{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:MLUI2FBZGW5P6NKLDESUEFMHJC","short_pith_number":"pith:MLUI2FBZ","canonical_record":{"source":{"id":"hep-ph/0304100","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-10T12:25:18Z","cross_cats_sorted":[],"title_canon_sha256":"730859c79ecf39506e3135946f21d6ce8a959555dd1fe5c50dec2a1f4514d0d4","abstract_canon_sha256":"7d186fdd21ff09972698755a255657d45b6ba71d5cdca120ef9379f8905e1422"},"schema_version":"1.0"},"canonical_sha256":"62e88d143935baff354b192542158748a6c0b4d8f8f190e0e52248cec098a87c","source":{"kind":"arxiv","id":"hep-ph/0304100","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0304100","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0304100v1","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0304100","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"pith_short_12","alias_value":"MLUI2FBZGW5P","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MLUI2FBZGW5P6NKL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MLUI2FBZ","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:MLUI2FBZGW5P6NKLDESUEFMHJC","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0304100","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-10T12:25:18Z","cross_cats_sorted":[],"title_canon_sha256":"730859c79ecf39506e3135946f21d6ce8a959555dd1fe5c50dec2a1f4514d0d4","abstract_canon_sha256":"7d186fdd21ff09972698755a255657d45b6ba71d5cdca120ef9379f8905e1422"},"schema_version":"1.0"},"canonical_sha256":"62e88d143935baff354b192542158748a6c0b4d8f8f190e0e52248cec098a87c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:36.820188Z","signature_b64":"hdTVhiTbn+1LzN0zoC3otjjpy49/USweflKdirI0bzwPilDTEC6Qi92FFBE5WOL2I1o78GFF4WSZbmPRxVNWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62e88d143935baff354b192542158748a6c0b4d8f8f190e0e52248cec098a87c","last_reissued_at":"2026-05-18T04:13:36.819514Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:36.819514Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0304100","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":"2026-05-18T04:13:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hpOtED4e8oyYizM50dzecWV2LJ9Jav+cm3Br2ptO2ZSQxKEKYoZ+22/qFlL83K4W70TwMsR92WNuMKmsI7LGAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:39:41.394238Z"},"content_sha256":"5269433bfd4bb250280205fc6d08251e61be70b0b34ec5b8eddb72067e4d3e46","schema_version":"1.0","event_id":"sha256:5269433bfd4bb250280205fc6d08251e61be70b0b34ec5b8eddb72067e4d3e46"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:MLUI2FBZGW5P6NKLDESUEFMHJC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New physics effects in the rare B_s --> \\gamma \\ell^+ \\ell^- decays with polarized photon","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. B. Sirvanli, G. Turan, U. O. Yilmaz","submitted_at":"2003-04-10T12:25:18Z","abstract_excerpt":"Using the most general model independent form of the effective Hamiltonian, the rare B_s --> \\gamma \\ell^+ \\ell^- decays are studied by taking into account the polarization of the photon. The total and the differential branching ratios for these decays, when photon is in the positive and negative helicity states, are presented. Dependence of these observables on the new Wilson coefficients are studied. It is also investigated the sensitivity of \"photon polarization asymmetry\" in B_s --> \\gamma \\ell^+ \\ell^- decays to the new Wilson coefficients. It has been shown that all these physical observ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0304100","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":"2026-05-18T04:13:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u1fKfaTwjLfV+BJ4cwbp5lMhwXLrZDdGLmd+rkpN6K6SHzJxmN1lHoONSb6G2GjgwHaCEbPtJ3Lpp3NxgUP/DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:39:41.394600Z"},"content_sha256":"2e48a2b630b49e4d54ed4601f724071a72e084da34ed083dfedcb34b3203365c","schema_version":"1.0","event_id":"sha256:2e48a2b630b49e4d54ed4601f724071a72e084da34ed083dfedcb34b3203365c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/bundle.json","state_url":"https://pith.science/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/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":"2026-06-01T13:39:41Z","links":{"resolver":"https://pith.science/pith/MLUI2FBZGW5P6NKLDESUEFMHJC","bundle":"https://pith.science/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/bundle.json","state":"https://pith.science/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MLUI2FBZGW5P6NKLDESUEFMHJC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:MLUI2FBZGW5P6NKLDESUEFMHJC","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":"7d186fdd21ff09972698755a255657d45b6ba71d5cdca120ef9379f8905e1422","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-10T12:25:18Z","title_canon_sha256":"730859c79ecf39506e3135946f21d6ce8a959555dd1fe5c50dec2a1f4514d0d4"},"schema_version":"1.0","source":{"id":"hep-ph/0304100","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0304100","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0304100v1","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0304100","created_at":"2026-05-18T04:13:36Z"},{"alias_kind":"pith_short_12","alias_value":"MLUI2FBZGW5P","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"MLUI2FBZGW5P6NKL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"MLUI2FBZ","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:2e48a2b630b49e4d54ed4601f724071a72e084da34ed083dfedcb34b3203365c","target":"graph","created_at":"2026-05-18T04:13:36Z","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":"Using the most general model independent form of the effective Hamiltonian, the rare B_s --> \\gamma \\ell^+ \\ell^- decays are studied by taking into account the polarization of the photon. The total and the differential branching ratios for these decays, when photon is in the positive and negative helicity states, are presented. Dependence of these observables on the new Wilson coefficients are studied. It is also investigated the sensitivity of \"photon polarization asymmetry\" in B_s --> \\gamma \\ell^+ \\ell^- decays to the new Wilson coefficients. It has been shown that all these physical observ","authors_text":"B. B. Sirvanli, G. Turan, U. O. Yilmaz","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2003-04-10T12:25:18Z","title":"New physics effects in the rare B_s --> \\gamma \\ell^+ \\ell^- decays with polarized photon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0304100","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":"sha256:5269433bfd4bb250280205fc6d08251e61be70b0b34ec5b8eddb72067e4d3e46","target":"record","created_at":"2026-05-18T04:13:36Z","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":"7d186fdd21ff09972698755a255657d45b6ba71d5cdca120ef9379f8905e1422","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2003-04-10T12:25:18Z","title_canon_sha256":"730859c79ecf39506e3135946f21d6ce8a959555dd1fe5c50dec2a1f4514d0d4"},"schema_version":"1.0","source":{"id":"hep-ph/0304100","kind":"arxiv","version":1}},"canonical_sha256":"62e88d143935baff354b192542158748a6c0b4d8f8f190e0e52248cec098a87c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"62e88d143935baff354b192542158748a6c0b4d8f8f190e0e52248cec098a87c","first_computed_at":"2026-05-18T04:13:36.819514Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:13:36.819514Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hdTVhiTbn+1LzN0zoC3otjjpy49/USweflKdirI0bzwPilDTEC6Qi92FFBE5WOL2I1o78GFF4WSZbmPRxVNWCw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:13:36.820188Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0304100","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5269433bfd4bb250280205fc6d08251e61be70b0b34ec5b8eddb72067e4d3e46","sha256:2e48a2b630b49e4d54ed4601f724071a72e084da34ed083dfedcb34b3203365c"],"state_sha256":"1d588d812b5fc195b1f331686c112356163984c1132f7f7b1cd81f67420eda62"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IzeomP7CGgfO+2Xih+qX2MCX7mhzXfy9wW1gYAVq1+YYNSLlfoiC7QWTXp7XStg908a4mYUtznYSm3JGXloXCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:39:41.396545Z","bundle_sha256":"3f94fc1aba0f017df9c873c2598eaa1f5889ef86e152c8b159a2e5fd4fa75513"}}