{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:F7HE5NBTO5ZTNLNFNTUNKLPOU5","short_pith_number":"pith:F7HE5NBT","schema_version":"1.0","canonical_sha256":"2fce4eb433777336ada56ce8d52deea7445c1cb9644da93c5357bab3b6a8d1d4","source":{"kind":"arxiv","id":"1504.08236","version":1},"attestation_state":"computed","paper":{"title":"Higgs boson production and decay at $e^{+}e^{-}$ colliders as a probe of the Left-Right twin Higgs model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bingfang Yang, Jinzhong Han, Ning Liu, Shaofeng Li","submitted_at":"2015-04-30T14:05:11Z","abstract_excerpt":"In the framework of the Left-Right twin Higgs (LRTH) model, we consider the constrains from the latest search for high-mass dilepton resonances at the LHC and find that the heavy neutral boson $Z_H$ is excluded with mass below 2.76 TeV. Under these constrains, we study the Higgs-Gauge coupling production processes $e^{+}e^{-}\\rightarrow ZH$, $e^{+}e^{-}\\rightarrow \\nu_{e}\\bar{\\nu_{e}}H$ and $e^{+}e^{-}\\rightarrow e^{+}e^{-}H$, top quark Yukawa coupling production process $e^{+}e^{-}\\rightarrow t\\bar{t}H$, Higgs self-couplings production processes $e^{+}e^{-}\\rightarrow ZHH$ and $e^{+}e^{-}\\rig"},"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":"1504.08236","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-04-30T14:05:11Z","cross_cats_sorted":[],"title_canon_sha256":"a293ffd673bfaab544b88985767de94db49d98e6008e729d13700773ae84d159","abstract_canon_sha256":"ea2df9edbefc141396cf2852d2504a604b92296a0d2829f7db8cfeb239f99624"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:05.413348Z","signature_b64":"Xe3Skn5Aoj/KP/Iq7YuIcTmvxUUuTqbZqYfHzHGJ/hbjimix6zrlN4LRuMCEpEagub1vwfUohephnlgVoBmfAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2fce4eb433777336ada56ce8d52deea7445c1cb9644da93c5357bab3b6a8d1d4","last_reissued_at":"2026-05-18T02:04:05.412641Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:05.412641Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson production and decay at $e^{+}e^{-}$ colliders as a probe of the Left-Right twin Higgs model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Bingfang Yang, Jinzhong Han, Ning Liu, Shaofeng Li","submitted_at":"2015-04-30T14:05:11Z","abstract_excerpt":"In the framework of the Left-Right twin Higgs (LRTH) model, we consider the constrains from the latest search for high-mass dilepton resonances at the LHC and find that the heavy neutral boson $Z_H$ is excluded with mass below 2.76 TeV. Under these constrains, we study the Higgs-Gauge coupling production processes $e^{+}e^{-}\\rightarrow ZH$, $e^{+}e^{-}\\rightarrow \\nu_{e}\\bar{\\nu_{e}}H$ and $e^{+}e^{-}\\rightarrow e^{+}e^{-}H$, top quark Yukawa coupling production process $e^{+}e^{-}\\rightarrow t\\bar{t}H$, Higgs self-couplings production processes $e^{+}e^{-}\\rightarrow ZHH$ and $e^{+}e^{-}\\rig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.08236","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":"1504.08236","created_at":"2026-05-18T02:04:05.412773+00:00"},{"alias_kind":"arxiv_version","alias_value":"1504.08236v1","created_at":"2026-05-18T02:04:05.412773+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.08236","created_at":"2026-05-18T02:04:05.412773+00:00"},{"alias_kind":"pith_short_12","alias_value":"F7HE5NBTO5ZT","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"F7HE5NBTO5ZTNLNF","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"F7HE5NBT","created_at":"2026-05-18T12:29:19.899920+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.24421","citing_title":"Double SM-like Higgs Production at future $ e^+ e^- $ colliders in the 3-Higgs Doublet Model under the $ S_{3} $ symmetry","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5","json":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5.json","graph_json":"https://pith.science/api/pith-number/F7HE5NBTO5ZTNLNFNTUNKLPOU5/graph.json","events_json":"https://pith.science/api/pith-number/F7HE5NBTO5ZTNLNFNTUNKLPOU5/events.json","paper":"https://pith.science/paper/F7HE5NBT"},"agent_actions":{"view_html":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5","download_json":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5.json","view_paper":"https://pith.science/paper/F7HE5NBT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1504.08236&json=true","fetch_graph":"https://pith.science/api/pith-number/F7HE5NBTO5ZTNLNFNTUNKLPOU5/graph.json","fetch_events":"https://pith.science/api/pith-number/F7HE5NBTO5ZTNLNFNTUNKLPOU5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5/action/storage_attestation","attest_author":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5/action/author_attestation","sign_citation":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5/action/citation_signature","submit_replication":"https://pith.science/pith/F7HE5NBTO5ZTNLNFNTUNKLPOU5/action/replication_record"}},"created_at":"2026-05-18T02:04:05.412773+00:00","updated_at":"2026-05-18T02:04:05.412773+00:00"}