{"as_of":"2026-07-19T00:51:00Z","canonical_paper_id":"2IRNVFPC","canonical_url":"https://pith.science/paper/2IRNVFPC/integrity","context_digest":"sha256:f128f21dddf2a0c9f765fdb08f641225d45e929a29766ea0d9895d663337610f","coverage_summary":[],"findings":[],"findings_empty_copy":"No checks are listed for this paper yet.","findings_observation_state":"no_listed_checks","links":{"arxiv":"https://arxiv.org/abs/1612.09081","bundle_json":"/pith/2IRNVFPCYS442HD7JYEHQZXQIX/bundle.json","citation_record":"/paper/2IRNVFPC/citation-record","evidence":"/evidence","html":"/paper/2IRNVFPC/integrity","integrity_json":"/paper/2IRNVFPC/integrity.json","json":"/paper/2IRNVFPC/integrity.json","legacy_integrity_json":"/pith/2IRNVFPC/integrity.json","paper":"/paper/2IRNVFPC","reference_changes":"/flags?citing=2IRNVFPC"},"paper":{"arxiv_id":"1612.09081","latest_version":1,"primary_cat":"hep-lat","title":"Heavy-heavy current improvement for calculation of $\\bar{B}\\rightarrow D^{(*)}\\ell \\bar{\\nu}$ semi-leptonic form factors using the Oktay-Kronfeld action"},"pith_number":"pith:2016:2IRNVFPCYS442HD7JYEHQZXQIX","pith_short":"2IRNVFPCYS442HD7JYEHQZXQIX","record":{"arxiv_id":"1612.09081","claim":"As of an unrecorded date, Pith completed 0 of 0 listed checks against arXiv:1612.09081. No listed check completed, so this record makes no findings claim.","counts":{"completed":0,"failed":0,"listed":0,"not_collected":0,"not_requested":0,"partial":0,"public_findings_from_completed":0,"skipped":0,"unavailable":0,"withheld":0},"coverage":[],"observed_at":null,"refusal":"This is a record of named checks, not a clean-status claim or a paper verdict.","schema":"pith.integrity.v1"},"schema":"pith.paper-integrity-record.v1","species":"LEDGER"}