{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:N2HSN7UGXDWBCDBOCVJEUINJQM","short_pith_number":"pith:N2HSN7UG","schema_version":"1.0","canonical_sha256":"6e8f26fe86b8ec110c2e15524a21a9830c2c0a35a55168d35de3a0ac4a673fa5","source":{"kind":"arxiv","id":"1608.07478","version":1},"attestation_state":"computed","paper":{"title":"Studying the $\\rho$ resonance parameters with staggered fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Lingyun Wang, Ziwen Fu","submitted_at":"2016-08-26T14:51:00Z","abstract_excerpt":"We deliver a lattice study of $\\rho$ resonance parameters with p-wave $\\pi\\pi$ scattering phases, which are extracted by finite-size methods at one center-of-mass frame and four moving frames for six MILC lattice ensembles with pion masses ranging from $346$ to $ 176$ MeV. The effective range formula is applied to describe the scattering phases as a function of the energy covering the resonance region, this allows us to extract $\\rho$ resonance parameters and to investigate the quark-mass dependence. Lattice studies with three flavors of the Asqtad-improved staggered fermions enable us to use "},"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":"1608.07478","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-08-26T14:51:00Z","cross_cats_sorted":[],"title_canon_sha256":"69087cbd87d579834dd90c7bb4d322bcb7d03ae112d1b98af55ef554f1451741","abstract_canon_sha256":"d0728ef98477cc705bd015bf77d863b0b61824f4e0fb5cbab62606e961903579"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:52.947819Z","signature_b64":"CkJJmTNW9I4z6U4YO4CjEbtP6I5SN6qdGjNlelNw0j8VA6Aaatuh0+KgGaAqmkSD9PuKZIxqamFBZ8eXskzbAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6e8f26fe86b8ec110c2e15524a21a9830c2c0a35a55168d35de3a0ac4a673fa5","last_reissued_at":"2026-05-18T01:07:52.947447Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:52.947447Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Studying the $\\rho$ resonance parameters with staggered fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Lingyun Wang, Ziwen Fu","submitted_at":"2016-08-26T14:51:00Z","abstract_excerpt":"We deliver a lattice study of $\\rho$ resonance parameters with p-wave $\\pi\\pi$ scattering phases, which are extracted by finite-size methods at one center-of-mass frame and four moving frames for six MILC lattice ensembles with pion masses ranging from $346$ to $ 176$ MeV. The effective range formula is applied to describe the scattering phases as a function of the energy covering the resonance region, this allows us to extract $\\rho$ resonance parameters and to investigate the quark-mass dependence. Lattice studies with three flavors of the Asqtad-improved staggered fermions enable us to use "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07478","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":"1608.07478","created_at":"2026-05-18T01:07:52.947505+00:00"},{"alias_kind":"arxiv_version","alias_value":"1608.07478v1","created_at":"2026-05-18T01:07:52.947505+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07478","created_at":"2026-05-18T01:07:52.947505+00:00"},{"alias_kind":"pith_short_12","alias_value":"N2HSN7UGXDWB","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"N2HSN7UGXDWBCDBO","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"N2HSN7UG","created_at":"2026-05-18T12:30:32.724797+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.08115","citing_title":"Field-theoretic versus data-driven evaluations of electromagnetic corrections to hadronic vacuum polarization in $(g-2)_\\mu$","ref_index":60,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM","json":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM.json","graph_json":"https://pith.science/api/pith-number/N2HSN7UGXDWBCDBOCVJEUINJQM/graph.json","events_json":"https://pith.science/api/pith-number/N2HSN7UGXDWBCDBOCVJEUINJQM/events.json","paper":"https://pith.science/paper/N2HSN7UG"},"agent_actions":{"view_html":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM","download_json":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM.json","view_paper":"https://pith.science/paper/N2HSN7UG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1608.07478&json=true","fetch_graph":"https://pith.science/api/pith-number/N2HSN7UGXDWBCDBOCVJEUINJQM/graph.json","fetch_events":"https://pith.science/api/pith-number/N2HSN7UGXDWBCDBOCVJEUINJQM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM/action/storage_attestation","attest_author":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM/action/author_attestation","sign_citation":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM/action/citation_signature","submit_replication":"https://pith.science/pith/N2HSN7UGXDWBCDBOCVJEUINJQM/action/replication_record"}},"created_at":"2026-05-18T01:07:52.947505+00:00","updated_at":"2026-05-18T01:07:52.947505+00:00"}