{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:FHTYJC2MOQHG6OXK7OOBQ5VF4S","short_pith_number":"pith:FHTYJC2M","schema_version":"1.0","canonical_sha256":"29e7848b4c740e6f3aeafb9c1876a5e48651f22fcf47d7e41ffa1c8d364e3abf","source":{"kind":"arxiv","id":"1512.00546","version":1},"attestation_state":"computed","paper":{"title":"Inflatino-less Cosmology","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":"Andrei Linde, John Joseph M. Carrasco, Renata Kallosh","submitted_at":"2015-12-02T02:33:34Z","abstract_excerpt":"We construct inflationary models in the context of supergravity with orthogonal nilpotent superfields [1]. When local supersymmetry is gauge-fixed in the unitary gauge, these models describe theories with only a single real scalar (the inflaton), a graviton and a gravitino. Critically, there is no inflatino, no sgoldstino, and no sinflaton in these models. This dramatically simplifies cosmological models which can simultaneously describe inflation, dark energy and SUSY breaking."},"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":"1512.00546","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-12-02T02:33:34Z","cross_cats_sorted":["astro-ph.CO","gr-qc","hep-ph"],"title_canon_sha256":"59b4992a11953422df15ec28df6d368cce5be779b9f258a56b8aeaaf6def59da","abstract_canon_sha256":"aca5301593e8d682d8a7eb7aa3dee5a815e825da069d66ccb8c784e0826fa82c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:30.429749Z","signature_b64":"Ap67wsPIhRy8hpXKRSdsG5Q4seiYuu+yLF2ZO5D+dJwZueZg2PF6lv7V1BwN54eUD2vphQgETPOrPSzKOg3sDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29e7848b4c740e6f3aeafb9c1876a5e48651f22fcf47d7e41ffa1c8d364e3abf","last_reissued_at":"2026-05-18T01:18:30.429142Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:30.429142Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inflatino-less Cosmology","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":"Andrei Linde, John Joseph M. Carrasco, Renata Kallosh","submitted_at":"2015-12-02T02:33:34Z","abstract_excerpt":"We construct inflationary models in the context of supergravity with orthogonal nilpotent superfields [1]. When local supersymmetry is gauge-fixed in the unitary gauge, these models describe theories with only a single real scalar (the inflaton), a graviton and a gravitino. Critically, there is no inflatino, no sgoldstino, and no sinflaton in these models. This dramatically simplifies cosmological models which can simultaneously describe inflation, dark energy and SUSY breaking."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.00546","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":"1512.00546","created_at":"2026-05-18T01:18:30.429236+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.00546v1","created_at":"2026-05-18T01:18:30.429236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.00546","created_at":"2026-05-18T01:18:30.429236+00:00"},{"alias_kind":"pith_short_12","alias_value":"FHTYJC2MOQHG","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"FHTYJC2MOQHG6OXK","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"FHTYJC2M","created_at":"2026-05-18T12:29:19.899920+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.16976","citing_title":"Creation of spin-3/2 dark matter via cosmological gravitational particle production","ref_index":3,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S","json":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S.json","graph_json":"https://pith.science/api/pith-number/FHTYJC2MOQHG6OXK7OOBQ5VF4S/graph.json","events_json":"https://pith.science/api/pith-number/FHTYJC2MOQHG6OXK7OOBQ5VF4S/events.json","paper":"https://pith.science/paper/FHTYJC2M"},"agent_actions":{"view_html":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S","download_json":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S.json","view_paper":"https://pith.science/paper/FHTYJC2M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.00546&json=true","fetch_graph":"https://pith.science/api/pith-number/FHTYJC2MOQHG6OXK7OOBQ5VF4S/graph.json","fetch_events":"https://pith.science/api/pith-number/FHTYJC2MOQHG6OXK7OOBQ5VF4S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S/action/storage_attestation","attest_author":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S/action/author_attestation","sign_citation":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S/action/citation_signature","submit_replication":"https://pith.science/pith/FHTYJC2MOQHG6OXK7OOBQ5VF4S/action/replication_record"}},"created_at":"2026-05-18T01:18:30.429236+00:00","updated_at":"2026-05-18T01:18:30.429236+00:00"}