{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:HKVXDNOEUFG44SHJEVIZIKHZJ7","short_pith_number":"pith:HKVXDNOE","canonical_record":{"source":{"id":"1711.02908","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T11:37:56Z","cross_cats_sorted":[],"title_canon_sha256":"9dc78a09f189ae89a242210c0c060d77c53075adedd5370284e200841f7cd18d","abstract_canon_sha256":"05434885c09dee375b77953fdf541410db66bbee940cfd8dd756c38bc5f7ba62"},"schema_version":"1.0"},"canonical_sha256":"3aab71b5c4a14dce48e925519428f94ff877d297817434f555c063d09e9e952d","source":{"kind":"arxiv","id":"1711.02908","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.02908","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"arxiv_version","alias_value":"1711.02908v2","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.02908","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"pith_short_12","alias_value":"HKVXDNOEUFG4","created_at":"2026-05-18T12:31:18Z"},{"alias_kind":"pith_short_16","alias_value":"HKVXDNOEUFG44SHJ","created_at":"2026-05-18T12:31:18Z"},{"alias_kind":"pith_short_8","alias_value":"HKVXDNOE","created_at":"2026-05-18T12:31:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:HKVXDNOEUFG44SHJEVIZIKHZJ7","target":"record","payload":{"canonical_record":{"source":{"id":"1711.02908","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T11:37:56Z","cross_cats_sorted":[],"title_canon_sha256":"9dc78a09f189ae89a242210c0c060d77c53075adedd5370284e200841f7cd18d","abstract_canon_sha256":"05434885c09dee375b77953fdf541410db66bbee940cfd8dd756c38bc5f7ba62"},"schema_version":"1.0"},"canonical_sha256":"3aab71b5c4a14dce48e925519428f94ff877d297817434f555c063d09e9e952d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:05.035763Z","signature_b64":"nNdRM/WfgU3OyIhdP82t0FiLhw5mpIqa7x78dMACapOBOOPYMjHvwL80kMEeHRz8VyDiEHC/RymeDFs5cH5lDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3aab71b5c4a14dce48e925519428f94ff877d297817434f555c063d09e9e952d","last_reissued_at":"2026-05-18T00:04:05.035077Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:05.035077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.02908","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:04:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EANbg6CVWJe9ayPp0sKg2ur7JfDCIyU9cKD2hQ3Zitf2utiUa7tU+14QJSfOET5U2Jz6FxNFNuAHktb3AgajBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T05:47:02.026668Z"},"content_sha256":"cbef81c95a144574bd83d97a1c5fe29f8066cffaa13028022bd92b186af24379","schema_version":"1.0","event_id":"sha256:cbef81c95a144574bd83d97a1c5fe29f8066cffaa13028022bd92b186af24379"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:HKVXDNOEUFG44SHJEVIZIKHZJ7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Unparticle effects on $B\\to D^{(*)}\\tau\\nu$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jong-Phil Lee","submitted_at":"2017-11-08T11:37:56Z","abstract_excerpt":"We examine the possible unparticle effects on $R(D^{(*)})$ associated with $B\\to D^{(*)}\\tau\\nu$ decays by minimum-$\\chi^2$ fitting. Recent measurements from Belle and LHCb are included in this analysis. While it is true that the new experimental results of $R(D^{(*)})$ get closer to the standard model predictions, there are still rooms for new physics and unparticles are also one possibility. Our best-fit values are $R(D)=0.456$ and $R(D^*)=0.270$, which are still far from the standard model values by more than ($R(D)$) or almost ($R(D^*)$) $2\\sigma$. We also find that the unparticle effects "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.02908","kind":"arxiv","version":2},"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":"2026-05-18T00:04:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+JT4JinElR2FHMAjKw1mqZxd8ZJO1Ygf6i8FpFo6sMRgHd4Os1tywA0HFdoWkiQ53wMDIrHrOgDScFOPIzqkCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T05:47:02.027500Z"},"content_sha256":"f6acb2a1b552c959a32adca9034527355b55016534f5b7b4bf2c8ffd38ec0978","schema_version":"1.0","event_id":"sha256:f6acb2a1b552c959a32adca9034527355b55016534f5b7b4bf2c8ffd38ec0978"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/bundle.json","state_url":"https://pith.science/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/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":"2026-06-09T05:47:02Z","links":{"resolver":"https://pith.science/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7","bundle":"https://pith.science/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/bundle.json","state":"https://pith.science/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HKVXDNOEUFG44SHJEVIZIKHZJ7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:HKVXDNOEUFG44SHJEVIZIKHZJ7","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":"05434885c09dee375b77953fdf541410db66bbee940cfd8dd756c38bc5f7ba62","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T11:37:56Z","title_canon_sha256":"9dc78a09f189ae89a242210c0c060d77c53075adedd5370284e200841f7cd18d"},"schema_version":"1.0","source":{"id":"1711.02908","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.02908","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"arxiv_version","alias_value":"1711.02908v2","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.02908","created_at":"2026-05-18T00:04:05Z"},{"alias_kind":"pith_short_12","alias_value":"HKVXDNOEUFG4","created_at":"2026-05-18T12:31:18Z"},{"alias_kind":"pith_short_16","alias_value":"HKVXDNOEUFG44SHJ","created_at":"2026-05-18T12:31:18Z"},{"alias_kind":"pith_short_8","alias_value":"HKVXDNOE","created_at":"2026-05-18T12:31:18Z"}],"graph_snapshots":[{"event_id":"sha256:f6acb2a1b552c959a32adca9034527355b55016534f5b7b4bf2c8ffd38ec0978","target":"graph","created_at":"2026-05-18T00:04:05Z","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":"We examine the possible unparticle effects on $R(D^{(*)})$ associated with $B\\to D^{(*)}\\tau\\nu$ decays by minimum-$\\chi^2$ fitting. Recent measurements from Belle and LHCb are included in this analysis. While it is true that the new experimental results of $R(D^{(*)})$ get closer to the standard model predictions, there are still rooms for new physics and unparticles are also one possibility. Our best-fit values are $R(D)=0.456$ and $R(D^*)=0.270$, which are still far from the standard model values by more than ($R(D)$) or almost ($R(D^*)$) $2\\sigma$. We also find that the unparticle effects ","authors_text":"Jong-Phil Lee","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T11:37:56Z","title":"Unparticle effects on $B\\to D^{(*)}\\tau\\nu$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.02908","kind":"arxiv","version":2},"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:cbef81c95a144574bd83d97a1c5fe29f8066cffaa13028022bd92b186af24379","target":"record","created_at":"2026-05-18T00:04:05Z","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":"05434885c09dee375b77953fdf541410db66bbee940cfd8dd756c38bc5f7ba62","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-11-08T11:37:56Z","title_canon_sha256":"9dc78a09f189ae89a242210c0c060d77c53075adedd5370284e200841f7cd18d"},"schema_version":"1.0","source":{"id":"1711.02908","kind":"arxiv","version":2}},"canonical_sha256":"3aab71b5c4a14dce48e925519428f94ff877d297817434f555c063d09e9e952d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3aab71b5c4a14dce48e925519428f94ff877d297817434f555c063d09e9e952d","first_computed_at":"2026-05-18T00:04:05.035077Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:05.035077Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nNdRM/WfgU3OyIhdP82t0FiLhw5mpIqa7x78dMACapOBOOPYMjHvwL80kMEeHRz8VyDiEHC/RymeDFs5cH5lDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:05.035763Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.02908","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cbef81c95a144574bd83d97a1c5fe29f8066cffaa13028022bd92b186af24379","sha256:f6acb2a1b552c959a32adca9034527355b55016534f5b7b4bf2c8ffd38ec0978"],"state_sha256":"2700338f19f4df027daf26c03290550ca7ca97392b4efd2dba414578cd2644ca"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ip8Xlw2q46UiIkvL7GC5L6aDoGiIkhIk/svPLl6dcr2DX5oHVCuTJyHw927wfQmMG4R0+pXkGKIFk92co9xlDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T05:47:02.031877Z","bundle_sha256":"4c357206b1b26d550a4f61b384729ed09074c2fc7e86e489402fec9b8af09acc"}}