{"schema":"https://pith.science/schemas/pith-integrity/v1.json","pith_number":"2605.15948","arxiv_id":"2605.15948","integrity":{"available":true,"endpoint":"/pith/2605.15948/integrity.json","summary":{"critical":0,"advisory":1,"informational":0,"by_detector":{"doi_compliance":{"total":1,"critical":0,"advisory":1,"informational":0}}},"clean":false,"detectors_run":[{"name":"doi_compliance","version":"1.0.0","status":"completed","ran_at":"2026-05-20T17:02:51.175888Z","findings_count":1},{"name":"claim_evidence","version":"1.0.0","status":"completed","ran_at":"2026-05-20T17:02:07.688307Z","findings_count":0},{"name":"doi_title_agreement","version":"1.0.0","status":"completed","ran_at":"2026-05-20T17:01:25.608142Z","findings_count":0},{"name":"ai_meta_artifact","version":"1.0.0","status":"skipped","ran_at":"2026-05-19T17:33:44.882776Z","findings_count":0}],"findings":[{"detector":"doi_compliance","finding_type":"recoverable_identifier","severity":"advisory","verdict_class":"incontrovertible","note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1016/0550-3213(88) was visible in the surrounding text but could not be confirmed against doi.org as printed.","detected_doi":"10.1016/0550-3213(88","detected_arxiv_id":null,"ref_index":59,"audited_at":"2026-05-20T17:02:51.175888Z"}],"snapshot_sha256":"c0fa45e627d9309cd43ee126136fac8820842d4bad26d462ccb46567b51f9e16"},"events":[{"event_id":5292,"event_type":"pith.integrity.v1","payload_sha256":"725adcb12a9eee0ddd59ab4d3ef4b0c2530d4ccd926b27653cb22f4de22544a6","signature_b64":"cDiZb+nq6Z/RisLJdsPMCuHCcHPzq/LF7eLMgW/D+TfYE8P32omQcNjVy8o/RYWSyaLveFjP7HexI+4nciwzAA==","signing_key_id":"pith-v1-2026-05","created_at":"2026-05-20T17:03:16.485160+00:00","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1016/0550-3213(88) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"S. Y. Khlebnikov and M. E. Shaposhnikov, “The Statistical Theory of Anomalous Fermion Number Nonconservation,” Nucl. Phys. B308, 885 (1988) doi:10.1016/0550- 3213(88)90133-2","arxiv_id":"2605.15948","detector":"doi_compliance","evidence":{"ref_index":59,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"S. Y. Khlebnikov and M. E. Shaposhnikov, “The Statistical Theory of Anomalous Fermion Number Nonconservation,” Nucl. Phys. B308, 885 (1988) doi:10.1016/0550- 3213(88)90133-2","reconstructed_doi":"10.1016/0550-3213(88"},"severity":"advisory","ref_index":59,"audited_at":"2026-05-20T17:02:51.175888Z","event_type":"pith.integrity.v1","detected_doi":"10.1016/0550-3213(88","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"28e57261dfee2f12ee7cf2eced28146c4ed0d26ac9fa1d1da35a9c99863b35f0","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.0.0","detected_arxiv_id":null}}],"endpoint_self":"/pith/2605.15948/integrity.json","protocol_url":"https://pith.science/pith-integrity-protocol"}