{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:3JW5VZRNY22S7KZBUDMCUCWMNR","short_pith_number":"pith:3JW5VZRN","schema_version":"1.0","canonical_sha256":"da6ddae62dc6b52fab21a0d82a0acc6c71994bfbad1d4309415e55154baf31b6","source":{"kind":"arxiv","id":"1709.05080","version":1},"attestation_state":"computed","paper":{"title":"$J/{\\psi}$ ${\\to}$ $D_{s,d}{\\pi}$, $D_{s,d}K$ decays with perturbative QCD approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Gongru Lu, Jie Gao, Jinshu Huang, Junfeng Sun, Qin Chang, Yueling Yang","submitted_at":"2017-09-15T07:21:44Z","abstract_excerpt":"Besides the conventional strong and electromagnetic decay modes, the $J/{\\psi}$ particle can also decay via the weak interaction in the standard model. In this paper, nonleptonic $J/{\\psi}$ ${\\to}$ $D_{s,d}{\\pi}$, $D_{s,d}K$ weak decays, corresponding to the externally emitted virtual $W$ boson process, are investigated with the perturbative QCD approach. It is found that branching ratio for the Cabibbo-favored $J/{\\psi}$ ${\\to}$ $D_{s}{\\pi}$ decay can reach up to ${\\cal O}(10^{-10})$, which might be potentially measurable at the future high-luminosity experiments."},"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":"1709.05080","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2017-09-15T07:21:44Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"0ce7a95a8f78a4dd78eaba980d3425f60c3864db1d2c61d2c45b888e97c2f134","abstract_canon_sha256":"0b402b95b6fd769e892e933587c10f7fefd83d2c0eb7ac778ab45a1f6b6d4ce3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:03.310763Z","signature_b64":"KtDfZudmsYTM5JzH0whGqpWux0yn0yHtPbH7w6acv8mSc2AiuI3WA5SDlUEiLJQfMR98+47si+Q9bpR3WsDnBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"da6ddae62dc6b52fab21a0d82a0acc6c71994bfbad1d4309415e55154baf31b6","last_reissued_at":"2026-05-18T00:35:03.310038Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:03.310038Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$J/{\\psi}$ ${\\to}$ $D_{s,d}{\\pi}$, $D_{s,d}K$ decays with perturbative QCD approach","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Gongru Lu, Jie Gao, Jinshu Huang, Junfeng Sun, Qin Chang, Yueling Yang","submitted_at":"2017-09-15T07:21:44Z","abstract_excerpt":"Besides the conventional strong and electromagnetic decay modes, the $J/{\\psi}$ particle can also decay via the weak interaction in the standard model. In this paper, nonleptonic $J/{\\psi}$ ${\\to}$ $D_{s,d}{\\pi}$, $D_{s,d}K$ weak decays, corresponding to the externally emitted virtual $W$ boson process, are investigated with the perturbative QCD approach. It is found that branching ratio for the Cabibbo-favored $J/{\\psi}$ ${\\to}$ $D_{s}{\\pi}$ decay can reach up to ${\\cal O}(10^{-10})$, which might be potentially measurable at the future high-luminosity experiments."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.05080","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":"1709.05080","created_at":"2026-05-18T00:35:03.310161+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.05080v1","created_at":"2026-05-18T00:35:03.310161+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.05080","created_at":"2026-05-18T00:35:03.310161+00:00"},{"alias_kind":"pith_short_12","alias_value":"3JW5VZRNY22S","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"3JW5VZRNY22S7KZB","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"3JW5VZRN","created_at":"2026-05-18T12:30:58.224056+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.13456","citing_title":"$D_{(s)}(2S)$ and $D^{*}_{(s)}(2S)$ production in nonleptonic $B_{(s)}$ weak decays","ref_index":83,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR","json":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR.json","graph_json":"https://pith.science/api/pith-number/3JW5VZRNY22S7KZBUDMCUCWMNR/graph.json","events_json":"https://pith.science/api/pith-number/3JW5VZRNY22S7KZBUDMCUCWMNR/events.json","paper":"https://pith.science/paper/3JW5VZRN"},"agent_actions":{"view_html":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR","download_json":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR.json","view_paper":"https://pith.science/paper/3JW5VZRN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.05080&json=true","fetch_graph":"https://pith.science/api/pith-number/3JW5VZRNY22S7KZBUDMCUCWMNR/graph.json","fetch_events":"https://pith.science/api/pith-number/3JW5VZRNY22S7KZBUDMCUCWMNR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR/action/storage_attestation","attest_author":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR/action/author_attestation","sign_citation":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR/action/citation_signature","submit_replication":"https://pith.science/pith/3JW5VZRNY22S7KZBUDMCUCWMNR/action/replication_record"}},"created_at":"2026-05-18T00:35:03.310161+00:00","updated_at":"2026-05-18T00:35:03.310161+00:00"}