{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:6NKMWTRP57N2WJSWQRLOY6XJA6","short_pith_number":"pith:6NKMWTRP","schema_version":"1.0","canonical_sha256":"f354cb4e2fefdbab26568456ec7ae90783f2c5f3725a5caa22705540e038fc25","source":{"kind":"arxiv","id":"1611.09676","version":1},"attestation_state":"computed","paper":{"title":"On the one-loop effective potential in nonlocal supersymmetric theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"A. Yu. Petrov, E. R. Bezerra de Mello, F. S. Gama, J. R. Nascimento","submitted_at":"2016-11-29T15:20:22Z","abstract_excerpt":"Within the superfield approach, we consider the nonlocal generalization of the Wess-Zumino model and calculate the one-loop low-energy contributions to the effective action. Four different nonlocal models are considered, among which only the first model does not reduce to the standard Wess-Zumino model when we take the parameter of nonlocality of the model, $\\Lambda$, much greater than any energy scale; in addition, this model also depends on an extra parameter, $\\xi$. As to the other three models, the result looks like the renormalized effective potential for the usual Wess-Zumino model, wher"},"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":"1611.09676","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-11-29T15:20:22Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"84ed0998dfde844312f3dfce74ae27c96bed097b9b22a0e9fb675b4f414095c0","abstract_canon_sha256":"b3d9f5b98a4ca66851e9824f3b078b7797e311d91eaf88ee96fec16ea05692ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:12.959813Z","signature_b64":"bAlUN8fdqwaJc7/62UvoIMp10I+GR5+cBzd7t/D9qL0XloR6TuFv1un7Sb5Ns9TIprKvc4vWR8VKzpfivknYCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f354cb4e2fefdbab26568456ec7ae90783f2c5f3725a5caa22705540e038fc25","last_reissued_at":"2026-05-18T00:51:12.959080Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:12.959080Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the one-loop effective potential in nonlocal supersymmetric theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"A. Yu. Petrov, E. R. Bezerra de Mello, F. S. Gama, J. R. Nascimento","submitted_at":"2016-11-29T15:20:22Z","abstract_excerpt":"Within the superfield approach, we consider the nonlocal generalization of the Wess-Zumino model and calculate the one-loop low-energy contributions to the effective action. Four different nonlocal models are considered, among which only the first model does not reduce to the standard Wess-Zumino model when we take the parameter of nonlocality of the model, $\\Lambda$, much greater than any energy scale; in addition, this model also depends on an extra parameter, $\\xi$. As to the other three models, the result looks like the renormalized effective potential for the usual Wess-Zumino model, wher"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.09676","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":"1611.09676","created_at":"2026-05-18T00:51:12.959203+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.09676v1","created_at":"2026-05-18T00:51:12.959203+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.09676","created_at":"2026-05-18T00:51:12.959203+00:00"},{"alias_kind":"pith_short_12","alias_value":"6NKMWTRP57N2","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"6NKMWTRP57N2WJSW","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"6NKMWTRP","created_at":"2026-05-18T12:30:01.593930+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/6NKMWTRP57N2WJSWQRLOY6XJA6","json":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6.json","graph_json":"https://pith.science/api/pith-number/6NKMWTRP57N2WJSWQRLOY6XJA6/graph.json","events_json":"https://pith.science/api/pith-number/6NKMWTRP57N2WJSWQRLOY6XJA6/events.json","paper":"https://pith.science/paper/6NKMWTRP"},"agent_actions":{"view_html":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6","download_json":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6.json","view_paper":"https://pith.science/paper/6NKMWTRP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.09676&json=true","fetch_graph":"https://pith.science/api/pith-number/6NKMWTRP57N2WJSWQRLOY6XJA6/graph.json","fetch_events":"https://pith.science/api/pith-number/6NKMWTRP57N2WJSWQRLOY6XJA6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6/action/storage_attestation","attest_author":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6/action/author_attestation","sign_citation":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6/action/citation_signature","submit_replication":"https://pith.science/pith/6NKMWTRP57N2WJSWQRLOY6XJA6/action/replication_record"}},"created_at":"2026-05-18T00:51:12.959203+00:00","updated_at":"2026-05-18T00:51:12.959203+00:00"}