{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:OLSY2W4H7O234H3KUUFIHYKN5C","short_pith_number":"pith:OLSY2W4H","canonical_record":{"source":{"id":"1009.4165","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-21T18:15:48Z","cross_cats_sorted":[],"title_canon_sha256":"dd39ffa472f62ca38330d8e860f2a3af91b58e3ea3b41cc3303a2cfc71077e99","abstract_canon_sha256":"b287dfbb49777c5c33b2935a0946d84677077375ce62d4a6e9f3b24ae14c699f"},"schema_version":"1.0"},"canonical_sha256":"72e58d5b87fbb5be1f6aa50a83e14de8b46f31de29d1b91ea6fb53a223de6ecb","source":{"kind":"arxiv","id":"1009.4165","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.4165","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"arxiv_version","alias_value":"1009.4165v3","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.4165","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"pith_short_12","alias_value":"OLSY2W4H7O23","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"OLSY2W4H7O234H3K","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"OLSY2W4H","created_at":"2026-05-18T12:26:12Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:OLSY2W4H7O234H3KUUFIHYKN5C","target":"record","payload":{"canonical_record":{"source":{"id":"1009.4165","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-21T18:15:48Z","cross_cats_sorted":[],"title_canon_sha256":"dd39ffa472f62ca38330d8e860f2a3af91b58e3ea3b41cc3303a2cfc71077e99","abstract_canon_sha256":"b287dfbb49777c5c33b2935a0946d84677077375ce62d4a6e9f3b24ae14c699f"},"schema_version":"1.0"},"canonical_sha256":"72e58d5b87fbb5be1f6aa50a83e14de8b46f31de29d1b91ea6fb53a223de6ecb","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:23:23.091953Z","signature_b64":"gMbQ4776GV14ISrn6axP27jZzHu+tvUQMOhA7Ci74Wc7Un5rzNmhs+CyikKEUEw2L3l3jomOrql9o+kcHm9TCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72e58d5b87fbb5be1f6aa50a83e14de8b46f31de29d1b91ea6fb53a223de6ecb","last_reissued_at":"2026-05-18T04:23:23.091330Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:23:23.091330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1009.4165","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:23:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s3z7mriiY77JFhcb7cMheoYxwRP8AGLPcQVX7EZSana5STW2tIF9t8LfrjyILr8506AKyJ1s6bQ1Kx2iCkDFBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T16:23:11.467133Z"},"content_sha256":"b1332218f2fc31159462724c7ba73df9d106416a14e47274a40064607101a157","schema_version":"1.0","event_id":"sha256:b1332218f2fc31159462724c7ba73df9d106416a14e47274a40064607101a157"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:OLSY2W4H7O234H3KUUFIHYKN5C","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Forward-backward asymmetry of top quark in unparticle physics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chuan-Hung Chen, C.S.Kim, G.Cvetic","submitted_at":"2010-09-21T18:15:48Z","abstract_excerpt":"The updated CDF measurement of the forward-backward asymmetry (FBA) in the top quark production p{bar p} -> t{bar t} at Tevatron (with the CMS energy 1.96 TeV) shows a deviation of 2*sigma from the value predicted by the Standard QCD Model. We present calculation of this quantity in the scenario where colored unparticle physics contributes to the s-channel of the process, and obtain the regions in the plane of the unparticle parameters lambda and dU which give the values of the FBA and of the total t{bar t} production cross section compatible with the present measurements."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.4165","kind":"arxiv","version":3},"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":"2026-05-18T04:23:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iX7g8JlKOFt+eNJ8e8sz2l7kJENBjnUPXORu/J5UE1z5deW167yQu626xeIUN5R6R8L6JAMJTKTzRFSFq2nKBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T16:23:11.467496Z"},"content_sha256":"3dc176f25c9cbabde3c1d3a800f832e249b7a416195442a3f0951afd5da32ba7","schema_version":"1.0","event_id":"sha256:3dc176f25c9cbabde3c1d3a800f832e249b7a416195442a3f0951afd5da32ba7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OLSY2W4H7O234H3KUUFIHYKN5C/bundle.json","state_url":"https://pith.science/pith/OLSY2W4H7O234H3KUUFIHYKN5C/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OLSY2W4H7O234H3KUUFIHYKN5C/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":"2026-06-20T16:23:11Z","links":{"resolver":"https://pith.science/pith/OLSY2W4H7O234H3KUUFIHYKN5C","bundle":"https://pith.science/pith/OLSY2W4H7O234H3KUUFIHYKN5C/bundle.json","state":"https://pith.science/pith/OLSY2W4H7O234H3KUUFIHYKN5C/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OLSY2W4H7O234H3KUUFIHYKN5C/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:OLSY2W4H7O234H3KUUFIHYKN5C","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":"b287dfbb49777c5c33b2935a0946d84677077375ce62d4a6e9f3b24ae14c699f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-21T18:15:48Z","title_canon_sha256":"dd39ffa472f62ca38330d8e860f2a3af91b58e3ea3b41cc3303a2cfc71077e99"},"schema_version":"1.0","source":{"id":"1009.4165","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.4165","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"arxiv_version","alias_value":"1009.4165v3","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.4165","created_at":"2026-05-18T04:23:23Z"},{"alias_kind":"pith_short_12","alias_value":"OLSY2W4H7O23","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_16","alias_value":"OLSY2W4H7O234H3K","created_at":"2026-05-18T12:26:12Z"},{"alias_kind":"pith_short_8","alias_value":"OLSY2W4H","created_at":"2026-05-18T12:26:12Z"}],"graph_snapshots":[{"event_id":"sha256:3dc176f25c9cbabde3c1d3a800f832e249b7a416195442a3f0951afd5da32ba7","target":"graph","created_at":"2026-05-18T04:23:23Z","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":"The updated CDF measurement of the forward-backward asymmetry (FBA) in the top quark production p{bar p} -> t{bar t} at Tevatron (with the CMS energy 1.96 TeV) shows a deviation of 2*sigma from the value predicted by the Standard QCD Model. We present calculation of this quantity in the scenario where colored unparticle physics contributes to the s-channel of the process, and obtain the regions in the plane of the unparticle parameters lambda and dU which give the values of the FBA and of the total t{bar t} production cross section compatible with the present measurements.","authors_text":"Chuan-Hung Chen, C.S.Kim, G.Cvetic","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-21T18:15:48Z","title":"Forward-backward asymmetry of top quark in unparticle physics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.4165","kind":"arxiv","version":3},"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:b1332218f2fc31159462724c7ba73df9d106416a14e47274a40064607101a157","target":"record","created_at":"2026-05-18T04:23:23Z","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":"b287dfbb49777c5c33b2935a0946d84677077375ce62d4a6e9f3b24ae14c699f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-21T18:15:48Z","title_canon_sha256":"dd39ffa472f62ca38330d8e860f2a3af91b58e3ea3b41cc3303a2cfc71077e99"},"schema_version":"1.0","source":{"id":"1009.4165","kind":"arxiv","version":3}},"canonical_sha256":"72e58d5b87fbb5be1f6aa50a83e14de8b46f31de29d1b91ea6fb53a223de6ecb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"72e58d5b87fbb5be1f6aa50a83e14de8b46f31de29d1b91ea6fb53a223de6ecb","first_computed_at":"2026-05-18T04:23:23.091330Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:23:23.091330Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gMbQ4776GV14ISrn6axP27jZzHu+tvUQMOhA7Ci74Wc7Un5rzNmhs+CyikKEUEw2L3l3jomOrql9o+kcHm9TCA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:23:23.091953Z","signed_message":"canonical_sha256_bytes"},"source_id":"1009.4165","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b1332218f2fc31159462724c7ba73df9d106416a14e47274a40064607101a157","sha256:3dc176f25c9cbabde3c1d3a800f832e249b7a416195442a3f0951afd5da32ba7"],"state_sha256":"57f21a1b45ad732f0c17b83562a7d398778ebff137f71d09a473a83e7da163ea"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xWs2jyv/Dm77ziJx1x1fHyNrirpJ3BOK+wt6+fJk1m2Dpduge2M8cegNSlOPvzoDRL8d2ON+ZNjgiDQ2UL15BA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T16:23:11.469426Z","bundle_sha256":"edf8eaa876c833125bc2cb8ae986c87e7ec1a1937f8ecd29eaa53302af5e89f9"}}