{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:YYU2BGNPGWOUHULWROMEMPHG6O","short_pith_number":"pith:YYU2BGNP","schema_version":"1.0","canonical_sha256":"c629a099af359d43d1768b98463ce6f3be7a4d9bef258ebc83095d0a152386a8","source":{"kind":"arxiv","id":"1708.06176","version":3},"attestation_state":"computed","paper":{"title":"$R(D^{(*)})$ in a general two Higgs doublet model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kazuhiro Tobe, Syuhei Iguro","submitted_at":"2017-08-21T12:16:50Z","abstract_excerpt":"Motivated by an anomaly in $R(D^{(*)})={\\rm BR}(\\bar{B}\\rightarrow D^{(*)} \\tau^-\\bar{\\nu})/{\\rm BR}(\\bar{B}\\rightarrow D^{(*)} l^-\\bar{\\nu})$ reported by BaBar, Belle and LHCb, we study $R(D^{(*)})$ in a general two Higgs doublet model (2HDM). Although it has been suggested that it is difficult for the 2HDM to explain the current world average for $R(D^{(*)})$, it would be important to clarify how large deviations from the standard model predictions for $R(D^{(*)})$ are possible in the 2HDM. We investigate possible corrections to $R(D^{(*)})$ in the 2HDM by taking into account various flavor "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1708.06176","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-08-21T12:16:50Z","cross_cats_sorted":[],"title_canon_sha256":"db4962e599914bded031de98fb5deb39e347552e04e6fdd98434f77c1b00bcc2","abstract_canon_sha256":"3d51e323f896dd150914f111b74e961acb15f9660bcd14aa106be9249c5d8c73"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:25.713469Z","signature_b64":"Y+pTCxvy5vS1svwpXgqPXJhnlWJo0uNvZnYTSAyXVCHJct5wRMP8o7H2rkTob7oggRfrO6L8WoP1HXxl6FCKBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c629a099af359d43d1768b98463ce6f3be7a4d9bef258ebc83095d0a152386a8","last_reissued_at":"2026-05-18T00:21:25.712912Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:25.712912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$R(D^{(*)})$ in a general two Higgs doublet model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kazuhiro Tobe, Syuhei Iguro","submitted_at":"2017-08-21T12:16:50Z","abstract_excerpt":"Motivated by an anomaly in $R(D^{(*)})={\\rm BR}(\\bar{B}\\rightarrow D^{(*)} \\tau^-\\bar{\\nu})/{\\rm BR}(\\bar{B}\\rightarrow D^{(*)} l^-\\bar{\\nu})$ reported by BaBar, Belle and LHCb, we study $R(D^{(*)})$ in a general two Higgs doublet model (2HDM). Although it has been suggested that it is difficult for the 2HDM to explain the current world average for $R(D^{(*)})$, it would be important to clarify how large deviations from the standard model predictions for $R(D^{(*)})$ are possible in the 2HDM. We investigate possible corrections to $R(D^{(*)})$ in the 2HDM by taking into account various flavor "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.06176","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1708.06176","created_at":"2026-05-18T00:21:25.713007+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.06176v3","created_at":"2026-05-18T00:21:25.713007+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.06176","created_at":"2026-05-18T00:21:25.713007+00:00"},{"alias_kind":"pith_short_12","alias_value":"YYU2BGNPGWOU","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"YYU2BGNPGWOUHULW","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"YYU2BGNP","created_at":"2026-05-18T12:31:59.375834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.09414","citing_title":"New physics searches via angular distributions of $ \\bar{B} \\to D^* (\\to D \\pi) \\tau (\\to \\ell \\nu_\\tau \\bar{\\nu}_\\ell) \\bar{\\nu}_\\tau$ decays","ref_index":7,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O","json":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O.json","graph_json":"https://pith.science/api/pith-number/YYU2BGNPGWOUHULWROMEMPHG6O/graph.json","events_json":"https://pith.science/api/pith-number/YYU2BGNPGWOUHULWROMEMPHG6O/events.json","paper":"https://pith.science/paper/YYU2BGNP"},"agent_actions":{"view_html":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O","download_json":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O.json","view_paper":"https://pith.science/paper/YYU2BGNP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.06176&json=true","fetch_graph":"https://pith.science/api/pith-number/YYU2BGNPGWOUHULWROMEMPHG6O/graph.json","fetch_events":"https://pith.science/api/pith-number/YYU2BGNPGWOUHULWROMEMPHG6O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O/action/storage_attestation","attest_author":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O/action/author_attestation","sign_citation":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O/action/citation_signature","submit_replication":"https://pith.science/pith/YYU2BGNPGWOUHULWROMEMPHG6O/action/replication_record"}},"created_at":"2026-05-18T00:21:25.713007+00:00","updated_at":"2026-05-18T00:21:25.713007+00:00"}