{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:RUTMXNXSCB67RXV6I3OI7DEEDY","short_pith_number":"pith:RUTMXNXS","canonical_record":{"source":{"id":"1409.3088","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T14:30:11Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"34ad6bf99c661fe44d3d0b3a0f37f3b63fb940fdc9dea47abdc7de2b29724c04","abstract_canon_sha256":"0989db013574a476afc32d23e55332a5a53fac5e5f49cd122b8ca2538ab05b1c"},"schema_version":"1.0"},"canonical_sha256":"8d26cbb6f2107df8debe46dc8f8c841e26c162889404d445dff1a8471e55b800","source":{"kind":"arxiv","id":"1409.3088","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.3088","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"arxiv_version","alias_value":"1409.3088v2","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3088","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"pith_short_12","alias_value":"RUTMXNXSCB67","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RUTMXNXSCB67RXV6","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RUTMXNXS","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:RUTMXNXSCB67RXV6I3OI7DEEDY","target":"record","payload":{"canonical_record":{"source":{"id":"1409.3088","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T14:30:11Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"34ad6bf99c661fe44d3d0b3a0f37f3b63fb940fdc9dea47abdc7de2b29724c04","abstract_canon_sha256":"0989db013574a476afc32d23e55332a5a53fac5e5f49cd122b8ca2538ab05b1c"},"schema_version":"1.0"},"canonical_sha256":"8d26cbb6f2107df8debe46dc8f8c841e26c162889404d445dff1a8471e55b800","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:46.962159Z","signature_b64":"rzCl/W1CZTYr709IXlclEo4wufTRa1ZV/osQWS5dz3ntEmljKr7HgCRXODCDW7ZhrniRKwUcinqb3z5crWaVBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d26cbb6f2107df8debe46dc8f8c841e26c162889404d445dff1a8471e55b800","last_reissued_at":"2026-05-18T02:35:46.961617Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:46.961617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1409.3088","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":"2026-05-18T02:35:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L2nwJV+godehFNdRwCFSe/tXluBpdOHVleSMN1bqGdXqHH3dcDpX2NbnFDnDViydLKydaF6Y9/VeksKhKSvuCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:09:25.589166Z"},"content_sha256":"5f5a82172c341565afd892ed6294dc4adf7c6b9bf99f9c4d9115822885d81629","schema_version":"1.0","event_id":"sha256:5f5a82172c341565afd892ed6294dc4adf7c6b9bf99f9c4d9115822885d81629"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:RUTMXNXSCB67RXV6I3OI7DEEDY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Testing New Physics Effects in $B \\to K^*\\ell^+\\ell^-$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Diganta Das, Rahul Sinha, Rusa Mandal","submitted_at":"2014-09-10T14:30:11Z","abstract_excerpt":"It is generally believed that the decay mode $B\\to K^*\\ell^+\\ell^-$ is one of the best modes to search for physics beyond the standard model. The angular distribution enables the independent measurement of several observables as a function of the dilepton invariant mass. The plethora of observables so obtained enable unique tests of the standard model contributions. We start by writing the most general parametric form of the standard model amplitude for $B\\to K^*\\ell^+\\ell^-$ taking into account comprehensively all contributions within SM. These include all short-distance and long-distance eff"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3088","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":"2026-05-18T02:35:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZQf7RpDeGbgKPPx4gaS4pMZ34V+klWmCuF6yYXpSeEB2YepoRqb0T1PkhqoUY33J2hcDn4Cc15ZKnyuQH5L6Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T05:09:25.589618Z"},"content_sha256":"89fe5f58a21f832c87f32ae615f71fcece434d6bf7eb459d492d2ed572cec523","schema_version":"1.0","event_id":"sha256:89fe5f58a21f832c87f32ae615f71fcece434d6bf7eb459d492d2ed572cec523"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/bundle.json","state_url":"https://pith.science/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/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":"2026-06-02T05:09:25Z","links":{"resolver":"https://pith.science/pith/RUTMXNXSCB67RXV6I3OI7DEEDY","bundle":"https://pith.science/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/bundle.json","state":"https://pith.science/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RUTMXNXSCB67RXV6I3OI7DEEDY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:RUTMXNXSCB67RXV6I3OI7DEEDY","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":"0989db013574a476afc32d23e55332a5a53fac5e5f49cd122b8ca2538ab05b1c","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T14:30:11Z","title_canon_sha256":"34ad6bf99c661fe44d3d0b3a0f37f3b63fb940fdc9dea47abdc7de2b29724c04"},"schema_version":"1.0","source":{"id":"1409.3088","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1409.3088","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"arxiv_version","alias_value":"1409.3088v2","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3088","created_at":"2026-05-18T02:35:46Z"},{"alias_kind":"pith_short_12","alias_value":"RUTMXNXSCB67","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RUTMXNXSCB67RXV6","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RUTMXNXS","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:89fe5f58a21f832c87f32ae615f71fcece434d6bf7eb459d492d2ed572cec523","target":"graph","created_at":"2026-05-18T02:35:46Z","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":"It is generally believed that the decay mode $B\\to K^*\\ell^+\\ell^-$ is one of the best modes to search for physics beyond the standard model. The angular distribution enables the independent measurement of several observables as a function of the dilepton invariant mass. The plethora of observables so obtained enable unique tests of the standard model contributions. We start by writing the most general parametric form of the standard model amplitude for $B\\to K^*\\ell^+\\ell^-$ taking into account comprehensively all contributions within SM. These include all short-distance and long-distance eff","authors_text":"Diganta Das, Rahul Sinha, Rusa Mandal","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T14:30:11Z","title":"Testing New Physics Effects in $B \\to K^*\\ell^+\\ell^-$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3088","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":"sha256:5f5a82172c341565afd892ed6294dc4adf7c6b9bf99f9c4d9115822885d81629","target":"record","created_at":"2026-05-18T02:35:46Z","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":"0989db013574a476afc32d23e55332a5a53fac5e5f49cd122b8ca2538ab05b1c","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-10T14:30:11Z","title_canon_sha256":"34ad6bf99c661fe44d3d0b3a0f37f3b63fb940fdc9dea47abdc7de2b29724c04"},"schema_version":"1.0","source":{"id":"1409.3088","kind":"arxiv","version":2}},"canonical_sha256":"8d26cbb6f2107df8debe46dc8f8c841e26c162889404d445dff1a8471e55b800","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8d26cbb6f2107df8debe46dc8f8c841e26c162889404d445dff1a8471e55b800","first_computed_at":"2026-05-18T02:35:46.961617Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:35:46.961617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rzCl/W1CZTYr709IXlclEo4wufTRa1ZV/osQWS5dz3ntEmljKr7HgCRXODCDW7ZhrniRKwUcinqb3z5crWaVBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:35:46.962159Z","signed_message":"canonical_sha256_bytes"},"source_id":"1409.3088","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5f5a82172c341565afd892ed6294dc4adf7c6b9bf99f9c4d9115822885d81629","sha256:89fe5f58a21f832c87f32ae615f71fcece434d6bf7eb459d492d2ed572cec523"],"state_sha256":"a0602cf42dba86ccb9e4ac508365574a21fdeeb735f381078202435390cb48fc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z9/YbqJnSYL4wCqGDw6Ssw3Kcp17jQ+vnnbzZmUNeR2OleVGVmvJl/Lpls6yyNfVcyuXFQZjlvg3wfsyiS1uDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T05:09:25.591963Z","bundle_sha256":"25e5c76854871e6d27061d5fa2ed41d21a9f6224f932b114b97390ecdd920450"}}