{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:NTTFS2OXFRRX7JX2WGLPIERZ2M","short_pith_number":"pith:NTTFS2OX","canonical_record":{"source":{"id":"1212.4074","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-17T17:24:16Z","cross_cats_sorted":[],"title_canon_sha256":"fab72f3bd1858999df474e456b8321ef31b21396c4d02114d53b8f332fa716b9","abstract_canon_sha256":"7291d695a9210c49da8c40438c0c87562b9fd0af46c87da7c63d99c5c51e1002"},"schema_version":"1.0"},"canonical_sha256":"6ce65969d72c637fa6fab196f41239d32c802efc87e021ef48da96f9ed4ba839","source":{"kind":"arxiv","id":"1212.4074","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4074","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4074v2","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4074","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"pith_short_12","alias_value":"NTTFS2OXFRRX","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"NTTFS2OXFRRX7JX2","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"NTTFS2OX","created_at":"2026-05-18T12:27:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:NTTFS2OXFRRX7JX2WGLPIERZ2M","target":"record","payload":{"canonical_record":{"source":{"id":"1212.4074","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-17T17:24:16Z","cross_cats_sorted":[],"title_canon_sha256":"fab72f3bd1858999df474e456b8321ef31b21396c4d02114d53b8f332fa716b9","abstract_canon_sha256":"7291d695a9210c49da8c40438c0c87562b9fd0af46c87da7c63d99c5c51e1002"},"schema_version":"1.0"},"canonical_sha256":"6ce65969d72c637fa6fab196f41239d32c802efc87e021ef48da96f9ed4ba839","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:50.348488Z","signature_b64":"9NRysWyDc6kBALTf5QkxvcJndqwibJCMXf9YtRwUhs88Z5UqJSgvLwzNnQpu0/34js2ojtL3AmfM7x3yN2ErAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ce65969d72c637fa6fab196f41239d32c802efc87e021ef48da96f9ed4ba839","last_reissued_at":"2026-05-18T03:29:50.347712Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:50.347712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.4074","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":"2026-05-18T03:29:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5efu896GkULonakl+L1J41DtUbqmiI5e8t61mrdIr34EZop8sx39Oyvx+2FtzcyM0YKAccxQyiGVRPJVZNpiCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:44:33.540651Z"},"content_sha256":"ce28f2aaa1eb9c963b564de6cc63879902b109f9e6392daae4830e4e7b84183c","schema_version":"1.0","event_id":"sha256:ce28f2aaa1eb9c963b564de6cc63879902b109f9e6392daae4830e4e7b84183c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:NTTFS2OXFRRX7JX2WGLPIERZ2M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Predicting $B -> \\rho \\gamma$ and $B_s -> \\rho \\gamma$ using holographic AdS/QCD Distribution Amplitudes for the $\\rho$ meson","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Ahmady, R. Sandapen","submitted_at":"2012-12-17T17:24:16Z","abstract_excerpt":"We derive holographic AdS/QCD Distribution Amplitudes for the transversely polarised $\\rho$ meson and we use them to predict the branching ratio for the decays $\\bar B^\\circ\\rightarrow \\rho^\\circ \\gamma$ and $\\bar B^\\circ_s\\rightarrow \\rho^\\circ \\gamma$ beyond leading power accuracy in the heavy quark limit. For $\\bar B^\\circ\\rightarrow \\rho^\\circ \\gamma$, our predictions agree with those generated using Sum Rules (SR) Distribution Amplitudes and with the data from the BaBar and Belle collaborations. In computing the weak annihilation amplitude which is power-supressed in $\\bar B^\\circ\\rightar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4074","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":"2026-05-18T03:29:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yr8jBvpnHYjNS6MVLiUFaCkkKL75THlQwcIj1eUcxuiHWlkiVaBWXv/XDFGrZJOCLMMcfAgY2pXQg61hz1TLBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:44:33.541267Z"},"content_sha256":"ac7cfcd0b85c1cf887dac94c4d6222c97c395fa305acdeb792c38019ead48b25","schema_version":"1.0","event_id":"sha256:ac7cfcd0b85c1cf887dac94c4d6222c97c395fa305acdeb792c38019ead48b25"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/bundle.json","state_url":"https://pith.science/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/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":"2026-05-27T01:44:33Z","links":{"resolver":"https://pith.science/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M","bundle":"https://pith.science/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/bundle.json","state":"https://pith.science/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NTTFS2OXFRRX7JX2WGLPIERZ2M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:NTTFS2OXFRRX7JX2WGLPIERZ2M","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":"7291d695a9210c49da8c40438c0c87562b9fd0af46c87da7c63d99c5c51e1002","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-17T17:24:16Z","title_canon_sha256":"fab72f3bd1858999df474e456b8321ef31b21396c4d02114d53b8f332fa716b9"},"schema_version":"1.0","source":{"id":"1212.4074","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.4074","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"arxiv_version","alias_value":"1212.4074v2","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4074","created_at":"2026-05-18T03:29:50Z"},{"alias_kind":"pith_short_12","alias_value":"NTTFS2OXFRRX","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_16","alias_value":"NTTFS2OXFRRX7JX2","created_at":"2026-05-18T12:27:16Z"},{"alias_kind":"pith_short_8","alias_value":"NTTFS2OX","created_at":"2026-05-18T12:27:16Z"}],"graph_snapshots":[{"event_id":"sha256:ac7cfcd0b85c1cf887dac94c4d6222c97c395fa305acdeb792c38019ead48b25","target":"graph","created_at":"2026-05-18T03:29:50Z","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"},"paper":{"abstract_excerpt":"We derive holographic AdS/QCD Distribution Amplitudes for the transversely polarised $\\rho$ meson and we use them to predict the branching ratio for the decays $\\bar B^\\circ\\rightarrow \\rho^\\circ \\gamma$ and $\\bar B^\\circ_s\\rightarrow \\rho^\\circ \\gamma$ beyond leading power accuracy in the heavy quark limit. For $\\bar B^\\circ\\rightarrow \\rho^\\circ \\gamma$, our predictions agree with those generated using Sum Rules (SR) Distribution Amplitudes and with the data from the BaBar and Belle collaborations. In computing the weak annihilation amplitude which is power-supressed in $\\bar B^\\circ\\rightar","authors_text":"M. Ahmady, R. Sandapen","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-17T17:24:16Z","title":"Predicting $B -> \\rho \\gamma$ and $B_s -> \\rho \\gamma$ using holographic AdS/QCD Distribution Amplitudes for the $\\rho$ meson"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4074","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:ce28f2aaa1eb9c963b564de6cc63879902b109f9e6392daae4830e4e7b84183c","target":"record","created_at":"2026-05-18T03:29:50Z","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":"7291d695a9210c49da8c40438c0c87562b9fd0af46c87da7c63d99c5c51e1002","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-17T17:24:16Z","title_canon_sha256":"fab72f3bd1858999df474e456b8321ef31b21396c4d02114d53b8f332fa716b9"},"schema_version":"1.0","source":{"id":"1212.4074","kind":"arxiv","version":2}},"canonical_sha256":"6ce65969d72c637fa6fab196f41239d32c802efc87e021ef48da96f9ed4ba839","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6ce65969d72c637fa6fab196f41239d32c802efc87e021ef48da96f9ed4ba839","first_computed_at":"2026-05-18T03:29:50.347712Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:29:50.347712Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9NRysWyDc6kBALTf5QkxvcJndqwibJCMXf9YtRwUhs88Z5UqJSgvLwzNnQpu0/34js2ojtL3AmfM7x3yN2ErAw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:29:50.348488Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.4074","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ce28f2aaa1eb9c963b564de6cc63879902b109f9e6392daae4830e4e7b84183c","sha256:ac7cfcd0b85c1cf887dac94c4d6222c97c395fa305acdeb792c38019ead48b25"],"state_sha256":"d5887ebb4d83e171ce95f1950abde8bcc706b32cb46a185eff772c599d708cee"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s1NTBY5eFQsCjFuLdcESfGjTyyJp8bn39L/VPy6xV06jJah+A7OfQfB0HqQ3U5CR0Ql2o21i0A0r/HhDniVQDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T01:44:33.544449Z","bundle_sha256":"c85598be66c1ac5b21cca6d4ca87b04fde561af1c0f1028a28e06783cbcf4150"}}