{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:OTU7CJ3SCPHA4VX6U7E3WDRZVB","short_pith_number":"pith:OTU7CJ3S","schema_version":"1.0","canonical_sha256":"74e9f1277213ce0e56fea7c9bb0e39a84306ee453048710a7b40c3187facaa38","source":{"kind":"arxiv","id":"1703.05454","version":2},"attestation_state":"computed","paper":{"title":"High-quality two-nucleon potentials up to fifth order of the chiral expansion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"D. R. Entem, R. Machleidt, Y. Nosyk","submitted_at":"2017-03-16T02:09:28Z","abstract_excerpt":"We present NN potentials through five orders of chiral effective field theory ranging from leading order (LO) to next-to-next-to-next-to-next-to-leading order (N4LO). The construction may be perceived as consistent in the sense that the same power counting scheme as well as the same cutoff procedures are applied in all orders. Moreover, the long-range parts of these potentials are fixed by the very accurate pi-N LECs as determined in the Roy-Steiner equations analysis by Hoferichter, Ruiz de Elvira and coworkers. In fact, the uncertainties of these LECs are so small that a variation within the"},"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":"1703.05454","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-03-16T02:09:28Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"74cbae844f72c3d4fb306a3813ea28ba8f7d14a0ac92f466537e3d09bffdfa64","abstract_canon_sha256":"d1ab071974931dce95003220cd556b6da5b7b60577fa9eaf2b9bfa89888307da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:03.339104Z","signature_b64":"PT094sXAeC+8FGOdYUi9JnFiUfGoC5mcD2s0aqPkGVjs8HSNRvsgunt1cIqfo4ZuiLqKUHdbBbBByccVLqCLDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"74e9f1277213ce0e56fea7c9bb0e39a84306ee453048710a7b40c3187facaa38","last_reissued_at":"2026-05-18T00:38:03.338622Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:03.338622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High-quality two-nucleon potentials up to fifth order of the chiral expansion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"D. R. Entem, R. Machleidt, Y. Nosyk","submitted_at":"2017-03-16T02:09:28Z","abstract_excerpt":"We present NN potentials through five orders of chiral effective field theory ranging from leading order (LO) to next-to-next-to-next-to-next-to-leading order (N4LO). The construction may be perceived as consistent in the sense that the same power counting scheme as well as the same cutoff procedures are applied in all orders. Moreover, the long-range parts of these potentials are fixed by the very accurate pi-N LECs as determined in the Roy-Steiner equations analysis by Hoferichter, Ruiz de Elvira and coworkers. In fact, the uncertainties of these LECs are so small that a variation within the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.05454","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":"1703.05454","created_at":"2026-05-18T00:38:03.338695+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.05454v2","created_at":"2026-05-18T00:38:03.338695+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.05454","created_at":"2026-05-18T00:38:03.338695+00:00"},{"alias_kind":"pith_short_12","alias_value":"OTU7CJ3SCPHA","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_16","alias_value":"OTU7CJ3SCPHA4VX6","created_at":"2026-05-18T12:31:34.259226+00:00"},{"alias_kind":"pith_short_8","alias_value":"OTU7CJ3S","created_at":"2026-05-18T12:31:34.259226+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"1906.10912","citing_title":"Coarse graining hadronic scattering","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2510.22648","citing_title":"Nucleon-nucleon scattering up to next-to-leading order in manifestly Lorentz-invariant chiral effective field theory: low phases and the deuteron","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2512.14117","citing_title":"Scrutiny of the new class of three-nucleon forces","ref_index":67,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB","json":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB.json","graph_json":"https://pith.science/api/pith-number/OTU7CJ3SCPHA4VX6U7E3WDRZVB/graph.json","events_json":"https://pith.science/api/pith-number/OTU7CJ3SCPHA4VX6U7E3WDRZVB/events.json","paper":"https://pith.science/paper/OTU7CJ3S"},"agent_actions":{"view_html":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB","download_json":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB.json","view_paper":"https://pith.science/paper/OTU7CJ3S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.05454&json=true","fetch_graph":"https://pith.science/api/pith-number/OTU7CJ3SCPHA4VX6U7E3WDRZVB/graph.json","fetch_events":"https://pith.science/api/pith-number/OTU7CJ3SCPHA4VX6U7E3WDRZVB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB/action/storage_attestation","attest_author":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB/action/author_attestation","sign_citation":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB/action/citation_signature","submit_replication":"https://pith.science/pith/OTU7CJ3SCPHA4VX6U7E3WDRZVB/action/replication_record"}},"created_at":"2026-05-18T00:38:03.338695+00:00","updated_at":"2026-05-18T00:38:03.338695+00:00"}