{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:TZC5P3BMX57QK26B2UJRMTP6KG","short_pith_number":"pith:TZC5P3BM","schema_version":"1.0","canonical_sha256":"9e45d7ec2cbf7f056bc1d513164dfe519f1c60c128c914d06a75d778b1eadad2","source":{"kind":"arxiv","id":"1105.2983","version":3},"attestation_state":"computed","paper":{"title":"No-Core MCSM calculation for $^{10}$Be and $^{12}$Be low-lying spectra","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Lang Liu, Noritaka Shimizu, Robert Roth, Takaharu Otsuka, Yutaka Utsuno","submitted_at":"2011-05-16T00:29:50Z","abstract_excerpt":"The low-lying excited states of $^{10}$Be and $^{12}$Be are investigated within a no-core Monte Carlo Shell Model (MCSM) framework employing a realistic potential obtained via the Unitary Correlation Operator Method. The excitation energies of the 2$^+_1$ and 2$^+_2$ states and the B(E2;$\\,2^+_{1,2}\\rightarrow$ 0$^+_{g.s.}$) for $^{10}$Be in the MCSM with a standard treatment of spurious center-of-mass motion show good agreement with experimental data. Some properties of low-lying states of $^{10}$Be are studied in terms of quadrupole moments, E2 transitions and single-particle occupation numb"},"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":"1105.2983","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-05-16T00:29:50Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"000175646acd8bd1c7a535bc30afee5782be03f69d4419480fbf584a088c77e6","abstract_canon_sha256":"42ed091b490db8f4f4c38dfe169178ffceb82ac246b461795902079076d43018"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:29.687703Z","signature_b64":"cMod3dwenJX+pC8i+uODS3k3mvnDH8Y+01JaBv8NMC9N6wZ78OD29beVot/8aeFvvjMdiYSjExShGHtupoqVBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e45d7ec2cbf7f056bc1d513164dfe519f1c60c128c914d06a75d778b1eadad2","last_reissued_at":"2026-05-18T03:41:29.687078Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:29.687078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"No-Core MCSM calculation for $^{10}$Be and $^{12}$Be low-lying spectra","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Lang Liu, Noritaka Shimizu, Robert Roth, Takaharu Otsuka, Yutaka Utsuno","submitted_at":"2011-05-16T00:29:50Z","abstract_excerpt":"The low-lying excited states of $^{10}$Be and $^{12}$Be are investigated within a no-core Monte Carlo Shell Model (MCSM) framework employing a realistic potential obtained via the Unitary Correlation Operator Method. The excitation energies of the 2$^+_1$ and 2$^+_2$ states and the B(E2;$\\,2^+_{1,2}\\rightarrow$ 0$^+_{g.s.}$) for $^{10}$Be in the MCSM with a standard treatment of spurious center-of-mass motion show good agreement with experimental data. Some properties of low-lying states of $^{10}$Be are studied in terms of quadrupole moments, E2 transitions and single-particle occupation numb"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2983","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":"1105.2983","created_at":"2026-05-18T03:41:29.687168+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.2983v3","created_at":"2026-05-18T03:41:29.687168+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2983","created_at":"2026-05-18T03:41:29.687168+00:00"},{"alias_kind":"pith_short_12","alias_value":"TZC5P3BMX57Q","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"TZC5P3BMX57QK26B","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"TZC5P3BM","created_at":"2026-05-18T12:26:42.757692+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/TZC5P3BMX57QK26B2UJRMTP6KG","json":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG.json","graph_json":"https://pith.science/api/pith-number/TZC5P3BMX57QK26B2UJRMTP6KG/graph.json","events_json":"https://pith.science/api/pith-number/TZC5P3BMX57QK26B2UJRMTP6KG/events.json","paper":"https://pith.science/paper/TZC5P3BM"},"agent_actions":{"view_html":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG","download_json":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG.json","view_paper":"https://pith.science/paper/TZC5P3BM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.2983&json=true","fetch_graph":"https://pith.science/api/pith-number/TZC5P3BMX57QK26B2UJRMTP6KG/graph.json","fetch_events":"https://pith.science/api/pith-number/TZC5P3BMX57QK26B2UJRMTP6KG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG/action/storage_attestation","attest_author":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG/action/author_attestation","sign_citation":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG/action/citation_signature","submit_replication":"https://pith.science/pith/TZC5P3BMX57QK26B2UJRMTP6KG/action/replication_record"}},"created_at":"2026-05-18T03:41:29.687168+00:00","updated_at":"2026-05-18T03:41:29.687168+00:00"}