{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:BL6MSCOVE73I2IRZV4I4FBEJBR","short_pith_number":"pith:BL6MSCOV","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"},"canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","source":{"kind":"arxiv","id":"2505.05960","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.05960","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"arxiv_version","alias_value":"2505.05960v1","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.05960","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_12","alias_value":"BL6MSCOVE73I","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_16","alias_value":"BL6MSCOVE73I2IRZ","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_8","alias_value":"BL6MSCOV","created_at":"2026-07-05T11:00:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:BL6MSCOVE73I2IRZV4I4FBEJBR","target":"record","payload":{"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"},"canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","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"},"source_kind":"arxiv","source_id":"2505.05960","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:00:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iJQ743Jk3THDAfJlZYcu59fKT18FHFa/oeBf1yRXLOdomF6Bap/FZovQMNOs1u3LAMPcTEouW7SClUDKQACUAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T13:07:00.918971Z"},"content_sha256":"a7e9740348756bd9438be25bb2820ff699ea035571769ff1419fd46e6164ce1a","schema_version":"1.0","event_id":"sha256:a7e9740348756bd9438be25bb2820ff699ea035571769ff1419fd46e6164ce1a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:BL6MSCOVE73I2IRZV4I4FBEJBR","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:00:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ab25PPCXZk3q+eyWOzlCWX4QYWdzAz1u+frFwCSr3QbzTQSsgPCkbDAQCL8V6vH6FjhJQTuuq4DEUn/B/g1/Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T13:07:00.919979Z"},"content_sha256":"442cd852b0f4883026438a1af5334b0ab9af9a3a0517536a72a5e5034cd91e01","schema_version":"1.0","event_id":"sha256:442cd852b0f4883026438a1af5334b0ab9af9a3a0517536a72a5e5034cd91e01"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/bundle.json","state_url":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-06T13:07:00Z","links":{"resolver":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR","bundle":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/bundle.json","state":"https://pith.science/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BL6MSCOVE73I2IRZV4I4FBEJBR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:BL6MSCOVE73I2IRZV4I4FBEJBR","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"6ce00746fc7751b02689ddae8f07efae3047876fb0124f15ab54541e4b6f3ba9","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-09T11:21:34Z","title_canon_sha256":"33eac8cb92553dc4bc01363b15c6f361175210cbbd01b4d427128782a0a793f9"},"schema_version":"1.0","source":{"id":"2505.05960","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2505.05960","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"arxiv_version","alias_value":"2505.05960v1","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.05960","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_12","alias_value":"BL6MSCOVE73I","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_16","alias_value":"BL6MSCOVE73I2IRZ","created_at":"2026-07-05T11:00:50Z"},{"alias_kind":"pith_short_8","alias_value":"BL6MSCOV","created_at":"2026-07-05T11:00:50Z"}],"graph_snapshots":[{"event_id":"sha256:442cd852b0f4883026438a1af5334b0ab9af9a3a0517536a72a5e5034cd91e01","target":"graph","created_at":"2026-07-05T11:00:50Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2505.05960/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"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","authors_text":"Dian-Yong Chen, Xiao-Yu Qi, Xing-Dao Guo","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-09T11:21:34Z","title":"The light meson decays of $D$ wave charmonia"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.05960","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:a7e9740348756bd9438be25bb2820ff699ea035571769ff1419fd46e6164ce1a","target":"record","created_at":"2026-07-05T11:00:50Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"6ce00746fc7751b02689ddae8f07efae3047876fb0124f15ab54541e4b6f3ba9","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-09T11:21:34Z","title_canon_sha256":"33eac8cb92553dc4bc01363b15c6f361175210cbbd01b4d427128782a0a793f9"},"schema_version":"1.0","source":{"id":"2505.05960","kind":"arxiv","version":1}},"canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0afcc909d527f68d2239af11c284890c4ea5163bf3659bbcb81b86587a218701","first_computed_at":"2026-07-05T11:00:50.855483Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:00:50.855483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BrS168HWnUIrlQZIJiYdEmNrS021y3ndCVNG7zrZWIK04xtZVLNGwLnqY/R/Jjv5Izm4cICVmmRLFgZ8KPcxBg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:00:50.856076Z","signed_message":"canonical_sha256_bytes"},"source_id":"2505.05960","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a7e9740348756bd9438be25bb2820ff699ea035571769ff1419fd46e6164ce1a","sha256:442cd852b0f4883026438a1af5334b0ab9af9a3a0517536a72a5e5034cd91e01"],"state_sha256":"102c303abc90e265a12cd00ff808f1d9e1a410a0a9df4a61eab6e98f68508145"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Cc8CZhqZ0EvI8Z+EUL+1nfsX9J2oTQD+L2Z6vXeM7P7u3LEmjBkchVIvJbD59HkO9fmgZe7P0bwYtSxGUPyuCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T13:07:00.926636Z","bundle_sha256":"88f6e7b0eefc43055fc54be883297b482176110b634bbb780430b7cb3d8a858e"}}