{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:HKR465IGXKXGF4LLBRJAKHFZDU","short_pith_number":"pith:HKR465IG","schema_version":"1.0","canonical_sha256":"3aa3cf7506baae62f16b0c52051cb91d0a1f724d6581c6962a4eea32d0f48e98","source":{"kind":"arxiv","id":"0712.4053","version":2},"attestation_state":"computed","paper":{"title":"Unitarity bounds in the Higgs model including triplet fields with custodial symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"ICRR), Mayumi Aoki (Tokyo U., Shinya Kanemura (Toyama U.)","submitted_at":"2007-12-25T08:51:00Z","abstract_excerpt":"We study bounds on Higgs boson masses from perturbative unitarity in the Georgi-Machacek model, whose Higgs sector is composed of a scalar isospin doublet, a real and a complex isospin triplet fields. This model can be compatible with the electroweak precision data without fine tuning because of the imposed global SU(2)_R symmetry in the Higgs potential, by which the electroweak rho parameter is unity at the tree level. All possible two-body elastic-scattering channels are taken into account to evaluate the S-wave amplitude matrix, and then the condition of perturbative unitarity is imposed on"},"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":"0712.4053","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-12-25T08:51:00Z","cross_cats_sorted":[],"title_canon_sha256":"28b1a8dd1981bc37600b568074c819dac0c8110871c719dbd2ffb657ca7cfbe7","abstract_canon_sha256":"9ed8f8a04cf98ab061e4016827f008f858e8cb75f6eb44a5c53bb9cdd3af9660"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:28:05.839990Z","signature_b64":"SxBKqqwPeDOjjh76KBnl8L4kYI/UOtz1c1g7eyuc7pSTUjuoNQRMaOKAu/PgFAp+oeeptLZotZQsmqaizZQ9Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3aa3cf7506baae62f16b0c52051cb91d0a1f724d6581c6962a4eea32d0f48e98","last_reissued_at":"2026-07-04T15:28:05.839585Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:28:05.839585Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unitarity bounds in the Higgs model including triplet fields with custodial symmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"ICRR), Mayumi Aoki (Tokyo U., Shinya Kanemura (Toyama U.)","submitted_at":"2007-12-25T08:51:00Z","abstract_excerpt":"We study bounds on Higgs boson masses from perturbative unitarity in the Georgi-Machacek model, whose Higgs sector is composed of a scalar isospin doublet, a real and a complex isospin triplet fields. This model can be compatible with the electroweak precision data without fine tuning because of the imposed global SU(2)_R symmetry in the Higgs potential, by which the electroweak rho parameter is unity at the tree level. All possible two-body elastic-scattering channels are taken into account to evaluate the S-wave amplitude matrix, and then the condition of perturbative unitarity is imposed on"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0712.4053","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/0712.4053/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":"0712.4053","created_at":"2026-07-04T15:28:05.839642+00:00"},{"alias_kind":"arxiv_version","alias_value":"0712.4053v2","created_at":"2026-07-04T15:28:05.839642+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0712.4053","created_at":"2026-07-04T15:28:05.839642+00:00"},{"alias_kind":"pith_short_12","alias_value":"HKR465IGXKXG","created_at":"2026-07-04T15:28:05.839642+00:00"},{"alias_kind":"pith_short_16","alias_value":"HKR465IGXKXGF4LL","created_at":"2026-07-04T15:28:05.839642+00:00"},{"alias_kind":"pith_short_8","alias_value":"HKR465IG","created_at":"2026-07-04T15:28:05.839642+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.15983","citing_title":"Radiative corrections to decays of the 125 GeV Higgs boson in the complex Higgs triplet model","ref_index":91,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU","json":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU.json","graph_json":"https://pith.science/api/pith-number/HKR465IGXKXGF4LLBRJAKHFZDU/graph.json","events_json":"https://pith.science/api/pith-number/HKR465IGXKXGF4LLBRJAKHFZDU/events.json","paper":"https://pith.science/paper/HKR465IG"},"agent_actions":{"view_html":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU","download_json":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU.json","view_paper":"https://pith.science/paper/HKR465IG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0712.4053&json=true","fetch_graph":"https://pith.science/api/pith-number/HKR465IGXKXGF4LLBRJAKHFZDU/graph.json","fetch_events":"https://pith.science/api/pith-number/HKR465IGXKXGF4LLBRJAKHFZDU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU/action/storage_attestation","attest_author":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU/action/author_attestation","sign_citation":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU/action/citation_signature","submit_replication":"https://pith.science/pith/HKR465IGXKXGF4LLBRJAKHFZDU/action/replication_record"}},"created_at":"2026-07-04T15:28:05.839642+00:00","updated_at":"2026-07-04T15:28:05.839642+00:00"}