{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:JJXP4V7VCFIYDHJTEFKBO2U7HD","short_pith_number":"pith:JJXP4V7V","schema_version":"1.0","canonical_sha256":"4a6efe57f51151819d332154176a9f38e1d1423de571108a06b2509347817570","source":{"kind":"arxiv","id":"nucl-th/0206061","version":1},"attestation_state":"computed","paper":{"title":"Quantum Monte Carlo calculations of $A=9,10$ nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"K. Varga, R. B. Wiringa, Steven C. Pieper","submitted_at":"2002-06-24T20:17:44Z","abstract_excerpt":"We report on quantum Monte Carlo calculations of the ground and low-lying excited states of $A=9,10$ nuclei using realistic Hamiltonians containing the Argonne $v_{18}$ two-nucleon potential alone or with one of several three-nucleon potentials, including Urbana IX and three of the new Illinois models. The calculations begin with correlated many-body wave functions that have an $\\alpha$-like core and multiple p-shell nucleons, $LS$-coupled to the appropriate $(J^{\\pi};T)$ quantum numbers for the state of interest. After optimization, these variational trial functions are used as input to a Gre"},"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/0206061","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2002-06-24T20:17:44Z","cross_cats_sorted":[],"title_canon_sha256":"df66126e81994387351b085862a9d292a17e6812e8d35afe57eedf607967950e","abstract_canon_sha256":"a9016d1d7c811238e68740230892a7a4fc396114b094418c0828459206353428"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:26:53.521640Z","signature_b64":"mD7XYe6U+sAAKaR9aiz0jaibGSGdI0cbhoExMFCE8mxZtyVSIpRddPhtOtItYYgyx9h1gcit038Pc7PyCNnAAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4a6efe57f51151819d332154176a9f38e1d1423de571108a06b2509347817570","last_reissued_at":"2026-07-04T15:26:53.521085Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:26:53.521085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Monte Carlo calculations of $A=9,10$ nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"K. Varga, R. B. Wiringa, Steven C. Pieper","submitted_at":"2002-06-24T20:17:44Z","abstract_excerpt":"We report on quantum Monte Carlo calculations of the ground and low-lying excited states of $A=9,10$ nuclei using realistic Hamiltonians containing the Argonne $v_{18}$ two-nucleon potential alone or with one of several three-nucleon potentials, including Urbana IX and three of the new Illinois models. The calculations begin with correlated many-body wave functions that have an $\\alpha$-like core and multiple p-shell nucleons, $LS$-coupled to the appropriate $(J^{\\pi};T)$ quantum numbers for the state of interest. After optimization, these variational trial functions are used as input to a Gre"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0206061","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/nucl-th/0206061/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":"nucl-th/0206061","created_at":"2026-07-04T15:26:53.521129+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0206061v1","created_at":"2026-07-04T15:26:53.521129+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0206061","created_at":"2026-07-04T15:26:53.521129+00:00"},{"alias_kind":"pith_short_12","alias_value":"JJXP4V7VCFIY","created_at":"2026-07-04T15:26:53.521129+00:00"},{"alias_kind":"pith_short_16","alias_value":"JJXP4V7VCFIYDHJT","created_at":"2026-07-04T15:26:53.521129+00:00"},{"alias_kind":"pith_short_8","alias_value":"JJXP4V7V","created_at":"2026-07-04T15:26:53.521129+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01493","citing_title":"Probing the tetrahedral $\\alpha$ clusters in relativistic $^{16}$O + $^{16}$O collisions","ref_index":33,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD","json":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD.json","graph_json":"https://pith.science/api/pith-number/JJXP4V7VCFIYDHJTEFKBO2U7HD/graph.json","events_json":"https://pith.science/api/pith-number/JJXP4V7VCFIYDHJTEFKBO2U7HD/events.json","paper":"https://pith.science/paper/JJXP4V7V"},"agent_actions":{"view_html":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD","download_json":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD.json","view_paper":"https://pith.science/paper/JJXP4V7V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0206061&json=true","fetch_graph":"https://pith.science/api/pith-number/JJXP4V7VCFIYDHJTEFKBO2U7HD/graph.json","fetch_events":"https://pith.science/api/pith-number/JJXP4V7VCFIYDHJTEFKBO2U7HD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD/action/storage_attestation","attest_author":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD/action/author_attestation","sign_citation":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD/action/citation_signature","submit_replication":"https://pith.science/pith/JJXP4V7VCFIYDHJTEFKBO2U7HD/action/replication_record"}},"created_at":"2026-07-04T15:26:53.521129+00:00","updated_at":"2026-07-04T15:26:53.521129+00:00"}