{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:45CPLTINHH25GYWWQK2FGPYG6J","short_pith_number":"pith:45CPLTIN","schema_version":"1.0","canonical_sha256":"e744f5cd0d39f5d362d682b4533f06f24ab0289421d6ce72d979a5789b98d4eb","source":{"kind":"arxiv","id":"hep-th/9907124","version":3},"attestation_state":"computed","paper":{"title":"Gravitino Production After Inflation","license":"","headline":"","cross_cats":["astro-ph","gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Andrei Linde, Antoine Van Proeyen, Lev Kofman, Renata Kallosh","submitted_at":"1999-07-15T14:15:24Z","abstract_excerpt":"We investigate the production of gravitinos in a cosmological background. Gravitinos can be produced during preheating after inflation due to a combined effect of interactions with an oscillating inflaton field and absence of conformal invariance. In order to get insight on conformal properties of gravitino we reformulate phenomenological supergravity in SU(2,2|1)-symmetric way. The Planck mass and F- and D-terms appear via the gauge-fixed value of a superfield that we call conformon. We find that in general the probability of gravitino production is not suppressed by the small gravitational c"},"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":"hep-th/9907124","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-07-15T14:15:24Z","cross_cats_sorted":["astro-ph","gr-qc","hep-ph"],"title_canon_sha256":"8bd85d1962fe55c9adb3b8fb0d62f71fce3bf730d2cf3d57871779d28bc11d96","abstract_canon_sha256":"a29585b829d9c2f653512107c6a58e6bc5491473981f59475e44c65bbf684933"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:52:12.478764Z","signature_b64":"ftmyEvgTELk2EXl17kZaA8Zp0nvqM/J8tFAxqJQITIu8g+XuvuVyUZ7L4h+c9kV2UGZUfVLWKLk7sgYmTab1Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e744f5cd0d39f5d362d682b4533f06f24ab0289421d6ce72d979a5789b98d4eb","last_reissued_at":"2026-07-04T15:52:12.478371Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:52:12.478371Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitino Production After Inflation","license":"","headline":"","cross_cats":["astro-ph","gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Andrei Linde, Antoine Van Proeyen, Lev Kofman, Renata Kallosh","submitted_at":"1999-07-15T14:15:24Z","abstract_excerpt":"We investigate the production of gravitinos in a cosmological background. Gravitinos can be produced during preheating after inflation due to a combined effect of interactions with an oscillating inflaton field and absence of conformal invariance. In order to get insight on conformal properties of gravitino we reformulate phenomenological supergravity in SU(2,2|1)-symmetric way. The Planck mass and F- and D-terms appear via the gauge-fixed value of a superfield that we call conformon. We find that in general the probability of gravitino production is not suppressed by the small gravitational c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9907124","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/hep-th/9907124/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":"hep-th/9907124","created_at":"2026-07-04T15:52:12.478435+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9907124v3","created_at":"2026-07-04T15:52:12.478435+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9907124","created_at":"2026-07-04T15:52:12.478435+00:00"},{"alias_kind":"pith_short_12","alias_value":"45CPLTINHH25","created_at":"2026-07-04T15:52:12.478435+00:00"},{"alias_kind":"pith_short_16","alias_value":"45CPLTINHH25GYWW","created_at":"2026-07-04T15:52:12.478435+00:00"},{"alias_kind":"pith_short_8","alias_value":"45CPLTIN","created_at":"2026-07-04T15:52:12.478435+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2606.23447","citing_title":"Dark matter from the quadratic spinor Lagrangian I: Geometric mass for a gravitationally produced spin-1/2 fermion","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23273","citing_title":"Dark matter from the quadratic spinor Lagrangian II: A spin-3/2 no-go and the uniqueness of the spin-1/2 candidate","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23273","citing_title":"Dark matter from the quadratic spinor Lagrangian II: A spin-3/2 no-go and the uniqueness of the spin-1/2 candidate","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2512.16976","citing_title":"Creation of spin-3/2 dark matter via cosmological gravitational particle production","ref_index":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J","json":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J.json","graph_json":"https://pith.science/api/pith-number/45CPLTINHH25GYWWQK2FGPYG6J/graph.json","events_json":"https://pith.science/api/pith-number/45CPLTINHH25GYWWQK2FGPYG6J/events.json","paper":"https://pith.science/paper/45CPLTIN"},"agent_actions":{"view_html":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J","download_json":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J.json","view_paper":"https://pith.science/paper/45CPLTIN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9907124&json=true","fetch_graph":"https://pith.science/api/pith-number/45CPLTINHH25GYWWQK2FGPYG6J/graph.json","fetch_events":"https://pith.science/api/pith-number/45CPLTINHH25GYWWQK2FGPYG6J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J/action/storage_attestation","attest_author":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J/action/author_attestation","sign_citation":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J/action/citation_signature","submit_replication":"https://pith.science/pith/45CPLTINHH25GYWWQK2FGPYG6J/action/replication_record"}},"created_at":"2026-07-04T15:52:12.478435+00:00","updated_at":"2026-07-04T15:52:12.478435+00:00"}