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First, using the semi-empirical mass formula with the DRHBc mass table, we investigate the symmetry energy at saturation density $\\rho_0$, denoted as $S_0$, and the ratio of surface to volume contributions to the symmetry energy, $\\kappa$. As a result, we obtain $S_0=27.85\\,{\\rm MeV}$ ($\\kappa=1.38$) for $a_{\\rm sym}(A) =S_0 (1 - \\kappa A^{-1/3})$ (Type I) and $S_0=32.66\\,{\\rm MeV}$ ($\\kappa=3.15$"},"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":"2307.05018","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-07-11T05:35:59Z","cross_cats_sorted":[],"title_canon_sha256":"020987016a5232bab52df1d83b527ee094340ec7215feeba790bc28697a67675","abstract_canon_sha256":"d0a451e2580544097bb879e546a9997920ba1fbdcc99a7b702c43372c322fee9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:29:24.963388Z","signature_b64":"YAyJ296HxcipnkQxQBxDGxi5infGoQzGYBuL2gBU0+w3WYDzLRgIPef9LiVDhCghUqy7egRNyUAWaF0jYpb0BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1149511cead48a362c1406245cae4f1fab323175169b5c9a677557a939a47b3e","last_reissued_at":"2026-07-05T06:29:24.962959Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:29:24.962959Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of neutron-rich nuclei masses on symmetry energy","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Dukjae Jang, Myung-Ki Cheoun, Seonghyun Kim, Soonchul Choi, Tsuyoshi Miyatsu","submitted_at":"2023-07-11T05:35:59Z","abstract_excerpt":"We explore the impact of neutron-rich nuclei masses on the symmetry energy properties using the mass table evaluated by the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) model. 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As a result, we obtain $S_0=27.85\\,{\\rm MeV}$ ($\\kappa=1.38$) for $a_{\\rm sym}(A) =S_0 (1 - \\kappa A^{-1/3})$ (Type I) and $S_0=32.66\\,{\\rm MeV}$ ($\\kappa=3.15$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.05018","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2307.05018/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":"2307.05018","created_at":"2026-07-05T06:29:24.963022+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.05018v1","created_at":"2026-07-05T06:29:24.963022+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.05018","created_at":"2026-07-05T06:29:24.963022+00:00"},{"alias_kind":"pith_short_12","alias_value":"CFEVCHHK2SFD","created_at":"2026-07-05T06:29:24.963022+00:00"},{"alias_kind":"pith_short_16","alias_value":"CFEVCHHK2SFDMLAU","created_at":"2026-07-05T06:29:24.963022+00:00"},{"alias_kind":"pith_short_8","alias_value":"CFEVCHHK","created_at":"2026-07-05T06:29:24.963022+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/CFEVCHHK2SFDMLAUAYSFZLSPD6","json":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6.json","graph_json":"https://pith.science/api/pith-number/CFEVCHHK2SFDMLAUAYSFZLSPD6/graph.json","events_json":"https://pith.science/api/pith-number/CFEVCHHK2SFDMLAUAYSFZLSPD6/events.json","paper":"https://pith.science/paper/CFEVCHHK"},"agent_actions":{"view_html":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6","download_json":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6.json","view_paper":"https://pith.science/paper/CFEVCHHK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.05018&json=true","fetch_graph":"https://pith.science/api/pith-number/CFEVCHHK2SFDMLAUAYSFZLSPD6/graph.json","fetch_events":"https://pith.science/api/pith-number/CFEVCHHK2SFDMLAUAYSFZLSPD6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6/action/storage_attestation","attest_author":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6/action/author_attestation","sign_citation":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6/action/citation_signature","submit_replication":"https://pith.science/pith/CFEVCHHK2SFDMLAUAYSFZLSPD6/action/replication_record"}},"created_at":"2026-07-05T06:29:24.963022+00:00","updated_at":"2026-07-05T06:29:24.963022+00:00"}