{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:OWZ22FXGAO6XT5OCQRVLOJN6FJ","short_pith_number":"pith:OWZ22FXG","schema_version":"1.0","canonical_sha256":"75b3ad16e603bd79f5c2846ab725be2a6dbb13237fffd3c5718c0720be2ac6fc","source":{"kind":"arxiv","id":"1801.08259","version":3},"attestation_state":"computed","paper":{"title":"New physics in inclusive $B \\to X_c\\ell \\bar{\\nu}$ decay in light of $R(D^{(*)})$ measurements","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmed Rashed, Alakabha Datta, Saeed Kamali","submitted_at":"2018-01-25T02:49:00Z","abstract_excerpt":"In this work we study the effects of new-physics (NP) operators with different Lorentz structures on the inclusive $B \\to X_c\\tau \\bar{\\nu}$ decay and make predictions for the ratio of total decay rates $R(X_c)=\\frac{\\Gamma(B \\to X_c\\tau \\bar{\\nu}_\\tau)}{\\Gamma(B \\to X_c \\ell \\bar{\\nu}_\\ell)}$ with $\\ell=e, \\mu$, the differential decay rates, $\\frac{d\\Gamma}{dq^2}$ and $\\frac{d\\Gamma}{dE_\\tau}$, forward-backward asymmetry $A_{FB}$ and the ratio of the differential decay rates $B(q^2)=\\frac{d\\Gamma(B \\to X_c\\tau \\bar{\\nu}_\\tau)/dq^2}{d\\Gamma(B \\to X_c \\ell \\bar{\\nu}_\\ell)/dq^2}$. In addition, w"},"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":"1801.08259","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-01-25T02:49:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e9d9493caad10448fc1296b84593ea3fa07dda29d25d174f2e149052dd423f32","abstract_canon_sha256":"1726ba4bdd5421b0a4bf61dd24d03934c13b1bff0fa00b79fc1ff646cdd95246"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:40.452337Z","signature_b64":"jM1ueMzn6aSS+K4dnWea48evMdNJhHsXrfyIZM+CIsP3N4zvAObhQbXVSmT128M4WWsL9GAvl/7YqGQw7yY9Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75b3ad16e603bd79f5c2846ab725be2a6dbb13237fffd3c5718c0720be2ac6fc","last_reissued_at":"2026-05-18T00:14:40.451667Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:40.451667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New physics in inclusive $B \\to X_c\\ell \\bar{\\nu}$ decay in light of $R(D^{(*)})$ measurements","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ahmed Rashed, Alakabha Datta, Saeed Kamali","submitted_at":"2018-01-25T02:49:00Z","abstract_excerpt":"In this work we study the effects of new-physics (NP) operators with different Lorentz structures on the inclusive $B \\to X_c\\tau \\bar{\\nu}$ decay and make predictions for the ratio of total decay rates $R(X_c)=\\frac{\\Gamma(B \\to X_c\\tau \\bar{\\nu}_\\tau)}{\\Gamma(B \\to X_c \\ell \\bar{\\nu}_\\ell)}$ with $\\ell=e, \\mu$, the differential decay rates, $\\frac{d\\Gamma}{dq^2}$ and $\\frac{d\\Gamma}{dE_\\tau}$, forward-backward asymmetry $A_{FB}$ and the ratio of the differential decay rates $B(q^2)=\\frac{d\\Gamma(B \\to X_c\\tau \\bar{\\nu}_\\tau)/dq^2}{d\\Gamma(B \\to X_c \\ell \\bar{\\nu}_\\ell)/dq^2}$. In addition, w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08259","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":"1801.08259","created_at":"2026-05-18T00:14:40.451764+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.08259v3","created_at":"2026-05-18T00:14:40.451764+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08259","created_at":"2026-05-18T00:14:40.451764+00:00"},{"alias_kind":"pith_short_12","alias_value":"OWZ22FXGAO6X","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_16","alias_value":"OWZ22FXGAO6XT5OC","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_8","alias_value":"OWZ22FXG","created_at":"2026-05-18T12:32:43.782077+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.12065","citing_title":"A Phenomenological Study of Semileptonic $B^+$ and $B_s^0$ Decays into Axial-Vector Mesons $\\big(D_1(2420),\\, D_1^\\prime(2430),\\, D_{s1}(2460),\\, \\text{and } D_{s1}^\\prime(2536)\\big)$ within the Stand","ref_index":64,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ","json":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ.json","graph_json":"https://pith.science/api/pith-number/OWZ22FXGAO6XT5OCQRVLOJN6FJ/graph.json","events_json":"https://pith.science/api/pith-number/OWZ22FXGAO6XT5OCQRVLOJN6FJ/events.json","paper":"https://pith.science/paper/OWZ22FXG"},"agent_actions":{"view_html":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ","download_json":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ.json","view_paper":"https://pith.science/paper/OWZ22FXG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.08259&json=true","fetch_graph":"https://pith.science/api/pith-number/OWZ22FXGAO6XT5OCQRVLOJN6FJ/graph.json","fetch_events":"https://pith.science/api/pith-number/OWZ22FXGAO6XT5OCQRVLOJN6FJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ/action/storage_attestation","attest_author":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ/action/author_attestation","sign_citation":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ/action/citation_signature","submit_replication":"https://pith.science/pith/OWZ22FXGAO6XT5OCQRVLOJN6FJ/action/replication_record"}},"created_at":"2026-05-18T00:14:40.451764+00:00","updated_at":"2026-05-18T00:14:40.451764+00:00"}