{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RSEGWRQXWREQP3RZBHH6XLCL4G","short_pith_number":"pith:RSEGWRQX","schema_version":"1.0","canonical_sha256":"8c886b4617b44907ee3909cfebac4be1bdc885745a2a93eae4e1825640e25b7a","source":{"kind":"arxiv","id":"1704.04407","version":2},"attestation_state":"computed","paper":{"title":"$L_\\mu -L_\\tau$ gauge-boson production from lepton flavor violating $\\tau$ decays at Belle II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chuan-Hung Chen, Takaaki Nomura","submitted_at":"2017-04-14T12:26:38Z","abstract_excerpt":"$L_\\mu -L_\\tau$ gauge boson ($Z'$) with a mass in the MeV to GeV region can resolve not only the muon $g-2$ excess, but also the gap in the high-energy cosmic neutrino spectrum at IceCube. It was recently proposed that such a light gauge boson can be detected during the Belle II experiment with a luminosity of 50 ab$^{-1}$ by the $e^+ e^- \\to \\gamma +\\slashed{E}$ process through the kinetic mixing with the photon, where the missing energy $\\slashed{E}$ is from the $Z' \\to \\bar\\nu \\nu$ decays. We study the phenomenological implications when a pair of singlet vector-like leptons carrying differe"},"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":"1704.04407","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-04-14T12:26:38Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"0e9003f4aa1c3373a548e45dabf02b91adfac3e96d84cdba40de304fe959f16b","abstract_canon_sha256":"3442c4fb420cf65bdf9ee3a5ae2139c84d19b673764854bb42160ac0e82c5fd7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:30.759158Z","signature_b64":"wnqIAsNBV2ypJLQNI1a6l0je2JlfON5HVKoA2jMrAlREudgIlhDYM2vYxiw7sxMMjeWQecaxbjvr/8FoajxODg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c886b4617b44907ee3909cfebac4be1bdc885745a2a93eae4e1825640e25b7a","last_reissued_at":"2026-05-18T00:29:30.758513Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:30.758513Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$L_\\mu -L_\\tau$ gauge-boson production from lepton flavor violating $\\tau$ decays at Belle II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chuan-Hung Chen, Takaaki Nomura","submitted_at":"2017-04-14T12:26:38Z","abstract_excerpt":"$L_\\mu -L_\\tau$ gauge boson ($Z'$) with a mass in the MeV to GeV region can resolve not only the muon $g-2$ excess, but also the gap in the high-energy cosmic neutrino spectrum at IceCube. It was recently proposed that such a light gauge boson can be detected during the Belle II experiment with a luminosity of 50 ab$^{-1}$ by the $e^+ e^- \\to \\gamma +\\slashed{E}$ process through the kinetic mixing with the photon, where the missing energy $\\slashed{E}$ is from the $Z' \\to \\bar\\nu \\nu$ decays. We study the phenomenological implications when a pair of singlet vector-like leptons carrying differe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.04407","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1704.04407","created_at":"2026-05-18T00:29:30.758596+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.04407v2","created_at":"2026-05-18T00:29:30.758596+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.04407","created_at":"2026-05-18T00:29:30.758596+00:00"},{"alias_kind":"pith_short_12","alias_value":"RSEGWRQXWREQ","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RSEGWRQXWREQP3RZ","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RSEGWRQX","created_at":"2026-05-18T12:31:39.905425+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.07192","citing_title":"Gauged $U(1)_{L_\\mu-L_\\tau}$ Scotogenic Model in light of $R_{K^{(*)}}$ Anomaly and AMS-02 Positron Excess","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G","json":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G.json","graph_json":"https://pith.science/api/pith-number/RSEGWRQXWREQP3RZBHH6XLCL4G/graph.json","events_json":"https://pith.science/api/pith-number/RSEGWRQXWREQP3RZBHH6XLCL4G/events.json","paper":"https://pith.science/paper/RSEGWRQX"},"agent_actions":{"view_html":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G","download_json":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G.json","view_paper":"https://pith.science/paper/RSEGWRQX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.04407&json=true","fetch_graph":"https://pith.science/api/pith-number/RSEGWRQXWREQP3RZBHH6XLCL4G/graph.json","fetch_events":"https://pith.science/api/pith-number/RSEGWRQXWREQP3RZBHH6XLCL4G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G/action/storage_attestation","attest_author":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G/action/author_attestation","sign_citation":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G/action/citation_signature","submit_replication":"https://pith.science/pith/RSEGWRQXWREQP3RZBHH6XLCL4G/action/replication_record"}},"created_at":"2026-05-18T00:29:30.758596+00:00","updated_at":"2026-05-18T00:29:30.758596+00:00"}