{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ZBESSXEXECDXFAVI3K3RZ5JMBV","short_pith_number":"pith:ZBESSXEX","schema_version":"1.0","canonical_sha256":"c849295c9720877282a8dab71cf52c0d7abc50b2c199378a8aa2af171e4531d5","source":{"kind":"arxiv","id":"1508.05040","version":1},"attestation_state":"computed","paper":{"title":"Exploring sd-shell nuclei from two- and three-nucleon interactions with realistic saturation properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Schwenk, J.D. Holt, J. Menendez, J. Simonis, K. Hebeler","submitted_at":"2015-08-20T16:48:53Z","abstract_excerpt":"We study ground- and excited-state properties of all sd-shell nuclei with neutron and proton numbers 8 <= N,Z <= 20, based on a set of low-resolution two- and three-nucleon interactions that predict realistic saturation properties of nuclear matter. We focus on estimating the theoretical uncertainties due to variation of the resolution scale, the low-energy couplings, as well as from the many-body method. The experimental two-neutron and two-proton separation energies are reasonably well reproduced, with an uncertainty range of about 5 MeV. The first excited 2+ energies also show overall agree"},"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":"1508.05040","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-08-20T16:48:53Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"01162671250aac6a147b418bb3675b25809e7ff2bf9136e4250581e1f115c987","abstract_canon_sha256":"d648edd308b6866f32d16f2f20de118f04e9ee71676e8f23699b8962e755c771"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:14.332442Z","signature_b64":"neme82vujGewOIgAFkkJvQXamwzE6gp26O5DERtcGtpKLGSv29vPS3LamweKLYJ9GUhugVh4xtidFmemKdWoDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c849295c9720877282a8dab71cf52c0d7abc50b2c199378a8aa2af171e4531d5","last_reissued_at":"2026-05-18T01:22:14.331694Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:14.331694Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Exploring sd-shell nuclei from two- and three-nucleon interactions with realistic saturation properties","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Schwenk, J.D. Holt, J. Menendez, J. Simonis, K. Hebeler","submitted_at":"2015-08-20T16:48:53Z","abstract_excerpt":"We study ground- and excited-state properties of all sd-shell nuclei with neutron and proton numbers 8 <= N,Z <= 20, based on a set of low-resolution two- and three-nucleon interactions that predict realistic saturation properties of nuclear matter. We focus on estimating the theoretical uncertainties due to variation of the resolution scale, the low-energy couplings, as well as from the many-body method. The experimental two-neutron and two-proton separation energies are reasonably well reproduced, with an uncertainty range of about 5 MeV. The first excited 2+ energies also show overall agree"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.05040","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":"1508.05040","created_at":"2026-05-18T01:22:14.331781+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.05040v1","created_at":"2026-05-18T01:22:14.331781+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.05040","created_at":"2026-05-18T01:22:14.331781+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZBESSXEXECDX","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZBESSXEXECDXFAVI","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZBESSXEX","created_at":"2026-05-18T12:29:52.810259+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/ZBESSXEXECDXFAVI3K3RZ5JMBV","json":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV.json","graph_json":"https://pith.science/api/pith-number/ZBESSXEXECDXFAVI3K3RZ5JMBV/graph.json","events_json":"https://pith.science/api/pith-number/ZBESSXEXECDXFAVI3K3RZ5JMBV/events.json","paper":"https://pith.science/paper/ZBESSXEX"},"agent_actions":{"view_html":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV","download_json":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV.json","view_paper":"https://pith.science/paper/ZBESSXEX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.05040&json=true","fetch_graph":"https://pith.science/api/pith-number/ZBESSXEXECDXFAVI3K3RZ5JMBV/graph.json","fetch_events":"https://pith.science/api/pith-number/ZBESSXEXECDXFAVI3K3RZ5JMBV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV/action/storage_attestation","attest_author":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV/action/author_attestation","sign_citation":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV/action/citation_signature","submit_replication":"https://pith.science/pith/ZBESSXEXECDXFAVI3K3RZ5JMBV/action/replication_record"}},"created_at":"2026-05-18T01:22:14.331781+00:00","updated_at":"2026-05-18T01:22:14.331781+00:00"}