{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:ZS6FZEB22ZYWUVWMPJUKZDFYAW","short_pith_number":"pith:ZS6FZEB2","canonical_record":{"source":{"id":"0705.0892","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-05-07T12:58:15Z","cross_cats_sorted":[],"title_canon_sha256":"5a7016a706f68941e19c062b0ddd44773f043e58117b71c6594a587483a504ca","abstract_canon_sha256":"9bf0bf02a0b7868f8512cb16913d00ade218afc4fa01785b7d71de532632ea38"},"schema_version":"1.0"},"canonical_sha256":"ccbc5c903ad6716a56cc7a68ac8cb805bf2bf964d4216ac2cc28de9add1deb85","source":{"kind":"arxiv","id":"0705.0892","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0705.0892","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"arxiv_version","alias_value":"0705.0892v2","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.0892","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_12","alias_value":"ZS6FZEB22ZYW","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_16","alias_value":"ZS6FZEB22ZYWUVWM","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_8","alias_value":"ZS6FZEB2","created_at":"2026-07-04T15:21:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:ZS6FZEB22ZYWUVWMPJUKZDFYAW","target":"record","payload":{"canonical_record":{"source":{"id":"0705.0892","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-05-07T12:58:15Z","cross_cats_sorted":[],"title_canon_sha256":"5a7016a706f68941e19c062b0ddd44773f043e58117b71c6594a587483a504ca","abstract_canon_sha256":"9bf0bf02a0b7868f8512cb16913d00ade218afc4fa01785b7d71de532632ea38"},"schema_version":"1.0"},"canonical_sha256":"ccbc5c903ad6716a56cc7a68ac8cb805bf2bf964d4216ac2cc28de9add1deb85","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:21:10.142064Z","signature_b64":"45dg+AXjcqvZqSIg8duYGLvX+mputKLDvcDyAI2KIklFJf37oM4s1yyLMuoRgdbKC3oy/a/yz+liDCGugrf/Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ccbc5c903ad6716a56cc7a68ac8cb805bf2bf964d4216ac2cc28de9add1deb85","last_reissued_at":"2026-07-04T15:21:10.141677Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:21:10.141677Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0705.0892","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":"2026-07-04T15:21:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0vSDJn0bCrHJirStFxOKHyDuC6XuBZA+NZUN8ReS3Jm+j2bMtaNFGmjziDA30UMGsEeL01z3bWVq70hnVT67Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T17:50:35.187789Z"},"content_sha256":"96d3cfb7feea3a31119928a76298b5935234f10051d933944cc7a80c3f2fcee9","schema_version":"1.0","event_id":"sha256:96d3cfb7feea3a31119928a76298b5935234f10051d933944cc7a80c3f2fcee9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:ZS6FZEB22ZYWUVWMPJUKZDFYAW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ds0*(2317) and Ds1(2460) mesons in two-body B-meson decays","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Amand Faessler, Sergey Kovalenko, Thomas Gutsche, Valery E. Lyubovitskij","submitted_at":"2007-05-07T12:58:15Z","abstract_excerpt":"We analyze the branching ratios of B to D(*) + Ds0*(Ds1) decays using the factorization hypothesis. The B to D(*) transition form factors are taken from a model-independent analysis done by Caprini, Lellouch and Neubert based on heavy quark spin symmetry and dispersive constraints, including short-distance and power corrections. The leptonic decay constants fDs0* and fDs1 are calculated assuming a molecular structure for the Ds0* and Ds1 mesons. The calculated branching ratios of B-meson two-body decays are compared with experimental data and other theoretical results."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.0892","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0705.0892/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":"2026-07-04T15:21:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QFfvCkmt0rj4RahznqTmNJZMEr71ui42cXPOwWC25aQVinNCWIqGFtZSVAKCiVcjTAjrfrp/4BlxRK5vTCH/Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-01T17:50:35.189269Z"},"content_sha256":"d1bf5e7bb1f44937bb9fb6e13c5ef5328ea3c3abd23893e0a1a2fcd3cb7369bc","schema_version":"1.0","event_id":"sha256:d1bf5e7bb1f44937bb9fb6e13c5ef5328ea3c3abd23893e0a1a2fcd3cb7369bc"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/bundle.json","state_url":"https://pith.science/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/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":"2026-08-01T17:50:35Z","links":{"resolver":"https://pith.science/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW","bundle":"https://pith.science/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/bundle.json","state":"https://pith.science/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZS6FZEB22ZYWUVWMPJUKZDFYAW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:ZS6FZEB22ZYWUVWMPJUKZDFYAW","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":"9bf0bf02a0b7868f8512cb16913d00ade218afc4fa01785b7d71de532632ea38","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2007-05-07T12:58:15Z","title_canon_sha256":"5a7016a706f68941e19c062b0ddd44773f043e58117b71c6594a587483a504ca"},"schema_version":"1.0","source":{"id":"0705.0892","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0705.0892","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"arxiv_version","alias_value":"0705.0892v2","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.0892","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_12","alias_value":"ZS6FZEB22ZYW","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_16","alias_value":"ZS6FZEB22ZYWUVWM","created_at":"2026-07-04T15:21:10Z"},{"alias_kind":"pith_short_8","alias_value":"ZS6FZEB2","created_at":"2026-07-04T15:21:10Z"}],"graph_snapshots":[{"event_id":"sha256:d1bf5e7bb1f44937bb9fb6e13c5ef5328ea3c3abd23893e0a1a2fcd3cb7369bc","target":"graph","created_at":"2026-07-04T15:21:10Z","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/0705.0892/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We analyze the branching ratios of B to D(*) + Ds0*(Ds1) decays using the factorization hypothesis. The B to D(*) transition form factors are taken from a model-independent analysis done by Caprini, Lellouch and Neubert based on heavy quark spin symmetry and dispersive constraints, including short-distance and power corrections. The leptonic decay constants fDs0* and fDs1 are calculated assuming a molecular structure for the Ds0* and Ds1 mesons. The calculated branching ratios of B-meson two-body decays are compared with experimental data and other theoretical results.","authors_text":"Amand Faessler, Sergey Kovalenko, Thomas Gutsche, Valery E. Lyubovitskij","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2007-05-07T12:58:15Z","title":"Ds0*(2317) and Ds1(2460) mesons in two-body B-meson decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.0892","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":"sha256:96d3cfb7feea3a31119928a76298b5935234f10051d933944cc7a80c3f2fcee9","target":"record","created_at":"2026-07-04T15:21:10Z","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":"9bf0bf02a0b7868f8512cb16913d00ade218afc4fa01785b7d71de532632ea38","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2007-05-07T12:58:15Z","title_canon_sha256":"5a7016a706f68941e19c062b0ddd44773f043e58117b71c6594a587483a504ca"},"schema_version":"1.0","source":{"id":"0705.0892","kind":"arxiv","version":2}},"canonical_sha256":"ccbc5c903ad6716a56cc7a68ac8cb805bf2bf964d4216ac2cc28de9add1deb85","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ccbc5c903ad6716a56cc7a68ac8cb805bf2bf964d4216ac2cc28de9add1deb85","first_computed_at":"2026-07-04T15:21:10.141677Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:21:10.141677Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"45dg+AXjcqvZqSIg8duYGLvX+mputKLDvcDyAI2KIklFJf37oM4s1yyLMuoRgdbKC3oy/a/yz+liDCGugrf/Ag==","signature_status":"signed_v1","signed_at":"2026-07-04T15:21:10.142064Z","signed_message":"canonical_sha256_bytes"},"source_id":"0705.0892","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:96d3cfb7feea3a31119928a76298b5935234f10051d933944cc7a80c3f2fcee9","sha256:d1bf5e7bb1f44937bb9fb6e13c5ef5328ea3c3abd23893e0a1a2fcd3cb7369bc"],"state_sha256":"5950c487f89e061c5ca0a6c9b5c8d5407da808bfe4b8127780b377642d8f54a3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RqS+xvk8d6okjVEPKcZXQ20LsK0+NON9OJBtNCq5Nc1aWW7wSKB4lbCqcD/RJqj84sHEOoAMrczKE9vHFe0xCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-01T17:50:35.195068Z","bundle_sha256":"927aac8a865ff7a3c1e30b0ff8acd4992037fdfd187407ada810775c0be8f2b3"}}