{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:42FDUL7PXI4NT7LB7WWI6FTCKM","short_pith_number":"pith:42FDUL7P","canonical_record":{"source":{"id":"1207.5912","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-25T08:04:24Z","cross_cats_sorted":[],"title_canon_sha256":"cec3ea4f2737bfba63067315c2bdbcc94bf69ae67abd7f223032c6f07c76b15e","abstract_canon_sha256":"7a4a6aa8ef2bed1eac3545d65cdc6fd75b8add62df5419719b4e9c396389bd95"},"schema_version":"1.0"},"canonical_sha256":"e68a3a2fefba38d9fd61fdac8f166253183fb4beddd236d2f293afaad7fe00ec","source":{"kind":"arxiv","id":"1207.5912","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5912","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5912v1","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5912","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"pith_short_12","alias_value":"42FDUL7PXI4N","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"42FDUL7PXI4NT7LB","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"42FDUL7P","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:42FDUL7PXI4NT7LB7WWI6FTCKM","target":"record","payload":{"canonical_record":{"source":{"id":"1207.5912","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-25T08:04:24Z","cross_cats_sorted":[],"title_canon_sha256":"cec3ea4f2737bfba63067315c2bdbcc94bf69ae67abd7f223032c6f07c76b15e","abstract_canon_sha256":"7a4a6aa8ef2bed1eac3545d65cdc6fd75b8add62df5419719b4e9c396389bd95"},"schema_version":"1.0"},"canonical_sha256":"e68a3a2fefba38d9fd61fdac8f166253183fb4beddd236d2f293afaad7fe00ec","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:50:09.956465Z","signature_b64":"1U469fYV0yBNEjrBMTYzrhuIYnynbXjxf4DMCADZkWCmvutLRT1dB4s3UQtDDW1lbGqOAOrOj/3HC1UPx9bzDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e68a3a2fefba38d9fd61fdac8f166253183fb4beddd236d2f293afaad7fe00ec","last_reissued_at":"2026-05-18T03:50:09.955872Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:50:09.955872Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1207.5912","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":"2026-05-18T03:50:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/VaQXu92nkYq1nToHu6AEmXmGhYPmCVKGO//NutnfbaoIEdl/wFIx0uybQKi5NEwveEI3qWXvJ8CUGM0pvAEDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T23:31:23.271380Z"},"content_sha256":"c3da4e670a3e12613511edc2cc6f1ece61609b2db3a30c091425ea8508c00bd0","schema_version":"1.0","event_id":"sha256:c3da4e670a3e12613511edc2cc6f1ece61609b2db3a30c091425ea8508c00bd0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:42FDUL7PXI4NT7LB7WWI6FTCKM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charmed Scalar Meson Production in $B$ Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Xin Yu, Yue-Long Shen","submitted_at":"2012-07-25T08:04:24Z","abstract_excerpt":"The study on the charmed scalar meson spectroscopy has become a hot topic both experimentally and theoretically. The $B_{(s)}$ decays provide an ideal place to study their property. We employ the $B$-meson light-cone sum rules to compute the $\\bar B_s^0\\to D_s^{*+}(2317)$ and $B^-\\to D_0^{*0}(2400)$ transition form factors at large recoil, assuming $D_s^{*+}(2317)$ and $D_0^{*0}(2400)$ being scalar quark-anti-quark states. The results are extrapolated to the whole momentum region with the help of HQET. Considering large uncertainties, our results can be consistent with the previous studies, wh"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5912","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":"2026-05-18T03:50:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zkWaSvx6q/NsHVybBR4d5QXQnQxS4dhHq7rzmhHs+7ZxbHZ+PXObAJDuhtZxq+moyQDJ8bsubUJY+Ol0LLrXBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T23:31:23.272064Z"},"content_sha256":"921d5b68a6c885f608d68f6d5bea6147640cae928c585abcfbef947c68f067b8","schema_version":"1.0","event_id":"sha256:921d5b68a6c885f608d68f6d5bea6147640cae928c585abcfbef947c68f067b8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/bundle.json","state_url":"https://pith.science/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/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":"2026-05-22T23:31:23Z","links":{"resolver":"https://pith.science/pith/42FDUL7PXI4NT7LB7WWI6FTCKM","bundle":"https://pith.science/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/bundle.json","state":"https://pith.science/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/42FDUL7PXI4NT7LB7WWI6FTCKM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:42FDUL7PXI4NT7LB7WWI6FTCKM","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":"7a4a6aa8ef2bed1eac3545d65cdc6fd75b8add62df5419719b4e9c396389bd95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-25T08:04:24Z","title_canon_sha256":"cec3ea4f2737bfba63067315c2bdbcc94bf69ae67abd7f223032c6f07c76b15e"},"schema_version":"1.0","source":{"id":"1207.5912","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1207.5912","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"arxiv_version","alias_value":"1207.5912v1","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.5912","created_at":"2026-05-18T03:50:09Z"},{"alias_kind":"pith_short_12","alias_value":"42FDUL7PXI4N","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"42FDUL7PXI4NT7LB","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"42FDUL7P","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:921d5b68a6c885f608d68f6d5bea6147640cae928c585abcfbef947c68f067b8","target":"graph","created_at":"2026-05-18T03:50:09Z","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 study on the charmed scalar meson spectroscopy has become a hot topic both experimentally and theoretically. The $B_{(s)}$ decays provide an ideal place to study their property. We employ the $B$-meson light-cone sum rules to compute the $\\bar B_s^0\\to D_s^{*+}(2317)$ and $B^-\\to D_0^{*0}(2400)$ transition form factors at large recoil, assuming $D_s^{*+}(2317)$ and $D_0^{*0}(2400)$ being scalar quark-anti-quark states. The results are extrapolated to the whole momentum region with the help of HQET. Considering large uncertainties, our results can be consistent with the previous studies, wh","authors_text":"Xin Yu, Yue-Long Shen","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-25T08:04:24Z","title":"Charmed Scalar Meson Production in $B$ Decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.5912","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:c3da4e670a3e12613511edc2cc6f1ece61609b2db3a30c091425ea8508c00bd0","target":"record","created_at":"2026-05-18T03:50:09Z","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":"7a4a6aa8ef2bed1eac3545d65cdc6fd75b8add62df5419719b4e9c396389bd95","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-07-25T08:04:24Z","title_canon_sha256":"cec3ea4f2737bfba63067315c2bdbcc94bf69ae67abd7f223032c6f07c76b15e"},"schema_version":"1.0","source":{"id":"1207.5912","kind":"arxiv","version":1}},"canonical_sha256":"e68a3a2fefba38d9fd61fdac8f166253183fb4beddd236d2f293afaad7fe00ec","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e68a3a2fefba38d9fd61fdac8f166253183fb4beddd236d2f293afaad7fe00ec","first_computed_at":"2026-05-18T03:50:09.955872Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:50:09.955872Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1U469fYV0yBNEjrBMTYzrhuIYnynbXjxf4DMCADZkWCmvutLRT1dB4s3UQtDDW1lbGqOAOrOj/3HC1UPx9bzDw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:50:09.956465Z","signed_message":"canonical_sha256_bytes"},"source_id":"1207.5912","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c3da4e670a3e12613511edc2cc6f1ece61609b2db3a30c091425ea8508c00bd0","sha256:921d5b68a6c885f608d68f6d5bea6147640cae928c585abcfbef947c68f067b8"],"state_sha256":"9bdccc3e16a515322aba5197930ed6604f571b387e6f8d1c059afac6f94cecda"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jjkIdHzw967xRBIIhk8UPg7QhxwTBCx2EXd2LPW1mjloDAiif6jUwFVFdbR4XakC5/xd5UbTF7YKv8fu8SR6Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T23:31:23.275465Z","bundle_sha256":"3157156aa77e5a43498429310f89377958b9be99c812865215c7634db0159205"}}