{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:J2D775PGYPGQRVADOPTCZYEOZ2","short_pith_number":"pith:J2D775PG","schema_version":"1.0","canonical_sha256":"4e87fff5e6c3cd08d40373e62ce08ece8ccafb3d738421c80027053ae5b50e2b","source":{"kind":"arxiv","id":"1502.01650","version":2},"attestation_state":"computed","paper":{"title":"Massive Born--Infeld and Other Dual Pairs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Sagnotti, S. Ferrara","submitted_at":"2015-02-05T17:33:04Z","abstract_excerpt":"We consider massive dual pairs of p-forms and (D-p-1)-forms described by non-linear Lagrangians, where non-linear curvature terms in one theory translate into non-linear mass-like terms in the dual theory. In particular, for D=2p and p even the two non-linear structures coincide when the non-linear massless theory is self-dual. This state of affairs finds a natural realization in the four-dimensional massive N=1 supersymmetric Born-Infeld action, which describes either a massive vector multiplet or a massive linear (tensor) multiplet with a Born-Infeld mass-like term. These systems should play"},"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":"1502.01650","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-02-05T17:33:04Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"cf994155a0a095948c7f7c47f124e5bfe0bd6f90d42082cdb7d285c5ee943961","abstract_canon_sha256":"32987ab7d166431a3179dcc32ad145b5db8220433991e86d3071b314fbbcc46f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:04.606814Z","signature_b64":"TlepEKyjG6qKti5rD+wcSDWq5WzeBwVj/a8V62djv6YVgGZ7OCf2ZDrB6kHDazrjWHu8fkwhtZSeZpE343c+Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e87fff5e6c3cd08d40373e62ce08ece8ccafb3d738421c80027053ae5b50e2b","last_reissued_at":"2026-05-18T01:41:04.606106Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:04.606106Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Massive Born--Infeld and Other Dual Pairs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"A. Sagnotti, S. Ferrara","submitted_at":"2015-02-05T17:33:04Z","abstract_excerpt":"We consider massive dual pairs of p-forms and (D-p-1)-forms described by non-linear Lagrangians, where non-linear curvature terms in one theory translate into non-linear mass-like terms in the dual theory. In particular, for D=2p and p even the two non-linear structures coincide when the non-linear massless theory is self-dual. This state of affairs finds a natural realization in the four-dimensional massive N=1 supersymmetric Born-Infeld action, which describes either a massive vector multiplet or a massive linear (tensor) multiplet with a Born-Infeld mass-like term. These systems should play"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.01650","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":"1502.01650","created_at":"2026-05-18T01:41:04.606225+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.01650v2","created_at":"2026-05-18T01:41:04.606225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.01650","created_at":"2026-05-18T01:41:04.606225+00:00"},{"alias_kind":"pith_short_12","alias_value":"J2D775PGYPGQ","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"J2D775PGYPGQRVAD","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"J2D775PG","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.00071","citing_title":"Diagnosing Effective Metal-Insulator and Hawking-Page Transitions: A Mixed-State Entanglement Perspective in Einstein-Born-Infeld-Massive Gravity","ref_index":43,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2","json":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2.json","graph_json":"https://pith.science/api/pith-number/J2D775PGYPGQRVADOPTCZYEOZ2/graph.json","events_json":"https://pith.science/api/pith-number/J2D775PGYPGQRVADOPTCZYEOZ2/events.json","paper":"https://pith.science/paper/J2D775PG"},"agent_actions":{"view_html":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2","download_json":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2.json","view_paper":"https://pith.science/paper/J2D775PG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.01650&json=true","fetch_graph":"https://pith.science/api/pith-number/J2D775PGYPGQRVADOPTCZYEOZ2/graph.json","fetch_events":"https://pith.science/api/pith-number/J2D775PGYPGQRVADOPTCZYEOZ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2/action/storage_attestation","attest_author":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2/action/author_attestation","sign_citation":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2/action/citation_signature","submit_replication":"https://pith.science/pith/J2D775PGYPGQRVADOPTCZYEOZ2/action/replication_record"}},"created_at":"2026-05-18T01:41:04.606225+00:00","updated_at":"2026-05-18T01:41:04.606225+00:00"}