{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:RAUXHSJYZKQO5VWS76IBYCYISS","short_pith_number":"pith:RAUXHSJY","schema_version":"1.0","canonical_sha256":"882973c938caa0eed6d2ff901c0b0894b8388da91b69c8372b297093f7fad8e3","source":{"kind":"arxiv","id":"1809.03957","version":2},"attestation_state":"computed","paper":{"title":"Higher derivative three-form gauge theories and their supersymmetric extension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Ryo Yokokura","submitted_at":"2018-09-11T15:03:38Z","abstract_excerpt":"We investigate three-form gauge theories with higher derivative interactions and their supersymmetric extensions in four space-time dimensions. For the bosonic three-form gauge theories, we show that derivatives on the field strength of the 3-form gauge field yield a tachyon as far as the Lagrangian contains a quadratic kinetic term, while such the term with opposite sign gives rise to a ghost. We confirm that there is neither a tachyon nor a ghost when all higher derivative terms are given by functions of the field strength. For this ghost/tachyon-free Lagrangian, we determine the boundary te"},"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":"1809.03957","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-09-11T15:03:38Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2668c73abeb57b42d57734701989aa781da0ecd2fdaacc5071a36caff2c0a655","abstract_canon_sha256":"1a9039388ceda4a4074fbc06f59bd245d4ea8812ec13dd0d485bda1e8fd2007b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:02:09.089620Z","signature_b64":"rZtZEQZ+z+GLK3pp4PsJGfApXtSXNuS6OpXE5kFRyN2j9QE9wnTzrHl0PG80I8tm8SiJGEu4klvB4dbHgvb9Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"882973c938caa0eed6d2ff901c0b0894b8388da91b69c8372b297093f7fad8e3","last_reissued_at":"2026-05-18T00:02:09.088956Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:02:09.088956Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher derivative three-form gauge theories and their supersymmetric extension","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Muneto Nitta, Ryo Yokokura","submitted_at":"2018-09-11T15:03:38Z","abstract_excerpt":"We investigate three-form gauge theories with higher derivative interactions and their supersymmetric extensions in four space-time dimensions. For the bosonic three-form gauge theories, we show that derivatives on the field strength of the 3-form gauge field yield a tachyon as far as the Lagrangian contains a quadratic kinetic term, while such the term with opposite sign gives rise to a ghost. We confirm that there is neither a tachyon nor a ghost when all higher derivative terms are given by functions of the field strength. For this ghost/tachyon-free Lagrangian, we determine the boundary te"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.03957","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":"1809.03957","created_at":"2026-05-18T00:02:09.089049+00:00"},{"alias_kind":"arxiv_version","alias_value":"1809.03957v2","created_at":"2026-05-18T00:02:09.089049+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.03957","created_at":"2026-05-18T00:02:09.089049+00:00"},{"alias_kind":"pith_short_12","alias_value":"RAUXHSJYZKQO","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_16","alias_value":"RAUXHSJYZKQO5VWS","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_8","alias_value":"RAUXHSJY","created_at":"2026-05-18T12:32:50.500415+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/RAUXHSJYZKQO5VWS76IBYCYISS","json":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS.json","graph_json":"https://pith.science/api/pith-number/RAUXHSJYZKQO5VWS76IBYCYISS/graph.json","events_json":"https://pith.science/api/pith-number/RAUXHSJYZKQO5VWS76IBYCYISS/events.json","paper":"https://pith.science/paper/RAUXHSJY"},"agent_actions":{"view_html":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS","download_json":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS.json","view_paper":"https://pith.science/paper/RAUXHSJY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1809.03957&json=true","fetch_graph":"https://pith.science/api/pith-number/RAUXHSJYZKQO5VWS76IBYCYISS/graph.json","fetch_events":"https://pith.science/api/pith-number/RAUXHSJYZKQO5VWS76IBYCYISS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS/action/storage_attestation","attest_author":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS/action/author_attestation","sign_citation":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS/action/citation_signature","submit_replication":"https://pith.science/pith/RAUXHSJYZKQO5VWS76IBYCYISS/action/replication_record"}},"created_at":"2026-05-18T00:02:09.089049+00:00","updated_at":"2026-05-18T00:02:09.089049+00:00"}