{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:25X4SN4IJRMOFUFGBPJO5QZYA6","short_pith_number":"pith:25X4SN4I","schema_version":"1.0","canonical_sha256":"d76fc937884c58e2d0a60bd2eec338079759e104d8e1044e451310a6d2ef3dd3","source":{"kind":"arxiv","id":"1806.01573","version":2},"attestation_state":"computed","paper":{"title":"Realistic shell-model calculations for p-shell nuclei including contributions of a chiral three-body force","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Gargano, F. R. Xu, L. Coraggio, L. De Angelis, N. Itaco, T. Fukui, Y. Z. Ma","submitted_at":"2018-06-05T09:21:44Z","abstract_excerpt":"In this paper we present an evolution of our derivation of the shell-model effective Hamiltonian, namely introducing effects of three-body contributions. More precisely, we consider a three-body potential at next-to-next-to-leading order in chiral perturbation theory, and the induced three-body forces that arise from many-body correlations among valence nucleons. The first one is included, in the derivation of the effective Hamiltonian for one- and two-valence nucleon-systems, at first order in the many-body perturbation theory. Namely, we include only the three-body interaction between one or"},"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":"1806.01573","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-06-05T09:21:44Z","cross_cats_sorted":[],"title_canon_sha256":"f8ea088ad2585d7ccdb0d027c1e613bf21702f0b81012d254850d5403dce97c3","abstract_canon_sha256":"73f15bab8ad60cc985616245b30398b109e61235ae2ea71438627fe52516e228"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:46.772286Z","signature_b64":"pF1mXzXi4yvoAM4YsmS/9ZtBmRYxg5WAofJfcRUAGzIo/QaMIYsMVCw0qFtNs1c5hDDUFy0/wjGKj8qfCP4YBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d76fc937884c58e2d0a60bd2eec338079759e104d8e1044e451310a6d2ef3dd3","last_reissued_at":"2026-05-18T00:03:46.771668Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:46.771668Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Realistic shell-model calculations for p-shell nuclei including contributions of a chiral three-body force","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Gargano, F. R. Xu, L. Coraggio, L. De Angelis, N. Itaco, T. Fukui, Y. Z. Ma","submitted_at":"2018-06-05T09:21:44Z","abstract_excerpt":"In this paper we present an evolution of our derivation of the shell-model effective Hamiltonian, namely introducing effects of three-body contributions. More precisely, we consider a three-body potential at next-to-next-to-leading order in chiral perturbation theory, and the induced three-body forces that arise from many-body correlations among valence nucleons. The first one is included, in the derivation of the effective Hamiltonian for one- and two-valence nucleon-systems, at first order in the many-body perturbation theory. Namely, we include only the three-body interaction between one or"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.01573","kind":"arxiv","version":2},"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":"1806.01573","created_at":"2026-05-18T00:03:46.771747+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.01573v2","created_at":"2026-05-18T00:03:46.771747+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.01573","created_at":"2026-05-18T00:03:46.771747+00:00"},{"alias_kind":"pith_short_12","alias_value":"25X4SN4IJRMO","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"25X4SN4IJRMOFUFG","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"25X4SN4I","created_at":"2026-05-18T12:31:59.375834+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/25X4SN4IJRMOFUFGBPJO5QZYA6","json":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6.json","graph_json":"https://pith.science/api/pith-number/25X4SN4IJRMOFUFGBPJO5QZYA6/graph.json","events_json":"https://pith.science/api/pith-number/25X4SN4IJRMOFUFGBPJO5QZYA6/events.json","paper":"https://pith.science/paper/25X4SN4I"},"agent_actions":{"view_html":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6","download_json":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6.json","view_paper":"https://pith.science/paper/25X4SN4I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.01573&json=true","fetch_graph":"https://pith.science/api/pith-number/25X4SN4IJRMOFUFGBPJO5QZYA6/graph.json","fetch_events":"https://pith.science/api/pith-number/25X4SN4IJRMOFUFGBPJO5QZYA6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6/action/storage_attestation","attest_author":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6/action/author_attestation","sign_citation":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6/action/citation_signature","submit_replication":"https://pith.science/pith/25X4SN4IJRMOFUFGBPJO5QZYA6/action/replication_record"}},"created_at":"2026-05-18T00:03:46.771747+00:00","updated_at":"2026-05-18T00:03:46.771747+00:00"}