{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:TDI2FAR4J7G2JICNBLXX7IEZI4","short_pith_number":"pith:TDI2FAR4","schema_version":"1.0","canonical_sha256":"98d1a2823c4fcda4a04d0aef7fa09947039f746cca9e9c4c4234e4b804e4d42a","source":{"kind":"arxiv","id":"1508.00886","version":2},"attestation_state":"computed","paper":{"title":"Two-Nucleon Higher Partial-Wave Scattering from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Amy Nicholson, Andre Walker-Loud, Balint Joo, Enrico Rinaldi, Evan Berkowitz, Mark Strother, Pavlos M. Vranas, Thorsten Kurth","submitted_at":"2015-08-04T19:47:31Z","abstract_excerpt":"We present a determination of nucleon-nucleon scattering phase shifts for l >= 0. The S, P, D and F phase shifts for both the spin-triplet and spin-singlet channels are computed with lattice Quantum ChromoDynamics. For l > 0, this is the first lattice QCD calculation using the Luscher finite-volume formalism. This required the design and implementation of novel lattice methods involving displaced sources and momentum-space cubic sinks. To demonstrate the utility of our approach, the calculations were performed in the SU(3)-flavor limit where the light quark masses have been tuned to the physic"},"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":"1508.00886","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-08-04T19:47:31Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"36f9810c265f8a923512239424c680fdca2e967cc1eb9133aa0c7717f5c8b9ca","abstract_canon_sha256":"89093c0dea9f38e20f2a81c772734579afb0fa5668e47cad8b2ba342e01c25cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:03.809196Z","signature_b64":"4AjpWJUfks3Ae34DLKT6kI4YKIxYwQXSl0W+t5akc+qsKITBggIawkpXuCggekKWYmHhyTQUvuKPQTeLkM4pBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"98d1a2823c4fcda4a04d0aef7fa09947039f746cca9e9c4c4234e4b804e4d42a","last_reissued_at":"2026-05-18T00:54:03.808699Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:03.808699Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-Nucleon Higher Partial-Wave Scattering from Lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Amy Nicholson, Andre Walker-Loud, Balint Joo, Enrico Rinaldi, Evan Berkowitz, Mark Strother, Pavlos M. Vranas, Thorsten Kurth","submitted_at":"2015-08-04T19:47:31Z","abstract_excerpt":"We present a determination of nucleon-nucleon scattering phase shifts for l >= 0. The S, P, D and F phase shifts for both the spin-triplet and spin-singlet channels are computed with lattice Quantum ChromoDynamics. For l > 0, this is the first lattice QCD calculation using the Luscher finite-volume formalism. This required the design and implementation of novel lattice methods involving displaced sources and momentum-space cubic sinks. To demonstrate the utility of our approach, the calculations were performed in the SU(3)-flavor limit where the light quark masses have been tuned to the physic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.00886","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":"1508.00886","created_at":"2026-05-18T00:54:03.808765+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.00886v2","created_at":"2026-05-18T00:54:03.808765+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.00886","created_at":"2026-05-18T00:54:03.808765+00:00"},{"alias_kind":"pith_short_12","alias_value":"TDI2FAR4J7G2","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"TDI2FAR4J7G2JICN","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"TDI2FAR4","created_at":"2026-05-18T12:29:42.218222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.16977","citing_title":"Two-nucleon systems at $m_{\\pi}\\approx292$ MeV from lattice QCD","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4","json":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4.json","graph_json":"https://pith.science/api/pith-number/TDI2FAR4J7G2JICNBLXX7IEZI4/graph.json","events_json":"https://pith.science/api/pith-number/TDI2FAR4J7G2JICNBLXX7IEZI4/events.json","paper":"https://pith.science/paper/TDI2FAR4"},"agent_actions":{"view_html":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4","download_json":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4.json","view_paper":"https://pith.science/paper/TDI2FAR4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.00886&json=true","fetch_graph":"https://pith.science/api/pith-number/TDI2FAR4J7G2JICNBLXX7IEZI4/graph.json","fetch_events":"https://pith.science/api/pith-number/TDI2FAR4J7G2JICNBLXX7IEZI4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4/action/storage_attestation","attest_author":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4/action/author_attestation","sign_citation":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4/action/citation_signature","submit_replication":"https://pith.science/pith/TDI2FAR4J7G2JICNBLXX7IEZI4/action/replication_record"}},"created_at":"2026-05-18T00:54:03.808765+00:00","updated_at":"2026-05-18T00:54:03.808765+00:00"}