{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:J4ETJDDITHJIN2GU2ZBOAHTHV6","short_pith_number":"pith:J4ETJDDI","schema_version":"1.0","canonical_sha256":"4f09348c6899d286e8d4d642e01e67afa0d20cf4d266b817a0643e540f90b5fe","source":{"kind":"arxiv","id":"1212.1105","version":1},"attestation_state":"computed","paper":{"title":"Electromagnetic structure of A=2 and 3 nuclei in chiral effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"L. E. Marcucci, L. Girlanda, M. Piarulli, M. Viviani, R. Schiavilla, S. Pastore","submitted_at":"2012-12-05T17:20:36Z","abstract_excerpt":"The objectives of the present work are twofold. The first is to address and resolve some of the differences present in independent, chiral-effective-field-theory (\\chiEFT) derivations up to one loop, recently appeared in the literature, of the nuclear charge and current operators. The second objective is to provide a complete set of \\chiEFT predictions for the structure functions and tensor polarization of the deuteron, for the charge and magnetic form factors of 3He and 3H, and for the charge and magnetic radii of these few-nucleon systems. The calculations use wave functions derived from hig"},"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":"1212.1105","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-12-05T17:20:36Z","cross_cats_sorted":[],"title_canon_sha256":"47b6d33f3379c1afb95257ccb0632cf53d6e0c510678ba22dd85f1ac5318d31b","abstract_canon_sha256":"446a8486c5d7e16053af8b761110ee1bd3fe29e3a38111b63166065cfbcc27bc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:47.356994Z","signature_b64":"GPj59RhtbIrcu06OJiotAVC0TMt9bEiqQe/Y9mVI97oq72Rq81Am1WOCr2RACdpDjGklVHm2KDEfPNgeW49MBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f09348c6899d286e8d4d642e01e67afa0d20cf4d266b817a0643e540f90b5fe","last_reissued_at":"2026-05-18T01:52:47.356620Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:47.356620Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic structure of A=2 and 3 nuclei in chiral effective field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"L. E. Marcucci, L. Girlanda, M. Piarulli, M. Viviani, R. Schiavilla, S. Pastore","submitted_at":"2012-12-05T17:20:36Z","abstract_excerpt":"The objectives of the present work are twofold. The first is to address and resolve some of the differences present in independent, chiral-effective-field-theory (\\chiEFT) derivations up to one loop, recently appeared in the literature, of the nuclear charge and current operators. The second objective is to provide a complete set of \\chiEFT predictions for the structure functions and tensor polarization of the deuteron, for the charge and magnetic form factors of 3He and 3H, and for the charge and magnetic radii of these few-nucleon systems. The calculations use wave functions derived from hig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.1105","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":"1212.1105","created_at":"2026-05-18T01:52:47.356677+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.1105v1","created_at":"2026-05-18T01:52:47.356677+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.1105","created_at":"2026-05-18T01:52:47.356677+00:00"},{"alias_kind":"pith_short_12","alias_value":"J4ETJDDITHJI","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"J4ETJDDITHJIN2GU","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"J4ETJDDI","created_at":"2026-05-18T12:27:09.501522+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/J4ETJDDITHJIN2GU2ZBOAHTHV6","json":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6.json","graph_json":"https://pith.science/api/pith-number/J4ETJDDITHJIN2GU2ZBOAHTHV6/graph.json","events_json":"https://pith.science/api/pith-number/J4ETJDDITHJIN2GU2ZBOAHTHV6/events.json","paper":"https://pith.science/paper/J4ETJDDI"},"agent_actions":{"view_html":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6","download_json":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6.json","view_paper":"https://pith.science/paper/J4ETJDDI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.1105&json=true","fetch_graph":"https://pith.science/api/pith-number/J4ETJDDITHJIN2GU2ZBOAHTHV6/graph.json","fetch_events":"https://pith.science/api/pith-number/J4ETJDDITHJIN2GU2ZBOAHTHV6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6/action/storage_attestation","attest_author":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6/action/author_attestation","sign_citation":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6/action/citation_signature","submit_replication":"https://pith.science/pith/J4ETJDDITHJIN2GU2ZBOAHTHV6/action/replication_record"}},"created_at":"2026-05-18T01:52:47.356677+00:00","updated_at":"2026-05-18T01:52:47.356677+00:00"}