{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:ONRIPRI6MFH542O5VJXF3SCIOZ","short_pith_number":"pith:ONRIPRI6","schema_version":"1.0","canonical_sha256":"736287c51e614fde69ddaa6e5dc848767d80edb6f6c1dfadd4df2343cd7f1528","source":{"kind":"arxiv","id":"0909.5414","version":1},"attestation_state":"computed","paper":{"title":"Subtractive renormalization of chiral effective theory NN potentials up to next-to-next-to-leading order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ch. Elster, C.-J. Yang, D. R. Phillips","submitted_at":"2009-09-29T19:44:32Z","abstract_excerpt":"We have developed a subtractive renormalization method with which we can evaluate nucleon-nucleon (NN) scattering phase shifts produced by the NN potential obtained at leading, next-to-leading, and next-to-next-to-leading order (NNLO) in chiral effective theory ($\\chi$ET). In this method the low-energy constants associated with short-distance NN physics are eliminated from the Lippmann-Schwinger equation (LSE) for the NN t-matrix, in favor of physical observables. This allows us to straightforwardly compute scattering phase shifts for ultra-violet cutoffs of at least 10 GeV. We then perform de"},"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":"0909.5414","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2009-09-29T19:44:32Z","cross_cats_sorted":[],"title_canon_sha256":"1411e4cad39ef5e0af879f08e69aa3177b0f2b84932d02e991402d31a08d218b","abstract_canon_sha256":"4d036cb98d86b8879b4690adddde15cf9c952ec6ac9fbcf503b55acd7d58ce54"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:20.791577Z","signature_b64":"i8hU+BBt2Pagg//ifhWqs/IWksF0TtG6agfDCB1u9uMayceBxpYgIZLR4EaRTqai2snaSd0n+iBiscCfxTWZAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"736287c51e614fde69ddaa6e5dc848767d80edb6f6c1dfadd4df2343cd7f1528","last_reissued_at":"2026-05-18T02:34:20.791074Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:20.791074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Subtractive renormalization of chiral effective theory NN potentials up to next-to-next-to-leading order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Ch. Elster, C.-J. Yang, D. R. Phillips","submitted_at":"2009-09-29T19:44:32Z","abstract_excerpt":"We have developed a subtractive renormalization method with which we can evaluate nucleon-nucleon (NN) scattering phase shifts produced by the NN potential obtained at leading, next-to-leading, and next-to-next-to-leading order (NNLO) in chiral effective theory ($\\chi$ET). In this method the low-energy constants associated with short-distance NN physics are eliminated from the Lippmann-Schwinger equation (LSE) for the NN t-matrix, in favor of physical observables. This allows us to straightforwardly compute scattering phase shifts for ultra-violet cutoffs of at least 10 GeV. We then perform de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0909.5414","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":"0909.5414","created_at":"2026-05-18T02:34:20.791149+00:00"},{"alias_kind":"arxiv_version","alias_value":"0909.5414v1","created_at":"2026-05-18T02:34:20.791149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0909.5414","created_at":"2026-05-18T02:34:20.791149+00:00"},{"alias_kind":"pith_short_12","alias_value":"ONRIPRI6MFH5","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"ONRIPRI6MFH542O5","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"ONRIPRI6","created_at":"2026-05-18T12:26:01.383474+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/ONRIPRI6MFH542O5VJXF3SCIOZ","json":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ.json","graph_json":"https://pith.science/api/pith-number/ONRIPRI6MFH542O5VJXF3SCIOZ/graph.json","events_json":"https://pith.science/api/pith-number/ONRIPRI6MFH542O5VJXF3SCIOZ/events.json","paper":"https://pith.science/paper/ONRIPRI6"},"agent_actions":{"view_html":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ","download_json":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ.json","view_paper":"https://pith.science/paper/ONRIPRI6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0909.5414&json=true","fetch_graph":"https://pith.science/api/pith-number/ONRIPRI6MFH542O5VJXF3SCIOZ/graph.json","fetch_events":"https://pith.science/api/pith-number/ONRIPRI6MFH542O5VJXF3SCIOZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ/action/storage_attestation","attest_author":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ/action/author_attestation","sign_citation":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ/action/citation_signature","submit_replication":"https://pith.science/pith/ONRIPRI6MFH542O5VJXF3SCIOZ/action/replication_record"}},"created_at":"2026-05-18T02:34:20.791149+00:00","updated_at":"2026-05-18T02:34:20.791149+00:00"}