{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:72JCUKCJSKAGTNIK4LLTAVGNCP","short_pith_number":"pith:72JCUKCJ","schema_version":"1.0","canonical_sha256":"fe922a2849928069b50ae2d73054cd13dcd9397ef29cc452548cb3abaa00c989","source":{"kind":"arxiv","id":"1805.05048","version":1},"attestation_state":"computed","paper":{"title":"Higgs boson decay $h^0\\rightarrow m_VZ$ in the BLMSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo-Zhu Ning, Hai-Bin Zhang, Jian-Bin Chen, Jing-Jing Feng, Shu-Min Zhao, Tai-Fu Feng","submitted_at":"2018-05-14T08:00:39Z","abstract_excerpt":"In the framework of BLMSSM, the Higgs decays $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$ are studied where $m_V$ represents a vector meson($\\rho, \\omega, \\phi, J/\\psi, \\Upsilon$ etc.). Corrections to the CP-even and CP-odd $h^0\\gamma Z$ couplings occur via loop diagrams where new particles are involved. Actually both of them obviously influence the decay rates of $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$. Concretely, our obtained numerical result shows that the decay width of $h^0\\rightarrow Z\\gamma$ can be 1.3 times larger than the prediction of the Standard Model(SM). For the"},"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":"1805.05048","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-14T08:00:39Z","cross_cats_sorted":[],"title_canon_sha256":"d15807f8ec486db01cd34c51a7d7499df566d7b3268074d9ec63e56660f8d731","abstract_canon_sha256":"18b36ccb05c830576a3572e4ca8e2283350decbe6ee0c2b2328231dc963d3d80"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:03.971078Z","signature_b64":"bSXKKLZnw9mfjJPwv9H/BkpamaMRX1MDGu+dixuJhKyvJuBVRhRT8mJSVthpZcueBtXtIfWO5a/yCeXIxCbUDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe922a2849928069b50ae2d73054cd13dcd9397ef29cc452548cb3abaa00c989","last_reissued_at":"2026-05-18T00:16:03.970727Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:03.970727Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson decay $h^0\\rightarrow m_VZ$ in the BLMSSM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guo-Zhu Ning, Hai-Bin Zhang, Jian-Bin Chen, Jing-Jing Feng, Shu-Min Zhao, Tai-Fu Feng","submitted_at":"2018-05-14T08:00:39Z","abstract_excerpt":"In the framework of BLMSSM, the Higgs decays $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$ are studied where $m_V$ represents a vector meson($\\rho, \\omega, \\phi, J/\\psi, \\Upsilon$ etc.). Corrections to the CP-even and CP-odd $h^0\\gamma Z$ couplings occur via loop diagrams where new particles are involved. Actually both of them obviously influence the decay rates of $h^0\\rightarrow Z\\gamma$ and $h^0\\rightarrow m_VZ$. Concretely, our obtained numerical result shows that the decay width of $h^0\\rightarrow Z\\gamma$ can be 1.3 times larger than the prediction of the Standard Model(SM). For the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05048","kind":"arxiv","version":1},"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":"1805.05048","created_at":"2026-05-18T00:16:03.970783+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.05048v1","created_at":"2026-05-18T00:16:03.970783+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.05048","created_at":"2026-05-18T00:16:03.970783+00:00"},{"alias_kind":"pith_short_12","alias_value":"72JCUKCJSKAG","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_16","alias_value":"72JCUKCJSKAGTNIK","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_8","alias_value":"72JCUKCJ","created_at":"2026-05-18T12:32:11.075285+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP","json":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP.json","graph_json":"https://pith.science/api/pith-number/72JCUKCJSKAGTNIK4LLTAVGNCP/graph.json","events_json":"https://pith.science/api/pith-number/72JCUKCJSKAGTNIK4LLTAVGNCP/events.json","paper":"https://pith.science/paper/72JCUKCJ"},"agent_actions":{"view_html":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP","download_json":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP.json","view_paper":"https://pith.science/paper/72JCUKCJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.05048&json=true","fetch_graph":"https://pith.science/api/pith-number/72JCUKCJSKAGTNIK4LLTAVGNCP/graph.json","fetch_events":"https://pith.science/api/pith-number/72JCUKCJSKAGTNIK4LLTAVGNCP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP/action/storage_attestation","attest_author":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP/action/author_attestation","sign_citation":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP/action/citation_signature","submit_replication":"https://pith.science/pith/72JCUKCJSKAGTNIK4LLTAVGNCP/action/replication_record"}},"created_at":"2026-05-18T00:16:03.970783+00:00","updated_at":"2026-05-18T00:16:03.970783+00:00"}