{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:LRK7BZDPJJEQ76HSOK7UZTSFZR","short_pith_number":"pith:LRK7BZDP","canonical_record":{"source":{"id":"hep-ph/0209191","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-09-17T16:25:26Z","cross_cats_sorted":[],"title_canon_sha256":"5a2ad1e3a5363163a91aeb1e438da0619f26d37749c9ab41649f537529eebaaa","abstract_canon_sha256":"17199a8a27ca2ba9ca330c0c5d90c09f433f775f127f33b91505853fb3eb4e76"},"schema_version":"1.0"},"canonical_sha256":"5c55f0e46f4a490ff8f272bf4cce45cc7ed6fcd2e43e767c27aba50489ab7c39","source":{"kind":"arxiv","id":"hep-ph/0209191","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0209191","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0209191v1","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0209191","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_12","alias_value":"LRK7BZDPJJEQ","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"LRK7BZDPJJEQ76HS","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"LRK7BZDP","created_at":"2026-07-04T14:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:LRK7BZDPJJEQ76HSOK7UZTSFZR","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0209191","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-09-17T16:25:26Z","cross_cats_sorted":[],"title_canon_sha256":"5a2ad1e3a5363163a91aeb1e438da0619f26d37749c9ab41649f537529eebaaa","abstract_canon_sha256":"17199a8a27ca2ba9ca330c0c5d90c09f433f775f127f33b91505853fb3eb4e76"},"schema_version":"1.0"},"canonical_sha256":"5c55f0e46f4a490ff8f272bf4cce45cc7ed6fcd2e43e767c27aba50489ab7c39","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:28:25.998441Z","signature_b64":"9nM+G/wv4vyt32OPLgs/bsSckefD1IwZsI+w/f3LS6b157H1xKoUteAsxG4WgG5qH+nBPJTXraqTypu+A1OfBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c55f0e46f4a490ff8f272bf4cce45cc7ed6fcd2e43e767c27aba50489ab7c39","last_reissued_at":"2026-07-04T14:28:25.998082Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:28:25.998082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0209191","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":"2026-07-04T14:28:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tmCsUXpQY4AyjESR8YbZu1JxQVPXXLzQAb7SXRmKSrvQLH8QSlA4pkaGFimV0tLREFafCI/6qaCjn+sUFVQADA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T18:55:50.688753Z"},"content_sha256":"02f5a18c69e843de74950420b590e4c9f34e58463ad165d72bf763b0f9891963","schema_version":"1.0","event_id":"sha256:02f5a18c69e843de74950420b590e4c9f34e58463ad165d72bf763b0f9891963"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:LRK7BZDPJJEQ76HSOK7UZTSFZR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"$B \\to K^* \\ell^+ \\ell^-\\big (\\rho \\ell \\nu_{\\ell}\\big)$ helicity analysis in the LEET","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Salim Safir (DESY, Hamburg)","submitted_at":"2002-09-17T16:25:26Z","abstract_excerpt":"We calculate the independent helicity amplitudes in the decays $B \\to K^* \\ell^+ \\ell^-$ and $B \\to \\rho \\ell \\nu_\\ell$ in the so-called Large-Energy-Effective-Theory (LEET). Taking into account the dominant $O(\\alpha_s)$ and SU(3) symmetry-breaking effects, we calculate various single (and total) distributions in these decays making use of the presently available data and decay form factors calculated in the QCD sum rule approach. Differential decay rates in the dilepton invariant mass and the Forward-Backward asymmetry in $B \\to K^* \\ell^+ \\ell^-$ are worked out. Measurements of the ratios $"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0209191","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0209191/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":"2026-07-04T14:28:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HogXWasZn3iDwRiPXUh7LwnsNsquh82rUw/jU7O1YwKHvzDFMFOhbAy4ixw+228n4i+ahwoUCCZP05XTDPxzDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T18:55:50.689437Z"},"content_sha256":"30383479a9b224ab505ccff076518b933260ee3b5522269e36673572a883a51c","schema_version":"1.0","event_id":"sha256:30383479a9b224ab505ccff076518b933260ee3b5522269e36673572a883a51c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/bundle.json","state_url":"https://pith.science/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/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":"2026-08-06T18:55:50Z","links":{"resolver":"https://pith.science/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR","bundle":"https://pith.science/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/bundle.json","state":"https://pith.science/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LRK7BZDPJJEQ76HSOK7UZTSFZR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:LRK7BZDPJJEQ76HSOK7UZTSFZR","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":"17199a8a27ca2ba9ca330c0c5d90c09f433f775f127f33b91505853fb3eb4e76","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2002-09-17T16:25:26Z","title_canon_sha256":"5a2ad1e3a5363163a91aeb1e438da0619f26d37749c9ab41649f537529eebaaa"},"schema_version":"1.0","source":{"id":"hep-ph/0209191","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0209191","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0209191v1","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0209191","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_12","alias_value":"LRK7BZDPJJEQ","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"LRK7BZDPJJEQ76HS","created_at":"2026-07-04T14:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"LRK7BZDP","created_at":"2026-07-04T14:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:30383479a9b224ab505ccff076518b933260ee3b5522269e36673572a883a51c","target":"graph","created_at":"2026-07-04T14:28:25Z","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/hep-ph/0209191/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the independent helicity amplitudes in the decays $B \\to K^* \\ell^+ \\ell^-$ and $B \\to \\rho \\ell \\nu_\\ell$ in the so-called Large-Energy-Effective-Theory (LEET). Taking into account the dominant $O(\\alpha_s)$ and SU(3) symmetry-breaking effects, we calculate various single (and total) distributions in these decays making use of the presently available data and decay form factors calculated in the QCD sum rule approach. Differential decay rates in the dilepton invariant mass and the Forward-Backward asymmetry in $B \\to K^* \\ell^+ \\ell^-$ are worked out. Measurements of the ratios $","authors_text":"A. Salim Safir (DESY, Hamburg)","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2002-09-17T16:25:26Z","title":"$B \\to K^* \\ell^+ \\ell^-\\big (\\rho \\ell \\nu_{\\ell}\\big)$ helicity analysis in the LEET"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0209191","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":"sha256:02f5a18c69e843de74950420b590e4c9f34e58463ad165d72bf763b0f9891963","target":"record","created_at":"2026-07-04T14:28:25Z","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":"17199a8a27ca2ba9ca330c0c5d90c09f433f775f127f33b91505853fb3eb4e76","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2002-09-17T16:25:26Z","title_canon_sha256":"5a2ad1e3a5363163a91aeb1e438da0619f26d37749c9ab41649f537529eebaaa"},"schema_version":"1.0","source":{"id":"hep-ph/0209191","kind":"arxiv","version":1}},"canonical_sha256":"5c55f0e46f4a490ff8f272bf4cce45cc7ed6fcd2e43e767c27aba50489ab7c39","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c55f0e46f4a490ff8f272bf4cce45cc7ed6fcd2e43e767c27aba50489ab7c39","first_computed_at":"2026-07-04T14:28:25.998082Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:28:25.998082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9nM+G/wv4vyt32OPLgs/bsSckefD1IwZsI+w/f3LS6b157H1xKoUteAsxG4WgG5qH+nBPJTXraqTypu+A1OfBQ==","signature_status":"signed_v1","signed_at":"2026-07-04T14:28:25.998441Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0209191","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:02f5a18c69e843de74950420b590e4c9f34e58463ad165d72bf763b0f9891963","sha256:30383479a9b224ab505ccff076518b933260ee3b5522269e36673572a883a51c"],"state_sha256":"32fca1ecff1c427fb46871f9602e944c2383e1dbb4bc399866d53f32188374e2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hi/FNV6BPhQK16l2Fk6GqctwRVtLU2knOEx6Bgzwygmj3H9Ly6Z1tziUZL+8rvK+8Z+Tmx3t5osefCN0xtc0AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T18:55:50.697613Z","bundle_sha256":"ac06d64ad64f3d8738555b172b09ed044b0d61e188545274b64d19d8b498a67d"}}