{"schema":"https://pith.science/schemas/pith-integrity/v1.json","pith_number":"2604.23298","arxiv_id":"2604.23298","integrity":{"available":true,"endpoint":"/pith/2604.23298/integrity.json","summary":{"critical":1,"advisory":0,"informational":0,"by_detector":{"doi_compliance":{"total":1,"critical":1,"advisory":0,"informational":0}}},"clean":false,"detectors_run":[{"name":"doi_compliance","version":"1.0.0","status":"completed","ran_at":"2026-05-19T23:16:33.348703Z","findings_count":1}],"findings":[{"detector":"doi_compliance","finding_type":"unresolvable_identifier","severity":"critical","verdict_class":"cross_source","note":"Identifier '10.5072/zenodo.484495' is syntactically valid but the DOI registry (doi.org) returned 404, and Crossref / OpenAlex / internal corpus also have no record. The cited work could not be located through any authoritative source.","detected_doi":"10.5072/zenodo.484495","detected_arxiv_id":null,"ref_index":1,"audited_at":"2026-05-19T23:16:33.348703Z"}],"snapshot_sha256":"f82f0838175d19dc8a808b78319aff22e1e315e407129ec14e5da76110e52c5a"},"events":[{"event_id":3605,"event_type":"pith.integrity.v1","payload_sha256":"b8ec3926bba7e508b4ecb1f05294a68c4cb85fcb5f08a13ce12f7a8b6164cd84","signature_b64":"LWIwTR9iK5HCGPUhguygxLtDcGr9FyC07QJ0RcxyLC7cIkCMJ0Nb9u2JP9QCDIs6AHHikr9Vqq/LhnOj9G07Dg==","signing_key_id":"pith-v1-2026-05","created_at":"2026-05-19T23:17:27.293231+00:00","payload":{"note":"Identifier '10.5072/zenodo.484495' is syntactically valid but the DOI registry (doi.org) returned 404, and Crossref / OpenAlex / internal corpus also have no record. The cited work could not be located through any authoritative source.","snippet":"Due to Bose-Einstein statistics, the isospin for the subsystem of two identityDmesons can be ony 1. In the expression, we have already set the total isospin toT= 1 2. Considering the spin quantum numbers:J(D) = 0and J(K) = 0, the spin partS","arxiv_id":"2604.23298","detector":"doi_compliance","evidence":{"doi":"10.5072/zenodo.484495","arxiv_id":null,"ref_index":1,"raw_excerpt":"Due to Bose-Einstein statistics, the isospin for the subsystem of two identityDmesons can be ony 1. In the expression, we have already set the total isospin toT= 1 2. Considering the spin quantum numbers:J(D) = 0and J(K) = 0, the spin partS JM of theDDKsystem is trivial. ForJ(D ∗) = 1, the spin partS JM of theD ∗D∗Ksystem can be expressed as SJM =S 00 = 1√ 3 |1−1⟩+ 1√ 3 |−1 1⟩ − 1√ 3 |0 0⟩,(21) wh","verdict_class":"cross_source","checked_sources":["crossref_by_doi","openalex_by_doi","doi_org_head"]},"severity":"critical","ref_index":1,"audited_at":"2026-05-19T23:16:33.348703Z","event_type":"pith.integrity.v1","detected_doi":"10.5072/zenodo.484495","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"unresolvable_identifier","evidence_hash":"fb7e6117eb83e630886a08e05d765006d2092d74be2f69869b38d6ff0fa72bfd","paper_version":1,"verdict_class":"cross_source","resolved_title":null,"detector_version":"1.0.0","detected_arxiv_id":null}}],"endpoint_self":"/pith/2604.23298/integrity.json","protocol_url":"https://pith.science/pith-integrity-protocol"}