{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NLKSUVMWHPA6IG4IAANSOHVY52","short_pith_number":"pith:NLKSUVMW","schema_version":"1.0","canonical_sha256":"6ad52a55963bc1e41b88001b271eb8eeb588dfa988973f1f5eefceaae32253a9","source":{"kind":"arxiv","id":"1805.08225","version":2},"attestation_state":"computed","paper":{"title":"Supercurrent anomaly and gauge invariance in N=1 supersymmetric Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Adriano Cherchiglia, Brigitte Hiller, Marcos Sampaio, Y. R. Batista","submitted_at":"2018-05-21T18:00:07Z","abstract_excerpt":"We analyse Feynman diagram calculational issues related to the quantum breaking of supercurrent conservation in a supersymmetric non-abelian Yang-Mills theory. For the sake of simplicity, we take a zero mass gauge field multiplet interacting with a massless Majorana spin-$1/2$ field in the adjoint representation of $SU(2)$. We shed light on a long-standing controversy regarding the perturbative evaluation of the supercurrent anomaly in connection with gauge and superconformal symmetry in different frameworks. We find that only superconformal symmetry is unambiguously broken using an invariant "},"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":"1805.08225","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-05-21T18:00:07Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"63c820839a7cd3b107a865abd8049b73b8a9bb58b20c046a6cdfde4703614fe4","abstract_canon_sha256":"8bc13476f9b3eaf0a4c5f4ff059c55c3eacdeab81bdf6e14c46181182f71cedc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:08:41.632963Z","signature_b64":"RaBA+6ASQqQkyGqfHdrFDEzJK9Cj+8NbTcDEzdCeTtD4IYun/3FaAbALyZePPzGc7XNOtPXoau/P8g+N3KTMAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ad52a55963bc1e41b88001b271eb8eeb588dfa988973f1f5eefceaae32253a9","last_reissued_at":"2026-05-18T00:08:41.632216Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:08:41.632216Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supercurrent anomaly and gauge invariance in N=1 supersymmetric Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Adriano Cherchiglia, Brigitte Hiller, Marcos Sampaio, Y. R. Batista","submitted_at":"2018-05-21T18:00:07Z","abstract_excerpt":"We analyse Feynman diagram calculational issues related to the quantum breaking of supercurrent conservation in a supersymmetric non-abelian Yang-Mills theory. For the sake of simplicity, we take a zero mass gauge field multiplet interacting with a massless Majorana spin-$1/2$ field in the adjoint representation of $SU(2)$. We shed light on a long-standing controversy regarding the perturbative evaluation of the supercurrent anomaly in connection with gauge and superconformal symmetry in different frameworks. We find that only superconformal symmetry is unambiguously broken using an invariant "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.08225","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":"1805.08225","created_at":"2026-05-18T00:08:41.632335+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.08225v2","created_at":"2026-05-18T00:08:41.632335+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.08225","created_at":"2026-05-18T00:08:41.632335+00:00"},{"alias_kind":"pith_short_12","alias_value":"NLKSUVMWHPA6","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NLKSUVMWHPA6IG4I","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NLKSUVMW","created_at":"2026-05-18T12:32:40.477152+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/NLKSUVMWHPA6IG4IAANSOHVY52","json":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52.json","graph_json":"https://pith.science/api/pith-number/NLKSUVMWHPA6IG4IAANSOHVY52/graph.json","events_json":"https://pith.science/api/pith-number/NLKSUVMWHPA6IG4IAANSOHVY52/events.json","paper":"https://pith.science/paper/NLKSUVMW"},"agent_actions":{"view_html":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52","download_json":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52.json","view_paper":"https://pith.science/paper/NLKSUVMW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.08225&json=true","fetch_graph":"https://pith.science/api/pith-number/NLKSUVMWHPA6IG4IAANSOHVY52/graph.json","fetch_events":"https://pith.science/api/pith-number/NLKSUVMWHPA6IG4IAANSOHVY52/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52/action/storage_attestation","attest_author":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52/action/author_attestation","sign_citation":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52/action/citation_signature","submit_replication":"https://pith.science/pith/NLKSUVMWHPA6IG4IAANSOHVY52/action/replication_record"}},"created_at":"2026-05-18T00:08:41.632335+00:00","updated_at":"2026-05-18T00:08:41.632335+00:00"}