{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:HXM3U4INAUPOX5SAHU345GMYFB","short_pith_number":"pith:HXM3U4IN","schema_version":"1.0","canonical_sha256":"3dd9ba710d051eebf6403d37ce9998285d24d26cf90dd44dfd74254d548261c6","source":{"kind":"arxiv","id":"2104.08288","version":3},"attestation_state":"computed","paper":{"title":"The Gravitino and the Swampland","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Dieter Lust, Marco Scalisi, Niccol\\`o Cribiori","submitted_at":"2021-04-16T18:00:02Z","abstract_excerpt":"We propose a new swampland conjecture stating that the limit of vanishing gravitino mass corresponds to the massless limit of an infinite tower of states and to the consequent breakdown of the effective field theory. We test our proposal in large classes of models coming from compactification of string theory to four dimensions, where we identify the Kaluza-Klein nature of the tower of states becoming light. We point out a general relation between the gravitino mass and abelian gauge coupling in models with extended supersymmetry, which can survive also in examples with minimal supersymmetry. "},"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":"2104.08288","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-04-16T18:00:02Z","cross_cats_sorted":["astro-ph.CO","gr-qc","hep-ph"],"title_canon_sha256":"36686e9d6dda6be9ec387991776d33f79dd1e2b196d6a8c63dc4d914c6785b34","abstract_canon_sha256":"17a39928d3fc1e5de21e293da36351afde32ab5a5333c6d9efb0cfbd9d9213f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:51:40.066765Z","signature_b64":"Q8SUJ6Go3l/fTea/ttnZLf0D3nJmm9iCuy/AqbZznhxzX8wGZ6tWGjqyexWXuYwvTi7IC9YsrZMTPfTDWtxQBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3dd9ba710d051eebf6403d37ce9998285d24d26cf90dd44dfd74254d548261c6","last_reissued_at":"2026-07-05T02:51:40.066157Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:51:40.066157Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Gravitino and the Swampland","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Dieter Lust, Marco Scalisi, Niccol\\`o Cribiori","submitted_at":"2021-04-16T18:00:02Z","abstract_excerpt":"We propose a new swampland conjecture stating that the limit of vanishing gravitino mass corresponds to the massless limit of an infinite tower of states and to the consequent breakdown of the effective field theory. We test our proposal in large classes of models coming from compactification of string theory to four dimensions, where we identify the Kaluza-Klein nature of the tower of states becoming light. We point out a general relation between the gravitino mass and abelian gauge coupling in models with extended supersymmetry, which can survive also in examples with minimal supersymmetry. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.08288","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2104.08288/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2104.08288","created_at":"2026-07-05T02:51:40.066244+00:00"},{"alias_kind":"arxiv_version","alias_value":"2104.08288v3","created_at":"2026-07-05T02:51:40.066244+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2104.08288","created_at":"2026-07-05T02:51:40.066244+00:00"},{"alias_kind":"pith_short_12","alias_value":"HXM3U4INAUPO","created_at":"2026-07-05T02:51:40.066244+00:00"},{"alias_kind":"pith_short_16","alias_value":"HXM3U4INAUPOX5SA","created_at":"2026-07-05T02:51:40.066244+00:00"},{"alias_kind":"pith_short_8","alias_value":"HXM3U4IN","created_at":"2026-07-05T02:51:40.066244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.08244","citing_title":"Stochastic Survival near Swampland Boundaries","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02708","citing_title":"Supersymmetry, Large Extra Dimensions and the Gravitino Conjecture","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06796","citing_title":"Decaying spin-3/2 dark matter from baryon number violation","ref_index":46,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB","json":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB.json","graph_json":"https://pith.science/api/pith-number/HXM3U4INAUPOX5SAHU345GMYFB/graph.json","events_json":"https://pith.science/api/pith-number/HXM3U4INAUPOX5SAHU345GMYFB/events.json","paper":"https://pith.science/paper/HXM3U4IN"},"agent_actions":{"view_html":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB","download_json":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB.json","view_paper":"https://pith.science/paper/HXM3U4IN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2104.08288&json=true","fetch_graph":"https://pith.science/api/pith-number/HXM3U4INAUPOX5SAHU345GMYFB/graph.json","fetch_events":"https://pith.science/api/pith-number/HXM3U4INAUPOX5SAHU345GMYFB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB/action/storage_attestation","attest_author":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB/action/author_attestation","sign_citation":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB/action/citation_signature","submit_replication":"https://pith.science/pith/HXM3U4INAUPOX5SAHU345GMYFB/action/replication_record"}},"created_at":"2026-07-05T02:51:40.066244+00:00","updated_at":"2026-07-05T02:51:40.066244+00:00"}