{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:ZJBVUGJDFCPMPRKBMHWAO5YNCW","short_pith_number":"pith:ZJBVUGJD","canonical_record":{"source":{"id":"1306.4095","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-18T08:08:16Z","cross_cats_sorted":[],"title_canon_sha256":"058318f146e65a670f5174f7a855c66f1f22ee6db7a63154cb80bb8af38b86c4","abstract_canon_sha256":"b14f2291f3ea15206ae3670425e1f61259a095295192df4783f0c6e91d99dc36"},"schema_version":"1.0"},"canonical_sha256":"ca435a1923289ec7c54161ec07770d15bcbd2ca9c73ec51267a04f8ee64e7a7b","source":{"kind":"arxiv","id":"1306.4095","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.4095","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"arxiv_version","alias_value":"1306.4095v1","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.4095","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"pith_short_12","alias_value":"ZJBVUGJDFCPM","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZJBVUGJDFCPMPRKB","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZJBVUGJD","created_at":"2026-05-18T12:28:09Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:ZJBVUGJDFCPMPRKBMHWAO5YNCW","target":"record","payload":{"canonical_record":{"source":{"id":"1306.4095","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-18T08:08:16Z","cross_cats_sorted":[],"title_canon_sha256":"058318f146e65a670f5174f7a855c66f1f22ee6db7a63154cb80bb8af38b86c4","abstract_canon_sha256":"b14f2291f3ea15206ae3670425e1f61259a095295192df4783f0c6e91d99dc36"},"schema_version":"1.0"},"canonical_sha256":"ca435a1923289ec7c54161ec07770d15bcbd2ca9c73ec51267a04f8ee64e7a7b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:20:37.173073Z","signature_b64":"B8hCbEvr1/WFmiCFTxIFQWWYTqAkDsH9Erb4hF+pUztot3FxocQBa7/TFdmWm498jAnNCRILNt6ZPsJKewYDBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca435a1923289ec7c54161ec07770d15bcbd2ca9c73ec51267a04f8ee64e7a7b","last_reissued_at":"2026-05-18T03:20:37.172350Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:20:37.172350Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.4095","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":"2026-05-18T03:20:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3bQ+HaXbEgnSIlN9ZY8PZy/CD+krJoSaAGgnqeWA03AfawOZw0e6SbT/GjuQFxAfYoC6Y9EpWbL2LGWDgfNaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:43:06.138353Z"},"content_sha256":"4744d3d5194ae831903f0e6efe6b1aba928da390fb835fc32e18b3251da44e9f","schema_version":"1.0","event_id":"sha256:4744d3d5194ae831903f0e6efe6b1aba928da390fb835fc32e18b3251da44e9f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:ZJBVUGJDFCPMPRKBMHWAO5YNCW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Investigation of the $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ transition 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":"2013-06-18T08:08:16Z","abstract_excerpt":"We calculate the transition form factors of the semileptonic $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ in the framework of QCD sum rules taking into account the two-gluon condensate corrections. Using the obtained results of form factors we estimate the decay widths and branching ratios related to this transition at all lepton channels. A comparison of the obtained results with the predictions of other non-perturbative approaches are also made. The orders of branching ratios for different lepton channels indicate that the $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ transition can be studied at LHC u"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.4095","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:20:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UeSWpnTwU2al0xnGuDD4N0KtTnk/Q6/uuxbzrXXjX9iXydreAKMPXZBQPrZGQjXJ9BjEdz1lqKdwNwLruUYRDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:43:06.139051Z"},"content_sha256":"bd312de0503ef90b0a817bf9b6d4e47341fcd854f44cf70145f8c529609ec12f","schema_version":"1.0","event_id":"sha256:bd312de0503ef90b0a817bf9b6d4e47341fcd854f44cf70145f8c529609ec12f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/bundle.json","state_url":"https://pith.science/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/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":"2026-05-25T13:43:06Z","links":{"resolver":"https://pith.science/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW","bundle":"https://pith.science/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/bundle.json","state":"https://pith.science/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZJBVUGJDFCPMPRKBMHWAO5YNCW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:ZJBVUGJDFCPMPRKBMHWAO5YNCW","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":"b14f2291f3ea15206ae3670425e1f61259a095295192df4783f0c6e91d99dc36","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-18T08:08:16Z","title_canon_sha256":"058318f146e65a670f5174f7a855c66f1f22ee6db7a63154cb80bb8af38b86c4"},"schema_version":"1.0","source":{"id":"1306.4095","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.4095","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"arxiv_version","alias_value":"1306.4095v1","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.4095","created_at":"2026-05-18T03:20:37Z"},{"alias_kind":"pith_short_12","alias_value":"ZJBVUGJDFCPM","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_16","alias_value":"ZJBVUGJDFCPMPRKB","created_at":"2026-05-18T12:28:09Z"},{"alias_kind":"pith_short_8","alias_value":"ZJBVUGJD","created_at":"2026-05-18T12:28:09Z"}],"graph_snapshots":[{"event_id":"sha256:bd312de0503ef90b0a817bf9b6d4e47341fcd854f44cf70145f8c529609ec12f","target":"graph","created_at":"2026-05-18T03:20:37Z","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":"We calculate the transition form factors of the semileptonic $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ in the framework of QCD sum rules taking into account the two-gluon condensate corrections. Using the obtained results of form factors we estimate the decay widths and branching ratios related to this transition at all lepton channels. A comparison of the obtained results with the predictions of other non-perturbative approaches are also made. The orders of branching ratios for different lepton channels indicate that the $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ transition can be studied at LHC u","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":"2013-06-18T08:08:16Z","title":"Investigation of the $B_c\\rightarrow \\chi_{c2} l \\bar{\\nu} $ transition via QCD sum rules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.4095","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":"sha256:4744d3d5194ae831903f0e6efe6b1aba928da390fb835fc32e18b3251da44e9f","target":"record","created_at":"2026-05-18T03:20:37Z","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":"b14f2291f3ea15206ae3670425e1f61259a095295192df4783f0c6e91d99dc36","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-06-18T08:08:16Z","title_canon_sha256":"058318f146e65a670f5174f7a855c66f1f22ee6db7a63154cb80bb8af38b86c4"},"schema_version":"1.0","source":{"id":"1306.4095","kind":"arxiv","version":1}},"canonical_sha256":"ca435a1923289ec7c54161ec07770d15bcbd2ca9c73ec51267a04f8ee64e7a7b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ca435a1923289ec7c54161ec07770d15bcbd2ca9c73ec51267a04f8ee64e7a7b","first_computed_at":"2026-05-18T03:20:37.172350Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:20:37.172350Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"B8hCbEvr1/WFmiCFTxIFQWWYTqAkDsH9Erb4hF+pUztot3FxocQBa7/TFdmWm498jAnNCRILNt6ZPsJKewYDBg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:20:37.173073Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.4095","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4744d3d5194ae831903f0e6efe6b1aba928da390fb835fc32e18b3251da44e9f","sha256:bd312de0503ef90b0a817bf9b6d4e47341fcd854f44cf70145f8c529609ec12f"],"state_sha256":"b337e78d7cd539aa7f1c32c62f8180ca237da6d05e98699287fcce9974b98097"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fl9LY8fhgwF7+Jm6ZdnEFanAlXG0bx6fhVADCzI+QCk3e34R1RBKdD1DIm4A/tPnsuM87axhW6fzFhNXgqQKAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T13:43:06.142875Z","bundle_sha256":"14d4f3368eb60ab0d1acb0c9950bcfe0ca6d274b0867283f72c2ab2bb7b9776a"}}