{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:BL6MSCOVE73I2IRZV4I4FBEJBR","short_pith_number":"pith:BL6MSCOV","schema_version":"1.0","canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","source":{"kind":"arxiv","id":"2505.05960","version":1},"attestation_state":"computed","paper":{"title":"The light meson decays of $D$ wave charmonia","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Xiao-Yu Qi, Xing-Dao Guo","submitted_at":"2025-05-09T11:21:34Z","abstract_excerpt":"Motivated by the large non-$D\\bar{D}$ branching fraction of $\\psi(3770)$, we investigate the light meson decays of the $D$-wave charmonia in the present work with the meson loop mechanism. With the parameter range determined by $\\psi (3770) \\to \\phi \\eta$, our estimations of the branching fractions of the light meson decays of $\\psi(3770)$ are consistent with the estimations in the literature. As for $\\psi(3823)$, the partial widths of $K^\\ast \\bar{K}^\\ast$ channel is estimated to be around 200 keV, which is the the predominant light meson decay channel of $\\psi(3823)$. Our estimations also in"},"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":"2505.05960","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-09T11:21:34Z","cross_cats_sorted":[],"title_canon_sha256":"33eac8cb92553dc4bc01363b15c6f361175210cbbd01b4d427128782a0a793f9","abstract_canon_sha256":"6ce00746fc7751b02689ddae8f07efae3047876fb0124f15ab54541e4b6f3ba9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:00:50.856076Z","signature_b64":"BrS168HWnUIrlQZIJiYdEmNrS021y3ndCVNG7zrZWIK04xtZVLNGwLnqY/R/Jjv5Izm4cICVmmRLFgZ8KPcxBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","last_reissued_at":"2026-07-05T11:00:50.855483Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:00:50.855483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The light meson decays of $D$ wave charmonia","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Dian-Yong Chen, Xiao-Yu Qi, Xing-Dao Guo","submitted_at":"2025-05-09T11:21:34Z","abstract_excerpt":"Motivated by the large non-$D\\bar{D}$ branching fraction of $\\psi(3770)$, we investigate the light meson decays of the $D$-wave charmonia in the present work with the meson loop mechanism. With the parameter range determined by $\\psi (3770) \\to \\phi \\eta$, our estimations of the branching fractions of the light meson decays of $\\psi(3770)$ are consistent with the estimations in the literature. As for $\\psi(3823)$, the partial widths of $K^\\ast \\bar{K}^\\ast$ channel is estimated to be around 200 keV, which is the the predominant light meson decay channel of $\\psi(3823)$. Our estimations also in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.05960","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.05960/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2505.05960","created_at":"2026-07-05T11:00:50.855545+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.05960v1","created_at":"2026-07-05T11:00:50.855545+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.05960","created_at":"2026-07-05T11:00:50.855545+00:00"},{"alias_kind":"pith_short_12","alias_value":"BL6MSCOVE73I","created_at":"2026-07-05T11:00:50.855545+00:00"},{"alias_kind":"pith_short_16","alias_value":"BL6MSCOVE73I2IRZ","created_at":"2026-07-05T11:00:50.855545+00:00"},{"alias_kind":"pith_short_8","alias_value":"BL6MSCOV","created_at":"2026-07-05T11:00:50.855545+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR","json":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR.json","graph_json":"https://pith.science/api/pith-number/BL6MSCOVE73I2IRZV4I4FBEJBR/graph.json","events_json":"https://pith.science/api/pith-number/BL6MSCOVE73I2IRZV4I4FBEJBR/events.json","paper":"https://pith.science/paper/BL6MSCOV"},"agent_actions":{"view_html":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR","download_json":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR.json","view_paper":"https://pith.science/paper/BL6MSCOV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.05960&json=true","fetch_graph":"https://pith.science/api/pith-number/BL6MSCOVE73I2IRZV4I4FBEJBR/graph.json","fetch_events":"https://pith.science/api/pith-number/BL6MSCOVE73I2IRZV4I4FBEJBR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/action/storage_attestation","attest_author":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/action/author_attestation","sign_citation":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/action/citation_signature","submit_replication":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/action/replication_record"}},"created_at":"2026-07-05T11:00:50.855545+00:00","updated_at":"2026-07-05T11:00:50.855545+00:00"}