{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:TNB64DV3E7PCLM2FZ6FXFGOEIB","short_pith_number":"pith:TNB64DV3","canonical_record":{"source":{"id":"1505.07977","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-29T10:03:20Z","cross_cats_sorted":[],"title_canon_sha256":"472c21f67ee136dfac9f63508a224e3d2a2241110765531b6dc4e95ebfaa621d","abstract_canon_sha256":"0730dcdcc755e116b27180298aafbcf6d6501b708f9c5f7d5a9d2d410e323124"},"schema_version":"1.0"},"canonical_sha256":"9b43ee0ebb27de25b345cf8b7299c440637a8eb8360a7f9fa4db1c8e423bc542","source":{"kind":"arxiv","id":"1505.07977","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.07977","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"arxiv_version","alias_value":"1505.07977v1","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.07977","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"pith_short_12","alias_value":"TNB64DV3E7PC","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_16","alias_value":"TNB64DV3E7PCLM2F","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_8","alias_value":"TNB64DV3","created_at":"2026-05-18T12:29:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:TNB64DV3E7PCLM2FZ6FXFGOEIB","target":"record","payload":{"canonical_record":{"source":{"id":"1505.07977","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-29T10:03:20Z","cross_cats_sorted":[],"title_canon_sha256":"472c21f67ee136dfac9f63508a224e3d2a2241110765531b6dc4e95ebfaa621d","abstract_canon_sha256":"0730dcdcc755e116b27180298aafbcf6d6501b708f9c5f7d5a9d2d410e323124"},"schema_version":"1.0"},"canonical_sha256":"9b43ee0ebb27de25b345cf8b7299c440637a8eb8360a7f9fa4db1c8e423bc542","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:16.535712Z","signature_b64":"8hAtAfV/vL8TrmYxQoIjsyss0/G2df9d/6UNcRbeKxAmV50sFFysHrmAYJf3+iEMcNwLcsxaeieSl9HgvdDMAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b43ee0ebb27de25b345cf8b7299c440637a8eb8360a7f9fa4db1c8e423bc542","last_reissued_at":"2026-05-18T01:34:16.534942Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:16.534942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.07977","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":"2026-05-18T01:34:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sOAOXPVpFhHNogK1fvI6eoYJ0E9ro99BLrEqSbjE0csP49sfPyas631IJmjcC/8PQ5TJEYzdQu5sCHsz9FKPDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T21:59:07.402313Z"},"content_sha256":"62f7aae984580e12ba5cdf4e2a1c065e2f3070b02129b020fe2dd896e2dda8ce","schema_version":"1.0","event_id":"sha256:62f7aae984580e12ba5cdf4e2a1c065e2f3070b02129b020fe2dd896e2dda8ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:TNB64DV3E7PCLM2FZ6FXFGOEIB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Diagonal and transition magnetic moments of negative parity heavy baryons in QCD sum rules","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"(2) Ac{\\i}badem-Kad{\\i}k\\\"oy, (3) King Saud University/Riyadh/Saudi Arabia), K. Azizi (2), M. Savc{\\i} (1) ((1) Middle East Technical University/Ankara/Turkey, T. Barakat (3), T. M. Aliev (1)","submitted_at":"2015-05-29T10:03:20Z","abstract_excerpt":"Diagonal and transition magnetic moments of the negative parity, spin-1/2 heavy baryons are studied in framework of the light cone QCD sum rules. By constructing the sum rules for different Lorentz structures, the unwanted contributions coming from negative (positive) to positive (negative) parity transitions are removed. It is obtained that the magnetic moments of all baryons, except $\\Lambda_b^0$, $\\Sigma_c^+$ and $\\Xi_c^{\\prime +}$, are quite large. It is also found that the transition magnetic moments between neutral negative parity heavy $\\Xi_Q^{\\prime 0}$ and $\\Xi_Q^0$ baryons are very s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.07977","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":"2026-05-18T01:34:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rsQJgI/MRyZO6N7Q86ZsUXBxVXvSH5FxL0P8QHBqQYTFU5sHuIeyKt/JjJBAC9810Teh7OY8iyoIyyID0aHhAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T21:59:07.402707Z"},"content_sha256":"e1e06327284f5ee494d21b6a2ca5e5f8f5409e44c1169d4df023fbbb8559d6f1","schema_version":"1.0","event_id":"sha256:e1e06327284f5ee494d21b6a2ca5e5f8f5409e44c1169d4df023fbbb8559d6f1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/bundle.json","state_url":"https://pith.science/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/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":"2026-05-24T21:59:07Z","links":{"resolver":"https://pith.science/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB","bundle":"https://pith.science/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/bundle.json","state":"https://pith.science/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TNB64DV3E7PCLM2FZ6FXFGOEIB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:TNB64DV3E7PCLM2FZ6FXFGOEIB","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":"0730dcdcc755e116b27180298aafbcf6d6501b708f9c5f7d5a9d2d410e323124","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-29T10:03:20Z","title_canon_sha256":"472c21f67ee136dfac9f63508a224e3d2a2241110765531b6dc4e95ebfaa621d"},"schema_version":"1.0","source":{"id":"1505.07977","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.07977","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"arxiv_version","alias_value":"1505.07977v1","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.07977","created_at":"2026-05-18T01:34:16Z"},{"alias_kind":"pith_short_12","alias_value":"TNB64DV3E7PC","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_16","alias_value":"TNB64DV3E7PCLM2F","created_at":"2026-05-18T12:29:42Z"},{"alias_kind":"pith_short_8","alias_value":"TNB64DV3","created_at":"2026-05-18T12:29:42Z"}],"graph_snapshots":[{"event_id":"sha256:e1e06327284f5ee494d21b6a2ca5e5f8f5409e44c1169d4df023fbbb8559d6f1","target":"graph","created_at":"2026-05-18T01:34:16Z","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":"Diagonal and transition magnetic moments of the negative parity, spin-1/2 heavy baryons are studied in framework of the light cone QCD sum rules. By constructing the sum rules for different Lorentz structures, the unwanted contributions coming from negative (positive) to positive (negative) parity transitions are removed. It is obtained that the magnetic moments of all baryons, except $\\Lambda_b^0$, $\\Sigma_c^+$ and $\\Xi_c^{\\prime +}$, are quite large. It is also found that the transition magnetic moments between neutral negative parity heavy $\\Xi_Q^{\\prime 0}$ and $\\Xi_Q^0$ baryons are very s","authors_text":"(2) Ac{\\i}badem-Kad{\\i}k\\\"oy, (3) King Saud University/Riyadh/Saudi Arabia), K. Azizi (2), M. Savc{\\i} (1) ((1) Middle East Technical University/Ankara/Turkey, T. Barakat (3), T. M. Aliev (1)","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-29T10:03:20Z","title":"Diagonal and transition magnetic moments of negative parity heavy baryons in QCD sum rules"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.07977","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":"sha256:62f7aae984580e12ba5cdf4e2a1c065e2f3070b02129b020fe2dd896e2dda8ce","target":"record","created_at":"2026-05-18T01:34:16Z","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":"0730dcdcc755e116b27180298aafbcf6d6501b708f9c5f7d5a9d2d410e323124","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-05-29T10:03:20Z","title_canon_sha256":"472c21f67ee136dfac9f63508a224e3d2a2241110765531b6dc4e95ebfaa621d"},"schema_version":"1.0","source":{"id":"1505.07977","kind":"arxiv","version":1}},"canonical_sha256":"9b43ee0ebb27de25b345cf8b7299c440637a8eb8360a7f9fa4db1c8e423bc542","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9b43ee0ebb27de25b345cf8b7299c440637a8eb8360a7f9fa4db1c8e423bc542","first_computed_at":"2026-05-18T01:34:16.534942Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:34:16.534942Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8hAtAfV/vL8TrmYxQoIjsyss0/G2df9d/6UNcRbeKxAmV50sFFysHrmAYJf3+iEMcNwLcsxaeieSl9HgvdDMAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:34:16.535712Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.07977","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:62f7aae984580e12ba5cdf4e2a1c065e2f3070b02129b020fe2dd896e2dda8ce","sha256:e1e06327284f5ee494d21b6a2ca5e5f8f5409e44c1169d4df023fbbb8559d6f1"],"state_sha256":"29a3f961ddabcb73b9fb0897115587039f0c794624e5fc6c3803bc11081183a4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xFaFZr1zy1pmS90k0IcPWrMBhkp62qsbfGcK8BIXDW/2IoKcc5ayqN7Fjj6Dwvac38pNARydlujp7bTEZNg1Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T21:59:07.405530Z","bundle_sha256":"492aad61fb39c345b047b6837237ed5be94473d7e14e32319be47059752db12d"}}