{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:UVSATCJBTL46DTC3UK56RUMWN7","short_pith_number":"pith:UVSATCJB","schema_version":"1.0","canonical_sha256":"a5640989219af9e1cc5ba2bbe8d1966fc0d4a2b4059cf8510941d7495d598f09","source":{"kind":"arxiv","id":"2406.19193","version":2},"attestation_state":"computed","paper":{"title":"Physical-mass calculation of $\\rho(770)$ and $K^*(892)$ resonance parameters via $\\pi \\pi$ and $K \\pi$ scattering amplitudes from lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Antonin Portelli, Fabian Joswig, Felix Erben, Maxwell T. Hansen, Michael Marshall, Nelson Pitanga Lachini, Peter Boyle, Vera G\\\"ulpers","submitted_at":"2024-06-27T14:12:11Z","abstract_excerpt":"We present our study of the $\\rho(770)$ and $K^*(892)$ resonances from lattice quantum chromodynamics (QCD) employing domain-wall fermions at physical quark masses. We determine the finite-volume energy spectrum in various momentum frames and obtain phase-shift parameterizations via the L\\\"uscher formalism, and as a final step the complex resonance poles of the $\\pi \\pi$ and $K \\pi$ elastic scattering amplitudes via an analytical continuation of the models. By sampling a large number of representative sets of underlying energy-level fits, we also assign a systematic uncertainty to our final re"},"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":"2406.19193","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2024-06-27T14:12:11Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"14508e653fbbbee39bb1aa6b03c8438336a8c0a3a94fde139a580fae26647731","abstract_canon_sha256":"26fd384f87c6076fd71f4a80de910d7f42adac4eace96143b827d5dd6c671a97"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:45:09.532935Z","signature_b64":"L3c2D1v8i8Rq0qJSt50Bz+7atOefyrp1fLHyZh2ce1BG68a9zsmKE5Jd9UBnU3yBcJ0qlsLu/AS2daRPNypmCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5640989219af9e1cc5ba2bbe8d1966fc0d4a2b4059cf8510941d7495d598f09","last_reissued_at":"2026-07-05T10:45:09.532296Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:45:09.532296Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Physical-mass calculation of $\\rho(770)$ and $K^*(892)$ resonance parameters via $\\pi \\pi$ and $K \\pi$ scattering amplitudes from lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Antonin Portelli, Fabian Joswig, Felix Erben, Maxwell T. Hansen, Michael Marshall, Nelson Pitanga Lachini, Peter Boyle, Vera G\\\"ulpers","submitted_at":"2024-06-27T14:12:11Z","abstract_excerpt":"We present our study of the $\\rho(770)$ and $K^*(892)$ resonances from lattice quantum chromodynamics (QCD) employing domain-wall fermions at physical quark masses. We determine the finite-volume energy spectrum in various momentum frames and obtain phase-shift parameterizations via the L\\\"uscher formalism, and as a final step the complex resonance poles of the $\\pi \\pi$ and $K \\pi$ elastic scattering amplitudes via an analytical continuation of the models. By sampling a large number of representative sets of underlying energy-level fits, we also assign a systematic uncertainty to our final re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.19193","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.19193/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":"2406.19193","created_at":"2026-07-05T10:45:09.532398+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.19193v2","created_at":"2026-07-05T10:45:09.532398+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.19193","created_at":"2026-07-05T10:45:09.532398+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVSATCJBTL46","created_at":"2026-07-05T10:45:09.532398+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVSATCJBTL46DTC3","created_at":"2026-07-05T10:45:09.532398+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVSATCJB","created_at":"2026-07-05T10:45:09.532398+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2407.10913","citing_title":"Hybrid calculation of hadronic vacuum polarization in muon g-2 to 0.48\\%","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2603.16266","citing_title":"Lattice QCD study of the $K^*(892)$ resonance at the physical point","ref_index":30,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7","json":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7.json","graph_json":"https://pith.science/api/pith-number/UVSATCJBTL46DTC3UK56RUMWN7/graph.json","events_json":"https://pith.science/api/pith-number/UVSATCJBTL46DTC3UK56RUMWN7/events.json","paper":"https://pith.science/paper/UVSATCJB"},"agent_actions":{"view_html":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7","download_json":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7.json","view_paper":"https://pith.science/paper/UVSATCJB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.19193&json=true","fetch_graph":"https://pith.science/api/pith-number/UVSATCJBTL46DTC3UK56RUMWN7/graph.json","fetch_events":"https://pith.science/api/pith-number/UVSATCJBTL46DTC3UK56RUMWN7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7/action/storage_attestation","attest_author":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7/action/author_attestation","sign_citation":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7/action/citation_signature","submit_replication":"https://pith.science/pith/UVSATCJBTL46DTC3UK56RUMWN7/action/replication_record"}},"created_at":"2026-07-05T10:45:09.532398+00:00","updated_at":"2026-07-05T10:45:09.532398+00:00"}