{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:HRVWQLX425PRJG6JYM5UARJAJP","short_pith_number":"pith:HRVWQLX4","schema_version":"1.0","canonical_sha256":"3c6b682efcd75f149bc9c33b4045204bdaef4777caaeefcb55862e5a2129acbd","source":{"kind":"arxiv","id":"nucl-th/0003028","version":1},"attestation_state":"computed","paper":{"title":"LOCV calculation for Beta-stable matter at finite temperature","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. R. Moshfegh, M. Modarres","submitted_at":"2000-03-13T12:44:29Z","abstract_excerpt":"The method of lowest-order constrained variational, which predicts reasonably the nuclear matter semi-empirical data is used to calculate the equation of state of beta-stable matter at finite temperature. The Reid soft-core with and without the N-$\\Delta$ interactions which fits the N-N scattering data as well as the $UV_{14}$ potential plus the three-nucleon interaction are considered in the nuclear many-body Hamiltonian. The electron and muon are treated relativistically in the total Hamiltonian at given temperature, to make the fluid electrically neutral and stable against beta decay. The 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":"nucl-th/0003028","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-03-13T12:44:29Z","cross_cats_sorted":[],"title_canon_sha256":"9d543c954d660e263df2de14454598177dc66c63889767386745a373986247e0","abstract_canon_sha256":"ee59707427dab6fe4c6f1eacc71f84bc90e1beb78d08984ea06e9f29da7a30ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:21.341638Z","signature_b64":"uDCno1O3NEf6C9Few2J0g1xHbAL/EN0IaEZTAfPOiBC5j5GI3waVOqUF8jMKUMFyHjU6p0Q7ziQVFUz5gDk5DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c6b682efcd75f149bc9c33b4045204bdaef4777caaeefcb55862e5a2129acbd","last_reissued_at":"2026-05-18T01:05:21.341055Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:21.341055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"LOCV calculation for Beta-stable matter at finite temperature","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. R. Moshfegh, M. Modarres","submitted_at":"2000-03-13T12:44:29Z","abstract_excerpt":"The method of lowest-order constrained variational, which predicts reasonably the nuclear matter semi-empirical data is used to calculate the equation of state of beta-stable matter at finite temperature. The Reid soft-core with and without the N-$\\Delta$ interactions which fits the N-N scattering data as well as the $UV_{14}$ potential plus the three-nucleon interaction are considered in the nuclear many-body Hamiltonian. The electron and muon are treated relativistically in the total Hamiltonian at given temperature, to make the fluid electrically neutral and stable against beta decay. The c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0003028","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":"nucl-th/0003028","created_at":"2026-05-18T01:05:21.341147+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0003028v1","created_at":"2026-05-18T01:05:21.341147+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0003028","created_at":"2026-05-18T01:05:21.341147+00:00"},{"alias_kind":"pith_short_12","alias_value":"HRVWQLX425PR","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"HRVWQLX425PRJG6J","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"HRVWQLX4","created_at":"2026-05-18T12:25:49.631198+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP","json":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP.json","graph_json":"https://pith.science/api/pith-number/HRVWQLX425PRJG6JYM5UARJAJP/graph.json","events_json":"https://pith.science/api/pith-number/HRVWQLX425PRJG6JYM5UARJAJP/events.json","paper":"https://pith.science/paper/HRVWQLX4"},"agent_actions":{"view_html":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP","download_json":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP.json","view_paper":"https://pith.science/paper/HRVWQLX4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0003028&json=true","fetch_graph":"https://pith.science/api/pith-number/HRVWQLX425PRJG6JYM5UARJAJP/graph.json","fetch_events":"https://pith.science/api/pith-number/HRVWQLX425PRJG6JYM5UARJAJP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP/action/storage_attestation","attest_author":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP/action/author_attestation","sign_citation":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP/action/citation_signature","submit_replication":"https://pith.science/pith/HRVWQLX425PRJG6JYM5UARJAJP/action/replication_record"}},"created_at":"2026-05-18T01:05:21.341147+00:00","updated_at":"2026-05-18T01:05:21.341147+00:00"}