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For the total branching ratio, we predict $\\mathcal{BR}(\\process)_{\\rm hLFQCD}=(6.36^{+0.59}_{-0.74})\\times 10^{-6}$ and $\\mathcal{BR}(\\process)_{\\rm SR}=(8.14^{+0.16}_{- 0.17})\\times 10^{-6}$. More interestingly, we find that the two model predictions for the differential branching ratio are sufficiently different at low momentum transfer, so that"},"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":"1805.02940","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-08T10:44:29Z","cross_cats_sorted":[],"title_canon_sha256":"37faf4e9ad42ccc935768067125f0ecf3190c0aa0d26064958e5c79e5712795f","abstract_canon_sha256":"86dd77f3941d9e64eb7af4c6614dca30e4ddd92a8d4f3ffd07056c2d26a87cf4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:31.248517Z","signature_b64":"h+IkiUF3qdtgfpMumatx0HbVkOBtkIWFEe+tJzkoQuUnmP6Fny5g2mC883oDjRN7MXsRNT/h9lQDoobT25NCBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c36f01ad765ee7daa4d2787099e35cd1bfe9baed0fad6f611ac29db15350495d","last_reissued_at":"2026-05-18T00:05:31.248017Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:31.248017Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing transition form factors in the rare $B\\to K^*\\nu\\bar\\nu$ decay","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander Morrison, Alexandre Leger, Mohammad Ahmady, Ruben Sandapen, Zoe McIntyre","submitted_at":"2018-05-08T10:44:29Z","abstract_excerpt":"We compare the Standard Model (SM) predictions for the differential branching ratio of the rare $B\\to K^*\\nu\\bar\\nu$ decays using $B \\to K^*$ form factors obtained from holographic light-front QCD (hLFQCD) and Sum Rules (SR) Distribution Amplitudes. For the total branching ratio, we predict $\\mathcal{BR}(\\process)_{\\rm hLFQCD}=(6.36^{+0.59}_{-0.74})\\times 10^{-6}$ and $\\mathcal{BR}(\\process)_{\\rm SR}=(8.14^{+0.16}_{- 0.17})\\times 10^{-6}$. 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