{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:XJILQZRMNWFQFRPZ77GS4P7UWV","short_pith_number":"pith:XJILQZRM","schema_version":"1.0","canonical_sha256":"ba50b8662c6d8b02c5f9ffcd2e3ff4b54d9cdfbc85ccf556cb4968981aa5f99b","source":{"kind":"arxiv","id":"1411.7550","version":1},"attestation_state":"computed","paper":{"title":"Component on-shell actions of supersymmetric 3-branes II. 3-brane in D=8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sutulin, N. Kozyrev, S. Bellucci, S. Krivonos","submitted_at":"2014-11-27T11:17:18Z","abstract_excerpt":"In the present paper we explicitly construct the on-shell supersymmetric component action for a 3-brane moving in D=8 within the nonlinear realizations framework. Similarly to the previously considered case of the super 3-brane in D=6, all ingredients entering the component action follow from the nonlinear realizations approach. The component action of the 3-brane possesses N=4, d=4 supersymmetry partially broken to N=2, d=4 one. The basic Goldstone superfield is the generalized version of N=2,d=4 hypermultiplet. The action has a structure, such that all terms of higher orders in the fermions "},"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":"1411.7550","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-11-27T11:17:18Z","cross_cats_sorted":[],"title_canon_sha256":"e0f2db7771d100970b8d5787b6c7c2c142312e55af6a02c15048855cf3736246","abstract_canon_sha256":"53f8f1949196f21496a65ff24ecd9ecc23e16317418df9545282c97bfa27fa1a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:18.874162Z","signature_b64":"lljc2XTrD2Axe7bu7KAwOlSegQtHFXukz+xef29YGqNTltuZDXySAvOgLGkKjF9uTrci9govjPnVpPMgKOJABg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba50b8662c6d8b02c5f9ffcd2e3ff4b54d9cdfbc85ccf556cb4968981aa5f99b","last_reissued_at":"2026-05-18T00:51:18.873485Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:18.873485Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Component on-shell actions of supersymmetric 3-branes II. 3-brane in D=8","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sutulin, N. Kozyrev, S. Bellucci, S. Krivonos","submitted_at":"2014-11-27T11:17:18Z","abstract_excerpt":"In the present paper we explicitly construct the on-shell supersymmetric component action for a 3-brane moving in D=8 within the nonlinear realizations framework. Similarly to the previously considered case of the super 3-brane in D=6, all ingredients entering the component action follow from the nonlinear realizations approach. The component action of the 3-brane possesses N=4, d=4 supersymmetry partially broken to N=2, d=4 one. The basic Goldstone superfield is the generalized version of N=2,d=4 hypermultiplet. The action has a structure, such that all terms of higher orders in the fermions "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1411.7550","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":"1411.7550","created_at":"2026-05-18T00:51:18.873605+00:00"},{"alias_kind":"arxiv_version","alias_value":"1411.7550v1","created_at":"2026-05-18T00:51:18.873605+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1411.7550","created_at":"2026-05-18T00:51:18.873605+00:00"},{"alias_kind":"pith_short_12","alias_value":"XJILQZRMNWFQ","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"XJILQZRMNWFQFRPZ","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"XJILQZRM","created_at":"2026-05-18T12:28:57.508820+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/XJILQZRMNWFQFRPZ77GS4P7UWV","json":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV.json","graph_json":"https://pith.science/api/pith-number/XJILQZRMNWFQFRPZ77GS4P7UWV/graph.json","events_json":"https://pith.science/api/pith-number/XJILQZRMNWFQFRPZ77GS4P7UWV/events.json","paper":"https://pith.science/paper/XJILQZRM"},"agent_actions":{"view_html":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV","download_json":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV.json","view_paper":"https://pith.science/paper/XJILQZRM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1411.7550&json=true","fetch_graph":"https://pith.science/api/pith-number/XJILQZRMNWFQFRPZ77GS4P7UWV/graph.json","fetch_events":"https://pith.science/api/pith-number/XJILQZRMNWFQFRPZ77GS4P7UWV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV/action/storage_attestation","attest_author":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV/action/author_attestation","sign_citation":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV/action/citation_signature","submit_replication":"https://pith.science/pith/XJILQZRMNWFQFRPZ77GS4P7UWV/action/replication_record"}},"created_at":"2026-05-18T00:51:18.873605+00:00","updated_at":"2026-05-18T00:51:18.873605+00:00"}