{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:GHFTIIQF4GESVNME4AROJIOO66","short_pith_number":"pith:GHFTIIQF","schema_version":"1.0","canonical_sha256":"31cb342205e1892ab584e022e4a1cef7987ef35ef38b240327ba61a8cad6dcca","source":{"kind":"arxiv","id":"1508.05421","version":3},"attestation_state":"computed","paper":{"title":"Subtleties in the beta function calculation of N=1 supersymmetric gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. L. Cherchiglia, A. P. Ba\\^eta Scarpelli, B. Hiller, Marcos Sampaio","submitted_at":"2015-08-21T21:59:27Z","abstract_excerpt":"We investigate some peculiarities in the calculation of the two-loop beta-function of $N=1$ supersymmetric models which are intimately related to the so-called \"Anomaly Puzzle\". There is an apparent paradox when the computation is performed in the framework of the covariant derivative background field method. In this formalism, it is obtained a finite two-loop effective action, although a non-null coefficient for the beta-function is achieved by means of the renormalized two-point function in the background field. We show that if the standard background field method is used, this two-point fun"},"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":"1508.05421","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-08-21T21:59:27Z","cross_cats_sorted":[],"title_canon_sha256":"7bb85447c513b658bf08a1f2855e1fde92e57b7582109d0991124525cc49c656","abstract_canon_sha256":"2efc8e1b9f58916f31c1d86a338a4c95ca11a7a3b86db20d6d9efb9c191aec77"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:44.698386Z","signature_b64":"WNpObL6ieI6i0A4A7TvbLIR98eB1pZJddgHG9R0DLzgKZyyJjZj0NCmpIE1fn3nBzzQ5tmbV21J3Ud5W4WI/Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31cb342205e1892ab584e022e4a1cef7987ef35ef38b240327ba61a8cad6dcca","last_reissued_at":"2026-05-18T01:21:44.697743Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:44.697743Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Subtleties in the beta function calculation of N=1 supersymmetric gauge theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. L. Cherchiglia, A. P. Ba\\^eta Scarpelli, B. Hiller, Marcos Sampaio","submitted_at":"2015-08-21T21:59:27Z","abstract_excerpt":"We investigate some peculiarities in the calculation of the two-loop beta-function of $N=1$ supersymmetric models which are intimately related to the so-called \"Anomaly Puzzle\". There is an apparent paradox when the computation is performed in the framework of the covariant derivative background field method. In this formalism, it is obtained a finite two-loop effective action, although a non-null coefficient for the beta-function is achieved by means of the renormalized two-point function in the background field. We show that if the standard background field method is used, this two-point fun"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.05421","kind":"arxiv","version":3},"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":"1508.05421","created_at":"2026-05-18T01:21:44.697833+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.05421v3","created_at":"2026-05-18T01:21:44.697833+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.05421","created_at":"2026-05-18T01:21:44.697833+00:00"},{"alias_kind":"pith_short_12","alias_value":"GHFTIIQF4GES","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_16","alias_value":"GHFTIIQF4GESVNME","created_at":"2026-05-18T12:29:22.688609+00:00"},{"alias_kind":"pith_short_8","alias_value":"GHFTIIQF","created_at":"2026-05-18T12:29:22.688609+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/GHFTIIQF4GESVNME4AROJIOO66","json":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66.json","graph_json":"https://pith.science/api/pith-number/GHFTIIQF4GESVNME4AROJIOO66/graph.json","events_json":"https://pith.science/api/pith-number/GHFTIIQF4GESVNME4AROJIOO66/events.json","paper":"https://pith.science/paper/GHFTIIQF"},"agent_actions":{"view_html":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66","download_json":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66.json","view_paper":"https://pith.science/paper/GHFTIIQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.05421&json=true","fetch_graph":"https://pith.science/api/pith-number/GHFTIIQF4GESVNME4AROJIOO66/graph.json","fetch_events":"https://pith.science/api/pith-number/GHFTIIQF4GESVNME4AROJIOO66/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66/action/storage_attestation","attest_author":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66/action/author_attestation","sign_citation":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66/action/citation_signature","submit_replication":"https://pith.science/pith/GHFTIIQF4GESVNME4AROJIOO66/action/replication_record"}},"created_at":"2026-05-18T01:21:44.697833+00:00","updated_at":"2026-05-18T01:21:44.697833+00:00"}