{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:KLBYSZLT5IVGJVSYQIE5QG23HP","short_pith_number":"pith:KLBYSZLT","schema_version":"1.0","canonical_sha256":"52c3896573ea2a64d6588209d81b5b3be8d7ad4fa264b72b33caba163ef88461","source":{"kind":"arxiv","id":"2206.13208","version":1},"attestation_state":"computed","paper":{"title":"Relativistic effects and three-body interactions in atomic nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"P. W. Zhao, Y. L. Yang","submitted_at":"2022-06-27T11:50:39Z","abstract_excerpt":"Based on the leading-order covariant pionless effective field theory, a relativistic nuclear Hamiltonian is derived and solved using the variational Monte Carlo approach for $A\\le 4$ nuclei by representing the nuclear many-body wave functions with a symmetry-based artificial neural network. It is found that the relativistic effects rescue the renormalizability of the theory, and overcome the energy collapse problem for $^3$H and $^4$He without promoting a repulsive three-nucleon interaction to leading order as in nonrelativistic calculations. Nevertheless, to exactly reproduce the experimental"},"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":"2206.13208","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2022-06-27T11:50:39Z","cross_cats_sorted":[],"title_canon_sha256":"26cd1d649d4172fbcfbae53741b37ccb9f4fbee0a11beb06c277f9adf22d0b10","abstract_canon_sha256":"dc0084db1302577942fcf2a9b6e05f546ef3a50df7c70df40e56c8d66f14aaa0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:18:47.405871Z","signature_b64":"7StesG6kvFYcgqQqVlwZSsoNMD+diI4cCiFRqVz1vDGUdWQvmKIZggVLX+WAL2FXyLv4OQGoC3WjUheJQcfWCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"52c3896573ea2a64d6588209d81b5b3be8d7ad4fa264b72b33caba163ef88461","last_reissued_at":"2026-07-05T05:18:47.405136Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:18:47.405136Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Relativistic effects and three-body interactions in atomic nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"P. W. Zhao, Y. L. Yang","submitted_at":"2022-06-27T11:50:39Z","abstract_excerpt":"Based on the leading-order covariant pionless effective field theory, a relativistic nuclear Hamiltonian is derived and solved using the variational Monte Carlo approach for $A\\le 4$ nuclei by representing the nuclear many-body wave functions with a symmetry-based artificial neural network. It is found that the relativistic effects rescue the renormalizability of the theory, and overcome the energy collapse problem for $^3$H and $^4$He without promoting a repulsive three-nucleon interaction to leading order as in nonrelativistic calculations. Nevertheless, to exactly reproduce the experimental"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2206.13208","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/2206.13208/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":"2206.13208","created_at":"2026-07-05T05:18:47.405202+00:00"},{"alias_kind":"arxiv_version","alias_value":"2206.13208v1","created_at":"2026-07-05T05:18:47.405202+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2206.13208","created_at":"2026-07-05T05:18:47.405202+00:00"},{"alias_kind":"pith_short_12","alias_value":"KLBYSZLT5IVG","created_at":"2026-07-05T05:18:47.405202+00:00"},{"alias_kind":"pith_short_16","alias_value":"KLBYSZLT5IVGJVSY","created_at":"2026-07-05T05:18:47.405202+00:00"},{"alias_kind":"pith_short_8","alias_value":"KLBYSZLT","created_at":"2026-07-05T05:18:47.405202+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24380","citing_title":"Fully-heavy multiquarks in neural-network quantum states","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP","json":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP.json","graph_json":"https://pith.science/api/pith-number/KLBYSZLT5IVGJVSYQIE5QG23HP/graph.json","events_json":"https://pith.science/api/pith-number/KLBYSZLT5IVGJVSYQIE5QG23HP/events.json","paper":"https://pith.science/paper/KLBYSZLT"},"agent_actions":{"view_html":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP","download_json":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP.json","view_paper":"https://pith.science/paper/KLBYSZLT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2206.13208&json=true","fetch_graph":"https://pith.science/api/pith-number/KLBYSZLT5IVGJVSYQIE5QG23HP/graph.json","fetch_events":"https://pith.science/api/pith-number/KLBYSZLT5IVGJVSYQIE5QG23HP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP/action/storage_attestation","attest_author":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP/action/author_attestation","sign_citation":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP/action/citation_signature","submit_replication":"https://pith.science/pith/KLBYSZLT5IVGJVSYQIE5QG23HP/action/replication_record"}},"created_at":"2026-07-05T05:18:47.405202+00:00","updated_at":"2026-07-05T05:18:47.405202+00:00"}