{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:4GV3ILJKVIKGFLR7OSVSQTZ4YA","short_pith_number":"pith:4GV3ILJK","schema_version":"1.0","canonical_sha256":"e1abb42d2aaa1462ae3f74ab284f3cc0142cd200e8660c87df3a421e76bf3342","source":{"kind":"arxiv","id":"hep-th/9506029","version":1},"attestation_state":"computed","paper":{"title":"Superspace Formulation of Yang- Mills Theory II: Inclusion of Gauge Invariant Operators and Scalars","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bhabani Prasad Mandal, Satish D. Joglekar","submitted_at":"1995-06-06T14:10:41Z","abstract_excerpt":"In a superspace formulation of Yang-Mills theory previously proposed, we show how gauge-invariant operators and scalars can be incorporated keeping intact the (broken) $Osp(3,1|2)$ symmetry of the superspace action. We show in both cases, that the WT identities can be cast in a simple form $\\frac{\\partial\\bar{W}}{\\partial\\theta}=0$."},"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":"hep-th/9506029","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-06-06T14:10:41Z","cross_cats_sorted":[],"title_canon_sha256":"dbc02bbe42525ea397c9bc8682a9327beb63e0560e28de2b1bdfb7147d142b68","abstract_canon_sha256":"455f546f5c99c009da96648911aceddce3e211567de90b99059e851c25970ae7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:03.975290Z","signature_b64":"kHcPaepRLUYrRxNBQNCZfXAEUBLe7rNazQhVD9ZQtTQywwqUz3RsUajVrTQxTiK5FdpsOP9x5Rald2bivzmfBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1abb42d2aaa1462ae3f74ab284f3cc0142cd200e8660c87df3a421e76bf3342","last_reissued_at":"2026-05-18T02:36:03.974694Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:03.974694Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superspace Formulation of Yang- Mills Theory II: Inclusion of Gauge Invariant Operators and Scalars","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Bhabani Prasad Mandal, Satish D. Joglekar","submitted_at":"1995-06-06T14:10:41Z","abstract_excerpt":"In a superspace formulation of Yang-Mills theory previously proposed, we show how gauge-invariant operators and scalars can be incorporated keeping intact the (broken) $Osp(3,1|2)$ symmetry of the superspace action. We show in both cases, that the WT identities can be cast in a simple form $\\frac{\\partial\\bar{W}}{\\partial\\theta}=0$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9506029","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":"hep-th/9506029","created_at":"2026-05-18T02:36:03.974786+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9506029v1","created_at":"2026-05-18T02:36:03.974786+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9506029","created_at":"2026-05-18T02:36:03.974786+00:00"},{"alias_kind":"pith_short_12","alias_value":"4GV3ILJKVIKG","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"4GV3ILJKVIKGFLR7","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"4GV3ILJK","created_at":"2026-05-18T12:25:47.102015+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/4GV3ILJKVIKGFLR7OSVSQTZ4YA","json":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA.json","graph_json":"https://pith.science/api/pith-number/4GV3ILJKVIKGFLR7OSVSQTZ4YA/graph.json","events_json":"https://pith.science/api/pith-number/4GV3ILJKVIKGFLR7OSVSQTZ4YA/events.json","paper":"https://pith.science/paper/4GV3ILJK"},"agent_actions":{"view_html":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA","download_json":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA.json","view_paper":"https://pith.science/paper/4GV3ILJK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9506029&json=true","fetch_graph":"https://pith.science/api/pith-number/4GV3ILJKVIKGFLR7OSVSQTZ4YA/graph.json","fetch_events":"https://pith.science/api/pith-number/4GV3ILJKVIKGFLR7OSVSQTZ4YA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA/action/storage_attestation","attest_author":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA/action/author_attestation","sign_citation":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA/action/citation_signature","submit_replication":"https://pith.science/pith/4GV3ILJKVIKGFLR7OSVSQTZ4YA/action/replication_record"}},"created_at":"2026-05-18T02:36:03.974786+00:00","updated_at":"2026-05-18T02:36:03.974786+00:00"}