{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:WJEBY5FJTJFJV6DEXAUZHEZCPJ","short_pith_number":"pith:WJEBY5FJ","schema_version":"1.0","canonical_sha256":"b2481c74a99a4a9af864b8299393227a53ffec085d47f9d7313c690ac7d00898","source":{"kind":"arxiv","id":"1507.06771","version":2},"attestation_state":"computed","paper":{"title":"Complex-mass renormalization in hadronic EFT: applicability at two-loop order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. Djukanovic, E. Epelbaum, H. Krebs, J. Gegelia, U.-G. Mei{\\ss}ner","submitted_at":"2015-07-24T08:08:30Z","abstract_excerpt":"We discuss the application of the complex-mass scheme to multi-loop diagrams in hadronic effective field theory by considering as an example a two-loop self-energy diagram. We show that the renormalized two-loop diagram satisfies the power counting."},"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":"1507.06771","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-07-24T08:08:30Z","cross_cats_sorted":[],"title_canon_sha256":"d03edb494add7f7c1a9db596adffc14ef963ab77bfaa4f4c9dfa9425b442e6a7","abstract_canon_sha256":"fff0d8aea3843f14d308d3a0c12c8046c1dc5eb1ca774f201d04b3c1355693d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:32:00.199886Z","signature_b64":"ebxpfAIZKKc1Ncww4/yTt9sAVOZStcjjIFL044emIMRnSsZWrz13mn7y3X5nQ1n+eqWXFwWWz6Pbb1vIPghfAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b2481c74a99a4a9af864b8299393227a53ffec085d47f9d7313c690ac7d00898","last_reissued_at":"2026-05-18T01:32:00.199179Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:32:00.199179Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Complex-mass renormalization in hadronic EFT: applicability at two-loop order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. Djukanovic, E. Epelbaum, H. Krebs, J. Gegelia, U.-G. Mei{\\ss}ner","submitted_at":"2015-07-24T08:08:30Z","abstract_excerpt":"We discuss the application of the complex-mass scheme to multi-loop diagrams in hadronic effective field theory by considering as an example a two-loop self-energy diagram. We show that the renormalized two-loop diagram satisfies the power counting."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.06771","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":"1507.06771","created_at":"2026-05-18T01:32:00.199280+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.06771v2","created_at":"2026-05-18T01:32:00.199280+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.06771","created_at":"2026-05-18T01:32:00.199280+00:00"},{"alias_kind":"pith_short_12","alias_value":"WJEBY5FJTJFJ","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_16","alias_value":"WJEBY5FJTJFJV6DE","created_at":"2026-05-18T12:29:47.479230+00:00"},{"alias_kind":"pith_short_8","alias_value":"WJEBY5FJ","created_at":"2026-05-18T12:29:47.479230+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/WJEBY5FJTJFJV6DEXAUZHEZCPJ","json":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ.json","graph_json":"https://pith.science/api/pith-number/WJEBY5FJTJFJV6DEXAUZHEZCPJ/graph.json","events_json":"https://pith.science/api/pith-number/WJEBY5FJTJFJV6DEXAUZHEZCPJ/events.json","paper":"https://pith.science/paper/WJEBY5FJ"},"agent_actions":{"view_html":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ","download_json":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ.json","view_paper":"https://pith.science/paper/WJEBY5FJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.06771&json=true","fetch_graph":"https://pith.science/api/pith-number/WJEBY5FJTJFJV6DEXAUZHEZCPJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WJEBY5FJTJFJV6DEXAUZHEZCPJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ/action/storage_attestation","attest_author":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ/action/author_attestation","sign_citation":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ/action/citation_signature","submit_replication":"https://pith.science/pith/WJEBY5FJTJFJV6DEXAUZHEZCPJ/action/replication_record"}},"created_at":"2026-05-18T01:32:00.199280+00:00","updated_at":"2026-05-18T01:32:00.199280+00:00"}