{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:PLI34G2DONARWZ36SG43DTGHJ6","short_pith_number":"pith:PLI34G2D","schema_version":"1.0","canonical_sha256":"7ad1be1b4373411b677e91b9b1ccc74f89535eccf5c8807dc38bd7f911d8c3c5","source":{"kind":"arxiv","id":"1306.0383","version":1},"attestation_state":"computed","paper":{"title":"Euler-Heisenberg lagrangian through Krein regularization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Refaei","submitted_at":"2013-06-03T12:36:17Z","abstract_excerpt":"The Euler-Heisenberg effective action at the one-loop for a constant electromagnetic field is derived in Krein space quantization with Ford's idea of uctuated light-cone. In this work we present a perturbative, but convergent solution of the effective action. Without using any renormalization procedure, the result coincides with the famous renormalized Euler-Heisenberg action."},"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":"1306.0383","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-06-03T12:36:17Z","cross_cats_sorted":[],"title_canon_sha256":"12a46c75791da8963f182f7be99c41909fe96f5fd0edcad60af158089fd71b1b","abstract_canon_sha256":"ffe84a4965dc508c7e77236dbeff04e0303deba6af46798a484de547046eaa4b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:55.365726Z","signature_b64":"tbukooVGUstDieIbptqdJ1EPgOTn2sfGBu0NAVLwtNliV6J/JGnESqT7AIqr2cyv/sDFUO4gzXNel5MGjZbiAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ad1be1b4373411b677e91b9b1ccc74f89535eccf5c8807dc38bd7f911d8c3c5","last_reissued_at":"2026-05-18T03:21:55.365243Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:55.365243Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Euler-Heisenberg lagrangian through Krein regularization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Refaei","submitted_at":"2013-06-03T12:36:17Z","abstract_excerpt":"The Euler-Heisenberg effective action at the one-loop for a constant electromagnetic field is derived in Krein space quantization with Ford's idea of uctuated light-cone. In this work we present a perturbative, but convergent solution of the effective action. Without using any renormalization procedure, the result coincides with the famous renormalized Euler-Heisenberg action."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.0383","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":""},"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":"1306.0383","created_at":"2026-05-18T03:21:55.365311+00:00"},{"alias_kind":"arxiv_version","alias_value":"1306.0383v1","created_at":"2026-05-18T03:21:55.365311+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.0383","created_at":"2026-05-18T03:21:55.365311+00:00"},{"alias_kind":"pith_short_12","alias_value":"PLI34G2DONAR","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PLI34G2DONARWZ36","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PLI34G2D","created_at":"2026-05-18T12:27:54.935989+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/PLI34G2DONARWZ36SG43DTGHJ6","json":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6.json","graph_json":"https://pith.science/api/pith-number/PLI34G2DONARWZ36SG43DTGHJ6/graph.json","events_json":"https://pith.science/api/pith-number/PLI34G2DONARWZ36SG43DTGHJ6/events.json","paper":"https://pith.science/paper/PLI34G2D"},"agent_actions":{"view_html":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6","download_json":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6.json","view_paper":"https://pith.science/paper/PLI34G2D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1306.0383&json=true","fetch_graph":"https://pith.science/api/pith-number/PLI34G2DONARWZ36SG43DTGHJ6/graph.json","fetch_events":"https://pith.science/api/pith-number/PLI34G2DONARWZ36SG43DTGHJ6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6/action/storage_attestation","attest_author":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6/action/author_attestation","sign_citation":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6/action/citation_signature","submit_replication":"https://pith.science/pith/PLI34G2DONARWZ36SG43DTGHJ6/action/replication_record"}},"created_at":"2026-05-18T03:21:55.365311+00:00","updated_at":"2026-05-18T03:21:55.365311+00:00"}