{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:2FB5UW6PS672Y5GXV7PFZB4YG7","short_pith_number":"pith:2FB5UW6P","canonical_record":{"source":{"id":"1805.08222","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-21T18:00:03Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3e08055f5e267976b8b81304369468a9350c770e617e1a2a1d22a439b5bfb0ed","abstract_canon_sha256":"0fb32f22d2b1b7e6f3f43af5a124fac4fe22534115e5d838ec55e2ec19758c29"},"schema_version":"1.0"},"canonical_sha256":"d143da5bcf97bfac74d7afde5c879837e9953fa7bee39d36d12a25b4c57b32ed","source":{"kind":"arxiv","id":"1805.08222","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.08222","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"arxiv_version","alias_value":"1805.08222v3","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.08222","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"pith_short_12","alias_value":"2FB5UW6PS672","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"2FB5UW6PS672Y5GX","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"2FB5UW6P","created_at":"2026-05-18T12:32:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:2FB5UW6PS672Y5GXV7PFZB4YG7","target":"record","payload":{"canonical_record":{"source":{"id":"1805.08222","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-21T18:00:03Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3e08055f5e267976b8b81304369468a9350c770e617e1a2a1d22a439b5bfb0ed","abstract_canon_sha256":"0fb32f22d2b1b7e6f3f43af5a124fac4fe22534115e5d838ec55e2ec19758c29"},"schema_version":"1.0"},"canonical_sha256":"d143da5bcf97bfac74d7afde5c879837e9953fa7bee39d36d12a25b4c57b32ed","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:20.923207Z","signature_b64":"GKvX7iG0XPL7u0NrISwHVuvb0QyEP+6QsZozwML9RXCgkZ7VEO8NmRJtbfQEUYLx4dLecO8XCcoMeppzcqBsAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d143da5bcf97bfac74d7afde5c879837e9953fa7bee39d36d12a25b4c57b32ed","last_reissued_at":"2026-05-17T23:47:20.922821Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:20.922821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.08222","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":"2026-05-17T23:47:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Tp36yoIZu/j81O04lYYiptkC6U47kX+y/kyIdaoCnMpGyHSra50qclcDSqX4oT6h3dUAv8/PL5EW/uXly/JcBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:13:47.422611Z"},"content_sha256":"2c36059f716967ff314ae1810d13e425241c9a1c8fe9b5dc028b87ccada542de","schema_version":"1.0","event_id":"sha256:2c36059f716967ff314ae1810d13e425241c9a1c8fe9b5dc028b87ccada542de"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:2FB5UW6PS672Y5GXV7PFZB4YG7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"$b \\to c \\tau \\nu_{\\tau}$ Decays: A Catalogue to Compare, Constrain, and Correlate New Physics Effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Soumitra Nandi, Srimoy Bhattacharya, Sunando Kumar Patra","submitted_at":"2018-05-21T18:00:03Z","abstract_excerpt":"In this article, we have predicted the standard model (SM) values of the asymmetric and angular observables in $B\\to D^{(\\ast)}\\tau\\nu_{\\tau}$ decays, using the results of the new up-to-date analysis in $B\\to D^{(*)}\\ell\\nu_{\\ell}$. We have also revisited the SM prediction of the inclusive ratio $\\mathcal{R}_{X_c}$, and have given its values in different schemes of the charm quark mass. This is the first analysis which includes all the known corrections in the SM. In addition, we have analysed the $b\\to c\\tau\\nu_\\tau$ decay modes in a model-independent framework of effective field theory beyon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.08222","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":"2026-05-17T23:47:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FEYJm7QoFEenN7n9YZHbDFOyWos0s3ifbsy4/jetF5w4WvMkp0urbxaS454mVSP9gZaMdZZXWsTqEbbQob+EBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T18:13:47.423358Z"},"content_sha256":"43c9f3a16eaaacaaca293b1379db0518f586409ae03ad69fb99840d24100efc2","schema_version":"1.0","event_id":"sha256:43c9f3a16eaaacaaca293b1379db0518f586409ae03ad69fb99840d24100efc2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/bundle.json","state_url":"https://pith.science/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/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":"2026-06-09T18:13:47Z","links":{"resolver":"https://pith.science/pith/2FB5UW6PS672Y5GXV7PFZB4YG7","bundle":"https://pith.science/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/bundle.json","state":"https://pith.science/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2FB5UW6PS672Y5GXV7PFZB4YG7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:2FB5UW6PS672Y5GXV7PFZB4YG7","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":"0fb32f22d2b1b7e6f3f43af5a124fac4fe22534115e5d838ec55e2ec19758c29","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-21T18:00:03Z","title_canon_sha256":"3e08055f5e267976b8b81304369468a9350c770e617e1a2a1d22a439b5bfb0ed"},"schema_version":"1.0","source":{"id":"1805.08222","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.08222","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"arxiv_version","alias_value":"1805.08222v3","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.08222","created_at":"2026-05-17T23:47:20Z"},{"alias_kind":"pith_short_12","alias_value":"2FB5UW6PS672","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"2FB5UW6PS672Y5GX","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"2FB5UW6P","created_at":"2026-05-18T12:32:02Z"}],"graph_snapshots":[{"event_id":"sha256:43c9f3a16eaaacaaca293b1379db0518f586409ae03ad69fb99840d24100efc2","target":"graph","created_at":"2026-05-17T23:47:20Z","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":"In this article, we have predicted the standard model (SM) values of the asymmetric and angular observables in $B\\to D^{(\\ast)}\\tau\\nu_{\\tau}$ decays, using the results of the new up-to-date analysis in $B\\to D^{(*)}\\ell\\nu_{\\ell}$. We have also revisited the SM prediction of the inclusive ratio $\\mathcal{R}_{X_c}$, and have given its values in different schemes of the charm quark mass. This is the first analysis which includes all the known corrections in the SM. In addition, we have analysed the $b\\to c\\tau\\nu_\\tau$ decay modes in a model-independent framework of effective field theory beyon","authors_text":"Soumitra Nandi, Srimoy Bhattacharya, Sunando Kumar Patra","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-21T18:00:03Z","title":"$b \\to c \\tau \\nu_{\\tau}$ Decays: A Catalogue to Compare, Constrain, and Correlate New Physics Effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.08222","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":"sha256:2c36059f716967ff314ae1810d13e425241c9a1c8fe9b5dc028b87ccada542de","target":"record","created_at":"2026-05-17T23:47:20Z","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":"0fb32f22d2b1b7e6f3f43af5a124fac4fe22534115e5d838ec55e2ec19758c29","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-21T18:00:03Z","title_canon_sha256":"3e08055f5e267976b8b81304369468a9350c770e617e1a2a1d22a439b5bfb0ed"},"schema_version":"1.0","source":{"id":"1805.08222","kind":"arxiv","version":3}},"canonical_sha256":"d143da5bcf97bfac74d7afde5c879837e9953fa7bee39d36d12a25b4c57b32ed","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d143da5bcf97bfac74d7afde5c879837e9953fa7bee39d36d12a25b4c57b32ed","first_computed_at":"2026-05-17T23:47:20.922821Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:47:20.922821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GKvX7iG0XPL7u0NrISwHVuvb0QyEP+6QsZozwML9RXCgkZ7VEO8NmRJtbfQEUYLx4dLecO8XCcoMeppzcqBsAQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:47:20.923207Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.08222","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2c36059f716967ff314ae1810d13e425241c9a1c8fe9b5dc028b87ccada542de","sha256:43c9f3a16eaaacaaca293b1379db0518f586409ae03ad69fb99840d24100efc2"],"state_sha256":"593372ba4af70bf42d38d62bedf761b8f8606b154cb4f3b48e3214cfd90c3212"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1+VGcSvLfCJK25spfluJ5Xa4B9YfGutOHMQMujn8635Fafcq8jCoRCn/i7b32nxkPG4RRuYJZSRsYF7vmGp0CQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T18:13:47.427163Z","bundle_sha256":"dc75aa2418379d4a89b6081b4f819216c88977596ce11808699196d6be203024"}}