{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:LWJZWXJ52JAHKJKYHDFRDYGMAV","short_pith_number":"pith:LWJZWXJ5","canonical_record":{"source":{"id":"1402.6887","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-27T12:35:14Z","cross_cats_sorted":[],"title_canon_sha256":"bdbd847cf6cdab4167693a1f796350c70c639623ef184d7783f51e6d16b4adc2","abstract_canon_sha256":"341ac88ac25c482e91e15069fd1d5830947dca8c31d7adaef56457a623835981"},"schema_version":"1.0"},"canonical_sha256":"5d939b5d3dd24075255838cb11e0cc055cea9e8a13d49b7ab126cb309e6b5439","source":{"kind":"arxiv","id":"1402.6887","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.6887","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"arxiv_version","alias_value":"1402.6887v2","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6887","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"pith_short_12","alias_value":"LWJZWXJ52JAH","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LWJZWXJ52JAHKJKY","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LWJZWXJ5","created_at":"2026-05-18T12:28:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:LWJZWXJ52JAHKJKYHDFRDYGMAV","target":"record","payload":{"canonical_record":{"source":{"id":"1402.6887","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-27T12:35:14Z","cross_cats_sorted":[],"title_canon_sha256":"bdbd847cf6cdab4167693a1f796350c70c639623ef184d7783f51e6d16b4adc2","abstract_canon_sha256":"341ac88ac25c482e91e15069fd1d5830947dca8c31d7adaef56457a623835981"},"schema_version":"1.0"},"canonical_sha256":"5d939b5d3dd24075255838cb11e0cc055cea9e8a13d49b7ab126cb309e6b5439","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:41:53.264927Z","signature_b64":"UKgMwjZCXjLMXWCq07j1/5Jb2lVg6v02NbYA80mNIyWlO0k3HvR0Ujw7R46a/KGfV3mkxztMcwfVGVtJVpk7Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d939b5d3dd24075255838cb11e0cc055cea9e8a13d49b7ab126cb309e6b5439","last_reissued_at":"2026-05-18T02:41:53.264294Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:41:53.264294Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.6887","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:41:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D0t1WfkE7TRfb2ytS6OCB7/dauj51WbRdAEanh4KZ3bMkSl8L/uOAIcy9zpJKVVn0Nu5gpDqNO8ZULNc+KH6Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T10:13:29.338118Z"},"content_sha256":"704015f3a9595d9639086ef9438303190cba78f7a269351e29873f1d7b693410","schema_version":"1.0","event_id":"sha256:704015f3a9595d9639086ef9438303190cba78f7a269351e29873f1d7b693410"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:LWJZWXJ52JAHKJKYHDFRDYGMAV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analysis of the strong $D_{2}^{*}(2460)^{0}\\rightarrow D^+ \\pi^- $ and $D_{s2}^{*}(2573)^{+}\\rightarrow D^{+} K^{0}$ transitions via QCD sum rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. Sundu, K. Azizi, Y. Sarac","submitted_at":"2014-02-27T12:35:14Z","abstract_excerpt":"The strong $D_{2}^{*}(2460)^{0}\\rightarrow D^+ \\pi^- $ and $D_{s2}^{*}(2573)^{+}\\rightarrow D^{+} K^{0}$ transitions are analyzed via three point QCD sum rules. First, we calculate the corresponding strong coupling constants $g_{D_2^*D\\pi}$ and $g_{D_{s2}^*DK}$. Then, we use them to calculate the corresponding decay widths and branching ratios. Making use of the existing experimental data on the ratio of the decay width in the pseudoscaler $D$ channel to that of the vector $D^*$ channel, finally, we estimate the decay width and branching ratio of the strong $D_2^*(2460)^0 \\rightarrow D^*(2010)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6887","kind":"arxiv","version":2},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:41:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"etpanLsKOpgAqdSegCuq65CE7afYWRxdd8jjnrLsrzfeq8681+1PmNMGxnX2bvE4vR3kQ7tWBtgIWjsYF5j0Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T10:13:29.338489Z"},"content_sha256":"3fa560ab0340dbb7b1246186bcc6b5053b2dbe162fc2aa6cefaa0ba074e71664","schema_version":"1.0","event_id":"sha256:3fa560ab0340dbb7b1246186bcc6b5053b2dbe162fc2aa6cefaa0ba074e71664"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/bundle.json","state_url":"https://pith.science/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/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":"2026-06-11T10:13:29Z","links":{"resolver":"https://pith.science/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV","bundle":"https://pith.science/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/bundle.json","state":"https://pith.science/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LWJZWXJ52JAHKJKYHDFRDYGMAV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:LWJZWXJ52JAHKJKYHDFRDYGMAV","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":"341ac88ac25c482e91e15069fd1d5830947dca8c31d7adaef56457a623835981","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-27T12:35:14Z","title_canon_sha256":"bdbd847cf6cdab4167693a1f796350c70c639623ef184d7783f51e6d16b4adc2"},"schema_version":"1.0","source":{"id":"1402.6887","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.6887","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"arxiv_version","alias_value":"1402.6887v2","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6887","created_at":"2026-05-18T02:41:53Z"},{"alias_kind":"pith_short_12","alias_value":"LWJZWXJ52JAH","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_16","alias_value":"LWJZWXJ52JAHKJKY","created_at":"2026-05-18T12:28:38Z"},{"alias_kind":"pith_short_8","alias_value":"LWJZWXJ5","created_at":"2026-05-18T12:28:38Z"}],"graph_snapshots":[{"event_id":"sha256:3fa560ab0340dbb7b1246186bcc6b5053b2dbe162fc2aa6cefaa0ba074e71664","target":"graph","created_at":"2026-05-18T02:41:53Z","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"},"paper":{"abstract_excerpt":"The strong $D_{2}^{*}(2460)^{0}\\rightarrow D^+ \\pi^- $ and $D_{s2}^{*}(2573)^{+}\\rightarrow D^{+} K^{0}$ transitions are analyzed via three point QCD sum rules. First, we calculate the corresponding strong coupling constants $g_{D_2^*D\\pi}$ and $g_{D_{s2}^*DK}$. Then, we use them to calculate the corresponding decay widths and branching ratios. Making use of the existing experimental data on the ratio of the decay width in the pseudoscaler $D$ channel to that of the vector $D^*$ channel, finally, we estimate the decay width and branching ratio of the strong $D_2^*(2460)^0 \\rightarrow D^*(2010)","authors_text":"H. Sundu, K. Azizi, Y. Sarac","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-27T12:35:14Z","title":"Analysis of the strong $D_{2}^{*}(2460)^{0}\\rightarrow D^+ \\pi^- $ and $D_{s2}^{*}(2573)^{+}\\rightarrow D^{+} K^{0}$ transitions via QCD sum rules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6887","kind":"arxiv","version":2},"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":"sha256:704015f3a9595d9639086ef9438303190cba78f7a269351e29873f1d7b693410","target":"record","created_at":"2026-05-18T02:41:53Z","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":"341ac88ac25c482e91e15069fd1d5830947dca8c31d7adaef56457a623835981","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-27T12:35:14Z","title_canon_sha256":"bdbd847cf6cdab4167693a1f796350c70c639623ef184d7783f51e6d16b4adc2"},"schema_version":"1.0","source":{"id":"1402.6887","kind":"arxiv","version":2}},"canonical_sha256":"5d939b5d3dd24075255838cb11e0cc055cea9e8a13d49b7ab126cb309e6b5439","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5d939b5d3dd24075255838cb11e0cc055cea9e8a13d49b7ab126cb309e6b5439","first_computed_at":"2026-05-18T02:41:53.264294Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:41:53.264294Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UKgMwjZCXjLMXWCq07j1/5Jb2lVg6v02NbYA80mNIyWlO0k3HvR0Ujw7R46a/KGfV3mkxztMcwfVGVtJVpk7Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:41:53.264927Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.6887","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:704015f3a9595d9639086ef9438303190cba78f7a269351e29873f1d7b693410","sha256:3fa560ab0340dbb7b1246186bcc6b5053b2dbe162fc2aa6cefaa0ba074e71664"],"state_sha256":"ae5cd4d0cab9e87bb9028c6cddc9f4b065104d20a1051a4eca75b0912c433ec4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"128V5FDsqYFb5TGO9AS2yZJmt9akSq5QGj0aRMuXYM/siz0APoNiJyVrlWT2K7ASftDclh2Ch0Qgav7EE9cjBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T10:13:29.340465Z","bundle_sha256":"d04e7d87aaa2cc7bca5b3aa54a9f383024fa6ba77e650dd608f5e5f8597d168b"}}