{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:7F7LKFDAPXOH7IK57OC7WFCWLD","short_pith_number":"pith:7F7LKFDA","canonical_record":{"source":{"id":"hep-th/0201096","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-15T01:24:30Z","cross_cats_sorted":[],"title_canon_sha256":"c3b28a560e574de3fecc27967184911a5b3f4a861cba56bd5120f33aa47b0bec","abstract_canon_sha256":"1ba798a378881f30bd79f299892b043e109a348f5b09e13051cb9eff4068662c"},"schema_version":"1.0"},"canonical_sha256":"f97eb514607ddc7fa15dfb85fb145658fa4a13909c01d0fe7a5b98a487c8d834","source":{"kind":"arxiv","id":"hep-th/0201096","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201096","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201096v3","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201096","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"pith_short_12","alias_value":"7F7LKFDAPXOH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"7F7LKFDAPXOH7IK5","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"7F7LKFDA","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:7F7LKFDAPXOH7IK57OC7WFCWLD","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0201096","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-15T01:24:30Z","cross_cats_sorted":[],"title_canon_sha256":"c3b28a560e574de3fecc27967184911a5b3f4a861cba56bd5120f33aa47b0bec","abstract_canon_sha256":"1ba798a378881f30bd79f299892b043e109a348f5b09e13051cb9eff4068662c"},"schema_version":"1.0"},"canonical_sha256":"f97eb514607ddc7fa15dfb85fb145658fa4a13909c01d0fe7a5b98a487c8d834","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:11.039567Z","signature_b64":"YHHolQdwVC66QbYMDYSfrncUnc0bq5PpaJfSuOPNEXltofHyS8U5tD7BYqxPx5nc2jd5MaHobO6TuEgoikkDCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f97eb514607ddc7fa15dfb85fb145658fa4a13909c01d0fe7a5b98a487c8d834","last_reissued_at":"2026-05-18T03:47:11.038960Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:11.038960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0201096","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:47:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UrlZJlkWAAxiSqdcndgy347dxOj09EVeL7XK7dqQcN2wg8rg1oCeRsg+JwQ7sUARK6CS4xRBQCmISoe4UPeCBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:45:36.364641Z"},"content_sha256":"a21a903a259364a88610343bcf1d49cfc4a23f04df692060ac5c45abbb059091","schema_version":"1.0","event_id":"sha256:a21a903a259364a88610343bcf1d49cfc4a23f04df692060ac5c45abbb059091"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:7F7LKFDAPXOH7IK57OC7WFCWLD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New 4D, N = 1 Superfield Theory: Model of Free Massive Superspin-3/2 Multiplet","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"I.L. Buchbinder, J. Phillips, Jr., S. James Gates, W. D. Linch","submitted_at":"2002-01-15T01:24:30Z","abstract_excerpt":"We present a Lagrangian formulation for the free superspin-3/2 massive 4D, N=1 superfield. The model is described by a dynamical real vector superfield and an auxiliary real scalar superfield. The corresponding multiplet contains spin-1, spin-2 and two spin-3/2 propagating component fields on-shell. The auxillary superfield is needed to ensure that the on-shell vector superfield carries only the irreducible representation of the Poincare supergroup with a given mass and the fixed superspin of 3/2. The bosonic sector of the component level of the model is also presented."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201096","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:47:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9AOezPXF3s0/8NNvhJlz+OgTyRoLmLbu4hdPiViTNCD5P2x3eOP4O+NbR4kTLYpP/+6TA7r3GABCCpvXPrcSDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:45:36.365052Z"},"content_sha256":"04d0bf30188c254bd69c79d8bbfd7c648e7a5d8a945e7bad159e9968ce9e04e7","schema_version":"1.0","event_id":"sha256:04d0bf30188c254bd69c79d8bbfd7c648e7a5d8a945e7bad159e9968ce9e04e7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/bundle.json","state_url":"https://pith.science/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-28T06:45:36Z","links":{"resolver":"https://pith.science/pith/7F7LKFDAPXOH7IK57OC7WFCWLD","bundle":"https://pith.science/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/bundle.json","state":"https://pith.science/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7F7LKFDAPXOH7IK57OC7WFCWLD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:7F7LKFDAPXOH7IK57OC7WFCWLD","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"1ba798a378881f30bd79f299892b043e109a348f5b09e13051cb9eff4068662c","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-15T01:24:30Z","title_canon_sha256":"c3b28a560e574de3fecc27967184911a5b3f4a861cba56bd5120f33aa47b0bec"},"schema_version":"1.0","source":{"id":"hep-th/0201096","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201096","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201096v3","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201096","created_at":"2026-05-18T03:47:11Z"},{"alias_kind":"pith_short_12","alias_value":"7F7LKFDAPXOH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"7F7LKFDAPXOH7IK5","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"7F7LKFDA","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:04d0bf30188c254bd69c79d8bbfd7c648e7a5d8a945e7bad159e9968ce9e04e7","target":"graph","created_at":"2026-05-18T03:47:11Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We present a Lagrangian formulation for the free superspin-3/2 massive 4D, N=1 superfield. The model is described by a dynamical real vector superfield and an auxiliary real scalar superfield. The corresponding multiplet contains spin-1, spin-2 and two spin-3/2 propagating component fields on-shell. The auxillary superfield is needed to ensure that the on-shell vector superfield carries only the irreducible representation of the Poincare supergroup with a given mass and the fixed superspin of 3/2. The bosonic sector of the component level of the model is also presented.","authors_text":"I.L. Buchbinder, J. Phillips, Jr., S. James Gates, W. D. Linch","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2002-01-15T01:24:30Z","title":"New 4D, N = 1 Superfield Theory: Model of Free Massive Superspin-3/2 Multiplet"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201096","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a21a903a259364a88610343bcf1d49cfc4a23f04df692060ac5c45abbb059091","target":"record","created_at":"2026-05-18T03:47:11Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"1ba798a378881f30bd79f299892b043e109a348f5b09e13051cb9eff4068662c","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-15T01:24:30Z","title_canon_sha256":"c3b28a560e574de3fecc27967184911a5b3f4a861cba56bd5120f33aa47b0bec"},"schema_version":"1.0","source":{"id":"hep-th/0201096","kind":"arxiv","version":3}},"canonical_sha256":"f97eb514607ddc7fa15dfb85fb145658fa4a13909c01d0fe7a5b98a487c8d834","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f97eb514607ddc7fa15dfb85fb145658fa4a13909c01d0fe7a5b98a487c8d834","first_computed_at":"2026-05-18T03:47:11.038960Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:47:11.038960Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YHHolQdwVC66QbYMDYSfrncUnc0bq5PpaJfSuOPNEXltofHyS8U5tD7BYqxPx5nc2jd5MaHobO6TuEgoikkDCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:47:11.039567Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0201096","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a21a903a259364a88610343bcf1d49cfc4a23f04df692060ac5c45abbb059091","sha256:04d0bf30188c254bd69c79d8bbfd7c648e7a5d8a945e7bad159e9968ce9e04e7"],"state_sha256":"3c747934a0e0687a6f566d9e7373425113918266e3e3bc0f9a9a5cd9492341f9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tDPS/wu/igye26bJbz97BUI8PtG8FXDSYcLK8ILNUfWoJzcTYFl9VyrAwVXLc0bgx5AVjCAebGHPP+uSxffAAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T06:45:36.368245Z","bundle_sha256":"fad0a96980c5738876f999f6e8ad6340080b7b06809970817bd12aab7e6c2bb0"}}