{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MS6PXTGVCSNLSXPWK7UK5SHHYC","short_pith_number":"pith:MS6PXTGV","schema_version":"1.0","canonical_sha256":"64bcfbccd5149ab95df657e8aec8e7c08a93289c4c8872f9bd84461a6dbc360f","source":{"kind":"arxiv","id":"2309.03727","version":2},"attestation_state":"computed","paper":{"title":"The decay $B\\to K+\\nu+\\bar{\\nu}$ at Belle II and a massless bino in R-parity-violating supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Herbert K. Dreiner, Julian Y. G\\\"unther, Zeren Simon Wang","submitted_at":"2023-09-07T14:13:14Z","abstract_excerpt":"Recently, \\texttt{Belle II} announced evidence for the decay $B^+\\to K^+ +\\nu +\\bar{\\nu}$ at the $3.5\\,\\sigma$ significance, and measured the corresponding decay branching ratio to be $2.7\\,\\sigma$ above the Standard Model prediction. Here, we provide a theoretical explanation based on a massless bino in R-parity-violating (RPV) supersymmetry. With a single non-vanishing RPV coupling $\\lambda'_{i23/i32}$, $\\lambda'_{i13/i33}$, or $\\lambda'_{i12/i22}$, where $i=1,2,3$, the decay $B^+\\to K^+ +\\overset{\\scriptscriptstyle(-)}{\\nu_i}+ \\tilde{\\chi}^0_1$ can be induced, which would lead to the same s"},"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":"2309.03727","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-09-07T14:13:14Z","cross_cats_sorted":[],"title_canon_sha256":"48f354c8cb1a8c13bdb8f2d3eccbed8ee912581dede3f6fa28a685ce995bdcdb","abstract_canon_sha256":"3a994db2476b68007e35ec881b529b0a29553dd548b98f63f52913a366aba242"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:05:07.287021Z","signature_b64":"c+h85jWAHxRoO9sZOhYrb5TZ2vo4j2/PkfJMjVZ/Xi6x6K8Z2Un7gYnQGiLm2MAipuq694AaS0v66hBM9G/vCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"64bcfbccd5149ab95df657e8aec8e7c08a93289c4c8872f9bd84461a6dbc360f","last_reissued_at":"2026-07-05T10:05:07.286584Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:05:07.286584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The decay $B\\to K+\\nu+\\bar{\\nu}$ at Belle II and a massless bino in R-parity-violating supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Herbert K. Dreiner, Julian Y. G\\\"unther, Zeren Simon Wang","submitted_at":"2023-09-07T14:13:14Z","abstract_excerpt":"Recently, \\texttt{Belle II} announced evidence for the decay $B^+\\to K^+ +\\nu +\\bar{\\nu}$ at the $3.5\\,\\sigma$ significance, and measured the corresponding decay branching ratio to be $2.7\\,\\sigma$ above the Standard Model prediction. Here, we provide a theoretical explanation based on a massless bino in R-parity-violating (RPV) supersymmetry. With a single non-vanishing RPV coupling $\\lambda'_{i23/i32}$, $\\lambda'_{i13/i33}$, or $\\lambda'_{i12/i22}$, where $i=1,2,3$, the decay $B^+\\to K^+ +\\overset{\\scriptscriptstyle(-)}{\\nu_i}+ \\tilde{\\chi}^0_1$ can be induced, which would lead to the same s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2309.03727","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2309.03727/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2309.03727","created_at":"2026-07-05T10:05:07.286644+00:00"},{"alias_kind":"arxiv_version","alias_value":"2309.03727v2","created_at":"2026-07-05T10:05:07.286644+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2309.03727","created_at":"2026-07-05T10:05:07.286644+00:00"},{"alias_kind":"pith_short_12","alias_value":"MS6PXTGVCSNL","created_at":"2026-07-05T10:05:07.286644+00:00"},{"alias_kind":"pith_short_16","alias_value":"MS6PXTGVCSNLSXPW","created_at":"2026-07-05T10:05:07.286644+00:00"},{"alias_kind":"pith_short_8","alias_value":"MS6PXTGV","created_at":"2026-07-05T10:05:07.286644+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.21642","citing_title":"Probing Light Dark Fermions in $B \\to D^{(*)}\\ell X_{\\rm inv}$ via Rate Distributions","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2606.08273","citing_title":"Probing Signatures of Right-Handed Neutrinos via $b \\to s \\nu \\bar\\nu$ Decays","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21065","citing_title":"The Single Photon Signature of a Light Long-lived Neutralino at Remote Detectors at the LHC","ref_index":66,"is_internal_anchor":false},{"citing_arxiv_id":"2507.10801","citing_title":"Probing vector- vs scalar-mediator dark-matter scenarios in $B\\to (K,K^*) M_X$ decays","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2509.20027","citing_title":"Belle II Constraints on the Non-Minimal Universal Extra Dimensional Model","ref_index":8,"is_internal_anchor":false},{"citing_arxiv_id":"2601.08907","citing_title":"Dark Matter emission at Belle II and NA62 in Minimal Flavor Violation framework","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC","json":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC.json","graph_json":"https://pith.science/api/pith-number/MS6PXTGVCSNLSXPWK7UK5SHHYC/graph.json","events_json":"https://pith.science/api/pith-number/MS6PXTGVCSNLSXPWK7UK5SHHYC/events.json","paper":"https://pith.science/paper/MS6PXTGV"},"agent_actions":{"view_html":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC","download_json":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC.json","view_paper":"https://pith.science/paper/MS6PXTGV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2309.03727&json=true","fetch_graph":"https://pith.science/api/pith-number/MS6PXTGVCSNLSXPWK7UK5SHHYC/graph.json","fetch_events":"https://pith.science/api/pith-number/MS6PXTGVCSNLSXPWK7UK5SHHYC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC/action/storage_attestation","attest_author":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC/action/author_attestation","sign_citation":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC/action/citation_signature","submit_replication":"https://pith.science/pith/MS6PXTGVCSNLSXPWK7UK5SHHYC/action/replication_record"}},"created_at":"2026-07-05T10:05:07.286644+00:00","updated_at":"2026-07-05T10:05:07.286644+00:00"}