{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:TDPVZM2YXXQLENVZ6V5F4A7DQU","short_pith_number":"pith:TDPVZM2Y","schema_version":"1.0","canonical_sha256":"98df5cb358bde0b236b9f57a5e03e3852b24361f58049521a8fc101a5ec5e481","source":{"kind":"arxiv","id":"hep-th/9405188","version":3},"attestation_state":"computed","paper":{"title":"Mass formulae and natural hierarchy in string effective supergravities","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"C.Kounnas, F.Zwirner, S.Ferrara","submitted_at":"1994-05-30T10:03:00Z","abstract_excerpt":"We study some conditions for the hierarchy $m_{3/2} << M_P$ to occur naturally in a generic effective supergravity theory. Absence of fine-tuning and perturbative calculability require that the effective potential has a sliding gravitino mass and vanishing cosmological constant, up to ${\\cal O}(m_{3/2}^4)$ corrections. In particular, cancellation of quadratically divergent contributions to the one-loop effective potential should take place, including the `hidden sector' of the theory. We show that these conditions can be met in the effective supergravities derived from four-dimensional superst"},"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/9405188","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-05-30T10:03:00Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"eb6b66843f7c85da5d4ab9cd3ac81c33ab7cb698077f3bda1e6b80f7f38517d2","abstract_canon_sha256":"145f4795c51249076129e57b0da36fc9c734fb28bf616fef877fd61dded699c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:04.380396Z","signature_b64":"LK8Htj2fqFCkjO+PADJmR/IxMRGOWIghEu3ZWsFc6SVgfGAQW8pbtCQLwlwPq53ywWQONNmaIlmGQC8tKkX8Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"98df5cb358bde0b236b9f57a5e03e3852b24361f58049521a8fc101a5ec5e481","last_reissued_at":"2026-05-18T02:36:04.379843Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:04.379843Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mass formulae and natural hierarchy in string effective supergravities","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"C.Kounnas, F.Zwirner, S.Ferrara","submitted_at":"1994-05-30T10:03:00Z","abstract_excerpt":"We study some conditions for the hierarchy $m_{3/2} << M_P$ to occur naturally in a generic effective supergravity theory. Absence of fine-tuning and perturbative calculability require that the effective potential has a sliding gravitino mass and vanishing cosmological constant, up to ${\\cal O}(m_{3/2}^4)$ corrections. In particular, cancellation of quadratically divergent contributions to the one-loop effective potential should take place, including the `hidden sector' of the theory. We show that these conditions can be met in the effective supergravities derived from four-dimensional superst"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9405188","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":""},"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/9405188","created_at":"2026-05-18T02:36:04.379924+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9405188v3","created_at":"2026-05-18T02:36:04.379924+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9405188","created_at":"2026-05-18T02:36:04.379924+00:00"},{"alias_kind":"pith_short_12","alias_value":"TDPVZM2YXXQL","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"TDPVZM2YXXQLENVZ","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"TDPVZM2Y","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.04146","citing_title":"(Pseudo-)Dirac Gravitinos","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU","json":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU.json","graph_json":"https://pith.science/api/pith-number/TDPVZM2YXXQLENVZ6V5F4A7DQU/graph.json","events_json":"https://pith.science/api/pith-number/TDPVZM2YXXQLENVZ6V5F4A7DQU/events.json","paper":"https://pith.science/paper/TDPVZM2Y"},"agent_actions":{"view_html":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU","download_json":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU.json","view_paper":"https://pith.science/paper/TDPVZM2Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9405188&json=true","fetch_graph":"https://pith.science/api/pith-number/TDPVZM2YXXQLENVZ6V5F4A7DQU/graph.json","fetch_events":"https://pith.science/api/pith-number/TDPVZM2YXXQLENVZ6V5F4A7DQU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU/action/storage_attestation","attest_author":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU/action/author_attestation","sign_citation":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU/action/citation_signature","submit_replication":"https://pith.science/pith/TDPVZM2YXXQLENVZ6V5F4A7DQU/action/replication_record"}},"created_at":"2026-05-18T02:36:04.379924+00:00","updated_at":"2026-05-18T02:36:04.379924+00:00"}