ca59ac41a16a4035db4d4e1ddd9c0f773","abstract_canon_sha256":"c70686112f7d52436d068b0351d56a102209a8bc7b258a542336e7d530649dfe"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:45:45.380944Z","signature_b64":"uiuEThUaUi/7HpCJHUIcehvckxV9EGYhR89mk4ijoI3MCRkNy8d1xc7bpTG0BZAhAowLkYYc9lOVGd/+hjw4BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb2912e440ef14f5b70ad7c006094ff7d56feec99e4f993636344e0a7f487edf","last_reissued_at":"2026-07-04T15:45:45.380491Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:45:45.380491Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Field Theory Without Feynman Diagrams: One-Loop Effective Actions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matthew J. Strassler","submitted_at":"1992-05-05T18:25:00Z","abstract_excerpt":"In this paper the connection between standard perturbation theory techniques and the new Bern-Kosower calculational rules for gauge theory is clarified. For one-loop effective actions of scalars, Dirac spinors, and vector bosons in a background gauge field, Bern-Kosower-type rules are derived without the use of either string theory or Feynman diagrams. The effective action is written as a one-dimensional path integral, which can be calculated to any order in the gauge coupling; evaluation leads to Feynman parameter integrals directly, bypassing the usual algebra required from Feynman diagrams,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9205205","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/hep-ph/9205205/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/9205205","created_at":"2026-07-04T15:45:45.380557+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9205205v1","created_at":"2026-07-04T15:45:45.380557+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9205205","created_at":"2026-07-04T15:45:45.380557+00:00"},{"alias_kind":"pith_short_12","alias_value":"5MURFZCA54KP","created_at":"2026-07-04T15:45:45.380557+00:00"},{"alias_kind":"pith_short_16","alias_value":"5MURFZCA54KPLNYK","created_at":"2026-07-04T15:45:45.380557+00:00"},{"alias_kind":"pith_short_8","alias_value":"5MURFZCA","created_at":"2026-07-04T15:45:45.380557+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.31331","citing_title":"Higher-Derivative Corrections to Reissner--Nordstr\\\"om Black Holes from Worldline QFT","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2604.08700","citing_title":"Axion Quality in Warped Extra-Dimension","ref_index":67,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67","json":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67.json","graph_json":"https://pith.science/api/pith-number/5MURFZCA54KPLNYK27AAMCKP67/graph.json","events_json":"https://pith.science/api/pith-number/5MURFZCA54KPLNYK27AAMCKP67/events.json","paper":"https://pith.science/paper/5MURFZCA"},"agent_actions":{"view_html":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67","download_json":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67.json","view_paper":"https://pith.science/paper/5MURFZCA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9205205&json=true","fetch_graph":"https://pith.science/api/pith-number/5MURFZCA54KPLNYK27AAMCKP67/graph.json","fetch_events":"https://pith.science/api/pith-number/5MURFZCA54KPLNYK27AAMCKP67/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67/action/storage_attestation","attest_author":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67/action/author_attestation","sign_citation":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67/action/citation_signature","submit_replication":"https://pith.science/pith/5MURFZCA54KPLNYK27AAMCKP67/action/replication_record"}},"created_at":"2026-07-04T15:45:45.380557+00:00","updated_at":"2026-07-04T15:45:45.380557+00:00"}